parameters.yaml

# Auto-generated by: abacus --generate-parameters-yaml
# Do not edit manually.
parameters:
  - name: suffix
    category: System variables
    type: String
    description: |
      In each run, ABACUS will generate a subdirectory in the working directory. This subdirectory contains all the information of the run. The subdirectory name has the format: OUT.suffix, where the suffix is the name you can pick up for your convenience.
    default_value: ABACUS
    unit: ""
    availability: ""
  - name: ntype
    category: System variables
    type: Integer
    description: |
      Number of different atom species in the calculation.
    default_value: "0"
    unit: ""
    availability: ""
  - name: calculation
    category: System variables
    type: String
    description: |
      Specify the type of calculation.

      * scf: perform self-consistent electronic structure calculations
      * nscf: perform non-self-consistent electronic structure calculations. A charge density file is required
      * relax: perform structure relaxation calculations, the relax_nmax parameter depicts the maximal number of ionic iterations
      * cell-relax: perform cell relaxation calculations
      * md: perform molecular dynamics simulations
      * get_pchg: obtain partial (band-decomposed) charge densities (for LCAO basis only). See out_pchg for more information
      * get_wf: obtain real space wave functions (for LCAO basis only). See out_wfc_norm and out_wfc_re_im for more information
      * get_s: obtain the overlap matrix formed by localized orbitals (for LCAO basis with multiple k points). The file name is OUT.${suffix}/sr_nao.csr, with the same file format as generated by out_hsr 1
      * gen_bessel: generates projectors, i.e., a series of Bessel functions, for the DeePKS method (for LCAO basis only)
      * gen_opt_abfs: generate opt-ABFs as discussed in this article
      * test_memory: obtain a rough estimation of memory consumption for the calculation
      * test_neighbour: obtain information of neighboring atoms (for LCAO basis only), please specify a positive search_radius manually
    default_value: scf
    unit: ""
    availability: ""
  - name: esolver_type
    category: System variables
    type: String
    description: |
      Choose the energy solver.
      * ksdft: Kohn-Sham density functional theory
      * ofdft: orbital-free density functional theory
      * tdofdft: time-dependent orbital-free density functional theory
      * sdft: stochastic density functional theory
      * tddft: real-time time-dependent density functional theory (RT-TDDFT)
      * lj: Leonard Jones potential
      * dp: DeeP potential
      * nep: Neuroevolution Potential
      * ks-lr: Kohn-Sham density functional theory + LR-TDDFT (Under Development Feature)
      * lr: LR-TDDFT with given KS orbitals (Under Development Feature)
    default_value: ksdft
    unit: ""
    availability: ""
  - name: symmetry
    category: System variables
    type: String
    description: |
      Takes value 1, 0 or -1.
      * -1: No symmetry will be considered. It is recommended to set -1 for non-colinear + soc calculations, where time reversal symmetry is broken sometimes.
      * 0: Only time reversal symmetry would be considered in symmetry operations, which implied k point and -k point would be treated as a single k point with twice the weight.
      * 1: Symmetry analysis will be performed to determine the type of Bravais lattice and associated symmetry operations (point groups, space groups, primitive cells, and irreducible k-points). For a magnetic system, the symmetry of the initial magnetic structure will be analyzed and preserved.

      [NOTE] When symmetry is enabled (value 1), k-points are reduced to the irreducible Brillouin zone (IBZ). For explicit k-point lists with custom weights (see KPT file), the custom weights are preserved during symmetry reduction. For Monkhorst-Pack grids, uniform weights are used.
    default_value: default
    unit: ""
    availability: ""
  - name: symmetry_prec
    category: System variables
    type: Real
    description: |
      The accuracy for symmetry analysis. Typically, the default value is good enough, but if the lattice parameters or atom positions in STRU file are not accurate enough, this value should be enlarged.
      [NOTE] Note: if calculation==cell_relax, this value can be dynamically changed corresponding to the variation of accuracy of the lattice parameters and atom positions during the relaxation.
    default_value: "1.0e-6"
    unit: Bohr
    availability: ""
  - name: symmetry_autoclose
    category: System variables
    type: Boolean
    description: |
      Control how to deal with error in symmetry analysis due to inaccurate lattice parameters or atom positions in STRU file, especially useful when calculation==cell-relax
      * False: quit with an error message
      * True: automatically set symmetry to 0 and continue running without symmetry analysis
    default_value: "True"
    unit: ""
    availability: symmetry==1
  - name: cal_force
    category: System variables
    type: Boolean
    description: |
      If set to True, calculate the force at the end of the electronic iteration.
    default_value: "False"
    unit: ""
    availability: ""
  - name: kpar
    category: System variables
    type: Integer
    description: |
      Divide all processors into kpar groups, and k points will be distributed among each group. The value taken should be less than or equal to the number of k points as well as the number of MPI processes.
    default_value: "1"
    unit: ""
    availability: ""
  - name: bndpar
    category: System variables
    type: Integer
    description: |
      Divide all processors into bndpar groups for SDFT or the BPCG solver. bndpar must be positive, no greater than the number of MPI processes, and kpar * bndpar must divide the number of MPI processes exactly.
    default_value: "1"
    unit: ""
    availability: ""
  - name: latname
    category: System variables
    type: String
    description: |
      Specifies the type of Bravias lattice. When set to none, the three lattice vectors are supplied explicitly in STRU file.

      Available options are:
      * none: free structure
      * sc: simple cubic
      * fcc: face-centered cubic
      * bcc: body-centered cubic
      * hexagonal: hexagonal
      * trigonal: trigonal
      * st: simple tetragonal
      * bct: body-centered tetragonal
      * so: orthorhombic
      * baco: base-centered orthorhombic
      * fco: face-centered orthorhombic
      * bco: body-centered orthorhombic
      * sm: simple monoclinic
      * bacm: base-centered monoclinic
      * triclinic: triclinic
    default_value: none
    unit: ""
    availability: ""
  - name: assume_isolated
    category: System variables
    type: String
    description: |
      Used to perform a calculation assuming an isolated system in a 3D supercell.

      Available options are:
      * none: regular periodic calculation without isolated-system correction.
      * makov-payne, m-p, mp: compute the Makov-Payne correction to the total energy and estimate a corrected vacuum level for eigenvalue alignment. This option is available only for cubic lattices (latname = sc, fcc, or bcc).

      Theory: G. Makov and M. C. Payne, Phys. Rev. B 51, 4014 (1995).
    default_value: none
    unit: ""
    availability: ""
  - name: init_wfc
    category: System variables
    type: String
    description: |
      The type of the starting wave functions.

      Available options are:
      * atomic: from atomic pseudo wave functions. If they are not enough, other wave functions are initialized with random numbers.
      * atomic+random: add small random numbers on atomic pseudo-wavefunctions
      * file: from binary files wf*.dat, which are output by setting out_wfc_pw to 2.
      * random: random numbers
      * nao: from numerical atomic orbitals. If they are not enough, other wave functions are initialized with random numbers.
      * nao+random: add small random numbers on numerical atomic orbitals

      [NOTE] Only the file option is useful for the lcao basis set, which is mostly used when calculation is set to get_wf and get_pchg.
    default_value: atomic
    unit: ""
    availability: ""
  - name: init_chg
    category: System variables
    type: String
    description: |
      This variable is used for both plane wave set and localized orbitals set. It indicates the type of starting density.

      * atomic: the density is starting from the summation of the atomic density of single atoms.
      * file: the density will be read in from a binary file charge-density.dat first. If it does not exist, the charge density will be read in from cube files.
      * wfc: the density will be calculated by wavefunctions and occupations.
      * dm: the density will be calculated by real space density matrix(DMR) of LCAO base.
      * dm_no_renormalize: same as dm, but the charge density is not renormalized to the number of electrons.
      * hr: the real space Hamiltonian matrix(HR) will be read in from file hrs1_nao.csr in directory read_file_dir.
      * auto: Abacus first attempts to read the density from a file; if not found, it defaults to using atomic density.
    default_value: atomic
    unit: ""
    availability: ""
  - name: init_vel
    category: System variables
    type: Boolean
    description: |
      * True: read the atom velocity (atomic unit : 1 a.u. = 21.877 Angstrom/fs) from the atom file (STRU) and determine the initial temperature md_tfirst. If md_tfirst is unset or less than zero, init_vel is autoset to be true.
      * False: assign value to atom velocity using Gaussian distributed random numbers.
    default_value: "False"
    unit: ""
    availability: ""
  - name: mem_saver
    category: System variables
    type: Integer
    description: |
      Save memory when performing nscf calculations.
      * 0: no memory saving techniques are used.
      * 1: a memory saving technique will be used for many k point calculations.
    default_value: "0"
    unit: ""
    availability: calculation==nscf and basis_type==pw
  - name: cal_stress
    category: System variables
    type: Boolean
    description: |
      If set to True, calculate the stress at the end of the electronic iteration.
    default_value: "False"
    unit: ""
    availability: ""
  - name: diago_proc
    category: System variables
    type: Integer
    description: |
      * 0: it will be set to the number of MPI processes.
      * >0: it specifies the number of processes used for carrying out diagonalization. Must be less than or equal to total number of MPI processes.
    default_value: "0"
    unit: ""
    availability: basis_type==pw
  - name: nbspline
    category: System variables
    type: Integer
    description: |
      If set to a natural number, a Cardinal B-spline interpolation will be used to calculate Structure Factor. nbspline represents the order of B-spline basis and a larger one can get more accurate results but cost more. It is turned off by default.
    default_value: "-1"
    unit: ""
    availability: ""
  - name: kspacing
    category: System variables
    type: Vector of Real (1 or 3 values)
    description: |
      Set the smallest allowed spacing between k points, unit in 1/bohr. It should be larger than 0.0, and suggest smaller than 0.25. When you have set this value > 0.0, then the KPT file is unnecessary. The default value 0.0 means that ABACUS will read the applied KPT file.

      [NOTE] If gamma_only is set to be true, kspacing is invalid.
    default_value: "0.0"
    unit: ""
    availability: ""
  - name: koffset
    category: System variables
    type: Vector of Real (3 values)
    description: |
      Set offsets for automatic k-point mesh generated by kspacing, in each reciprocal direction. This parameter is only effective when kspacing > 0.0 and gamma_only is false.
    default_value: 0.0 0.0 0.0
    unit: ""
    availability: ""
  - name: kmesh_type
    category: System variables
    type: String
    description: |
      Set mesh type used for automatic k-point mesh generated by kspacing. Available options are gamma and mp. This parameter is only effective when kspacing > 0.0 and gamma_only is false.
    default_value: gamma
    unit: ""
    availability: ""
  - name: min_dist_coef
    category: System variables
    type: Real
    description: |
      A factor related to the allowed minimum distance between two atoms. At the beginning, ABACUS will check the structure, and if the distance of two atoms is shorter than min_dist_coef*(standard covalent bond length), we think this structure is unreasonable.
    default_value: "0.2"
    unit: ""
    availability: ""
  - name: device
    category: System variables
    type: String
    description: |
      Specifies the computing device for ABACUS.

      Available options are:
      * cpu: for CPUs via Intel, AMD, or Other supported CPU devices
      * gpu: for GPUs via CUDA or ROCm.

      [NOTE] ks_solver must also be set to the algorithms supported. lcao_in_pw currently does not support gpu.
    default_value: cpu
    unit: ""
    availability: ""
  - name: precision
    category: System variables
    type: String
    description: |
      Specifies the precision when performing scf calculation.
      * single: single precision
      * double: double precision
    default_value: double
    unit: ""
    availability: basis_type==pw
  - name: gint_precision
    category: System variables
    type: String
    description: |
      Specifies the precision when performing grid integral in LCAO calculations.
      * single: single precision
      * double: double precision
      * mix: mixed precision, starting from single precision and switching to double precision when the SCF residual becomes small enough
    default_value: double
    unit: ""
    availability: basis_type==lcao
  - name: timer_enable_nvtx
    category: System variables
    type: Boolean
    description: |
      Controls whether NVTX profiling labels are emitted by the timer. This feature is only effective on CUDA platforms.

      * True: Enable NVTX profiling labels in the timer.
      * False: Disable NVTX profiling labels in the timer.
    default_value: "False"
    unit: ""
    availability: ""
  - name: cell_factor
    category: System variables
    type: Real
    description: |
      Used in the construction of the pseudopotential tables. For cell-relax calculations, this is automatically set to 2.0.
    default_value: "1.2"
    unit: ""
    availability: ""
  - name: dm_to_rho
    category: System variables
    type: Boolean
    description: |
      Reads density matrix in npz format and calculates electron density.
    default_value: "False"
    unit: ""
    availability: ""
  - name: chg_extrap
    category: System variables
    type: String
    description: |
      Charge extrapolation method for MD and relaxation calculations.
    default_value: default
    unit: ""
    availability: ""
  - name: ecutwfc
    category: Plane wave related variables
    type: Real
    description: |
      Energy cutoff for plane wave functions. Note that even for localized orbitals basis, you still need to setup an energy cutoff for this system. Because our local pseudopotential parts and the related force are calculated from plane wave basis set.
      [NOTE] ecutwfc and ecutrho can be set simultaneously. If only one parameter is set, abacus will automatically set another parameter based on the 4-time relationship.
    default_value: "50 for PW basis, 100 for LCAO basis"
    unit: Ry
    availability: ""
  - name: ecutrho
    category: Plane wave related variables
    type: Real
    description: |
      Energy cutoff for charge density and potential. For norm-conserving pseudopotential you should stick to the default value, you can reduce it by a little but it will introduce noise especially on forces and stress.
    default_value: "4*ecutwfc"
    unit: Ry
    availability: ""
  - name: nx
    category: Plane wave related variables
    type: Integer
    description: |
      If set to a positive number, specifies the number of FFT grid points in x direction. If set to 0, the number will be calculated from ecutrho.

      [NOTE] You must specify all three dimensions (nx, ny, nz) for this setting to be used.
    default_value: "0"
    unit: ""
    availability: ""
  - name: ny
    category: Plane wave related variables
    type: Integer
    description: |
      If set to a positive number, specifies the number of FFT grid points in y direction. If set to 0, the number will be calculated from ecutrho.

      [NOTE] You must specify all three dimensions (nx, ny, nz) for this setting to be used.
    default_value: "0"
    unit: ""
    availability: ""
  - name: nz
    category: Plane wave related variables
    type: Integer
    description: |
      If set to a positive number, specifies the number of FFT grid points in z direction. If set to 0, the number will be calculated from ecutrho.

      [NOTE] You must specify all three dimensions (nx, ny, nz) for this setting to be used.
    default_value: "0"
    unit: ""
    availability: ""
  - name: ndx
    category: Plane wave related variables
    type: Integer
    description: |
      If set to a positive number, specifies the number of FFT grid points for the dense part of charge density in x direction. If set to 0, the number will be calculated from ecutwfc.

      [NOTE] You must specify all three dimensions (ndx, ndy, ndz) for this setting to be used. These parameters must be used combined with nx, ny, nz. If nx, ny, nz are unset, ndx, ndy, ndz are used as nx, ny, nz.
    default_value: "0"
    unit: ""
    availability: ""
  - name: ndy
    category: Plane wave related variables
    type: Integer
    description: |
      If set to a positive number, specifies the number of FFT grid points for the dense part of charge density in y direction. If set to 0, the number will be calculated from ecutwfc.

      [NOTE] You must specify all three dimensions (ndx, ndy, ndz) for this setting to be used. These parameters must be used combined with nx, ny, nz. If nx, ny, nz are unset, ndx, ndy, ndz are used as nx, ny, nz.
    default_value: "0"
    unit: ""
    availability: ""
  - name: ndz
    category: Plane wave related variables
    type: Integer
    description: |
      If set to a positive number, specifies the number of FFT grid points for the dense part of charge density in z direction. If set to 0, the number will be calculated from ecutwfc.

      [NOTE] You must specify all three dimensions (ndx, ndy, ndz) for this setting to be used. These parameters must be used combined with nx, ny, nz. If nx, ny, nz are unset, ndx, ndy, ndz are used as nx, ny, nz.
    default_value: "0"
    unit: ""
    availability: ""
  - name: pw_seed
    category: Plane wave related variables
    type: Integer
    description: |
      Specify the random seed to initialize wave functions. Only positive integers are available.
    default_value: "0"
    unit: ""
    availability: basis_type==pw
  - name: diag_subspace
    category: Plane wave related variables
    type: Integer
    description: |
      The method to diagonalize subspace in dav_subspace method.
      * 0: by LAPACK
      * 1: by GenELPA
      * 2: by ScaLAPACK
    default_value: "0"
    unit: ""
    availability: basis_type==pw and ks_solver==dav_subspace
  - name: erf_ecut
    category: Plane wave related variables
    type: Real
    description: |
      Used in variable-cell molecular dynamics (or in stress calculation). See erf_sigma for details.
    default_value: "0.0"
    unit: Ry
    availability: ""
  - name: fft_mode
    category: Plane wave related variables
    type: Integer
    description: |
      Set the mode of FFTW.
      * 0: FFTW_ESTIMATE
      * 1: FFTW_MEASURE
      * 2: FFTW_PATIENT
      * 3: FFTW_EXHAUSTIVE
    default_value: "0"
    unit: ""
    availability: ""
  - name: erf_height
    category: Plane wave related variables
    type: Real
    description: |
      Used in variable-cell molecular dynamics (or in stress calculation). See erf_sigma for details.
    default_value: "0.0"
    unit: Ry
    availability: ""
  - name: erf_sigma
    category: Plane wave related variables
    type: Real
    description: |
      In order to recover the accuracy of a constant energy cutoff calculation, the kinetic functional is modified, which is used in variable-cell molecular dynamics (or in stress calculation).
    default_value: "0.1"
    unit: Ry
    availability: ""
  - name: stru_file
    category: Input files
    type: String
    description: |
      The name of the structure file containing various information about atom species, including pseudopotential files, local orbitals files, cell information, atom positions, and whether atoms should be allowed to move.
    default_value: STRU
    unit: ""
    availability: ""
  - name: kpoint_file
    category: Input files
    type: String
    description: |
      The name of the k-point file that includes the k-point information of Brillouin zone.
    default_value: KPT
    unit: ""
    availability: ""
  - name: pseudo_dir
    category: Input files
    type: String
    description: |
      The directory of pseudopotential files. This parameter is combined with the pseudopotential filenames in the STRU file to form the complete pseudopotential file paths.
    default_value: "\"\""
    unit: ""
    availability: ""
  - name: orbital_dir
    category: Input files
    type: String
    description: |
      The directory to save numerical atomic orbitals. This parameter is combined with orbital filenames in the STRU file to form the complete orbital file paths.
    default_value: "\"\""
    unit: ""
    availability: ""
  - name: read_file_dir
    category: Input files
    type: String
    description: |
      Location of files, such as the electron density (chgs1.cube), required as a starting point.
    default_value: OUT.$suffix
    unit: ""
    availability: ""
  - name: restart_load
    category: Input files
    type: Boolean
    description: |
      If restart_save is set to true and an electronic iteration is finished, calculations can be restarted from the charge density file, which are saved in the former calculation.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: basis_type
    category: Electronic structure
    type: String
    description: |
      Choose the basis set.
      * pw: Using plane-wave basis set only.
      * lcao: Using localized atomic orbital sets.
      * lcao_in_pw: Expand the localized atomic set in plane-wave basis, non-self-consistent field calculation not tested.
    default_value: pw
    unit: ""
    availability: ""
  - name: ks_solver
    category: Electronic structure
    type: String
    description: |
      Choose the diagonalization methods for the Hamiltonian matrix expanded in a certain basis set.

      For plane-wave basis,

      * cg: The conjugate-gradient (CG) method.
      * dav: The Davidson algorithm.
      * dav_subspace: The Davidson algorithm without orthogonalization operation, this method is the most recommended for efficiency. `pw_diag_ndim` can be set to 2 for this method.
      * bpcg: The BPCG method, which is a block-parallel Conjugate Gradient (CG) method, typically exhibits higher acceleration in a GPU environment. The BPCG method is currently under testing and is not recommended for use.

      For numerical atomic orbitals basis,

      * lapack: Use LAPACK to diagonalize the Hamiltonian, only used for serial version
      * genelpa: Use the CPU-only GEN-ELPA interface to diagonalize the Hamiltonian.
      * scalapack_gvx: Use Scalapack to diagonalize the Hamiltonian.
      * cusolver: Use CUSOLVER to diagonalize the Hamiltonian, at least one GPU is needed.
      * cusolvermp: Use CUSOLVER to diagonalize the Hamiltonian, supporting multi-GPU devices. Note that you should set the number of MPI processes equal to the number of GPUs.
      * elpa: The ELPA solver supports both CPU and GPU. By setting the `device` to GPU, you can launch the ELPA solver with GPU acceleration (provided that you have installed a GPU-supported version of ELPA, which requires you to manually compile and install ELPA, and the ABACUS should be compiled with -DENABLE_ELPA=ON and -DUSE_CUDA=ON). The ELPA solver also supports multi-GPU acceleration.

      If you set ks_solver=`genelpa` for basis_type=`pw`, the program will stop with an error message:

      ``text genelpa can not be used with plane wave basis. ``

      Then the user has to correct the input file and restart the calculation.
    default_value: "\n    - PW basis: cg.\n    - LCAO basis:\n        - genelpa (if compiling option `ENABLE_ELPA` has been set)\n        - lapack (if compiling option `ENABLE_MPI` has not been set)\n        - scalapack_gvx (if compiling option `ENABLE_ELPA` has not been set and compiling option `ENABLE_MPI` has been set)\n        - cusolver (if compiling option `USE_CUDA` has been set)"
    unit: ""
    availability: ""
  - name: nbands
    category: Electronic structure
    type: Integer
    description: |
      The number of Kohn-Sham orbitals to calculate. It is recommended to setup this value, especially when smearing techniques are utilized, more bands should be included.
    default_value: ""
    unit: ""
    availability: ""
  - name: nelec
    category: Electronic structure
    type: Real
    description: |
      * 0.0: The total number of electrons will be calculated by the sum of valence electrons (i.e. assuming neutral system).
      * >0.0: this denotes the total number of electrons in the system. Must be less than 2*nbands.
    default_value: "0.0"
    unit: ""
    availability: ""
  - name: nelec_delta
    category: Electronic structure
    type: Real
    description: |
      The total number of electrons will be calculated by nelec+nelec_delta.
    default_value: "0.0"
    unit: ""
    availability: ""
  - name: nupdown
    category: Electronic structure
    type: Real
    description: |
      * 0.0: no constrain apply to system.
      * >0.0: The different number of electrons between spin-up and spin-down channels. The range of value must be in [-nelec ~ nelec]. It is one type of constrainted DFT method, two Fermi energies will be calculated.
    default_value: "0.0"
    unit: ""
    availability: ""
  - name: dft_functional
    category: Electronic structure
    type: String
    description: |
      In our package, the XC functional can either be set explicitly using the dft_functional keyword in INPUT file. If dft_functional is not specified, ABACUS will use the xc functional indicated in the pseudopotential file. On the other hand, if dft_functional is specified, it will overwrite the functional from pseudopotentials and performs calculation with whichever functional the user prefers. We further offer two ways of supplying exchange-correlation functional. The first is using 'short-hand' names. A complete list of 'short-hand' expressions can be found in the source code. Supported density functionals are:
      * LDA functionals
        * LDA (equivalent with PZ and SLAPZNOGXNOGC), PWLDA
      * GGA functionals
        * PBE (equivalent with SLAPWPBXPBC), PBESOL, REVPBE, WC, BLYP, BP(referred to BP86), PW91, HCTH, OLYP, BLYP_LR
      * meta-GGA functionals
        * SCAN (require LIBXC)
      * Hybrid functionals
        * PBE0, HF
        * If LIBXC is available, additional short-hand names of hybrid functionals are supported: HSE(referred to HSE06), B3LYP, LC_PBE, LC_WPBE, LRC_WPBE, LRC_WPBEH, CAM_PBEH, WP22, CWP22, MULLER (equivalent with POWER)
      * Hybrid meta-GGA functionals
        * SCAN0 (require LIBXC)

      The other way is only available when compiling with LIBXC, and it allows for supplying exchange-correlation functionals as combinations of LIBXC keywords for functional components, joined by a plus sign, for example, dft_functional='LDA_X_1D_EXPONENTIAL+LDA_C_1D_CSC'.
    default_value: Used the same as DFT functional as specified in the pseudopotential files.
    unit: ""
    availability: ""
  - name: xc_temperature
    category: Electronic structure
    type: Real
    description: |
      Specifies temperature when using temperature-dependent XC functionals (KSDT and so on).
    default_value: "0.0"
    unit: Ry
    availability: ""
  - name: xc_exch_ext
    category: Electronic structure
    type: Integer followed by Real values
    description: |
      Customized parameterization of the exchange part of an XC functional. The first value should be the Libxc ID of the original functional, followed by the complete list of external parameters required by the linked Libxc version. If unset, Libxc's own default parameters are used. For functional IDs and parameter definitions, refer to the Libxc documentation and source code.

      [NOTE] Solely setting this keyword will take no effect on XC functionals. One should also set dft_functional to the corresponding functional to apply the customized parameterization. Presently this feature can only support parameterization on one exchange functional.
    default_value: ""
    unit: ""
    availability: ""
  - name: xc_corr_ext
    category: Electronic structure
    type: Integer followed by Real values
    description: |
      Customized parameterization of the correlation part of an XC functional. The first value should be the Libxc ID of the original functional, followed by the complete list of external parameters required by the linked Libxc version. If unset, Libxc's own default parameters are used. For functional IDs and parameter definitions, refer to the Libxc documentation and source code.

      [NOTE] Solely setting this keyword will take no effect on XC functionals. One should also set dft_functional to the corresponding functional to apply the customized parameterization. Presently this feature can only support parameterization on one correlation functional.
    default_value: ""
    unit: ""
    availability: ""
  - name: pseudo_rcut
    category: Electronic structure
    type: Real
    description: |
      Cut-off of radial integration for pseudopotentials.
    default_value: "15"
    unit: Bohr
    availability: ""
  - name: pseudo_mesh
    category: Electronic structure
    type: Boolean
    description: |
      * 0: Use a mesh for radial integration of pseudopotentials.
      * 1: Use the mesh that is consistent with quantum espresso
    default_value: "0"
    unit: ""
    availability: ""
  - name: nspin
    category: Electronic structure
    type: Integer
    description: |
      The number of spin components of wave functions.
      * 1: Spin degeneracy
      * 2: Collinear spin polarized.
      * 4: Noncollinear or spin-orbit calculations. Set nspin to 4 explicitly when noncolin or lspinorb is enabled.
    default_value: "1"
    unit: ""
    availability: ""
  - name: smearing_method
    category: Electronic structure
    type: String
    description: |
      It indicates which occupation and smearing method is used in the calculation.
      * fixed: fixed occupations (available for non-coductors only)
      * gauss or gaussian: Gaussian smearing method.
      * mp: methfessel-paxton smearing method; recommended for metals.
      * mp2: 2-nd methfessel-paxton smearing method; recommended for metals.
      * mv or cold: marzari-vanderbilt smearing method.
      * fd: Fermi-Dirac smearing method: and smearing_sigma below is the temperature (in Ry).
    default_value: gauss
    unit: ""
    availability: ""
  - name: smearing_sigma
    category: Electronic structure
    type: Real
    description: |
      Energy range for smearing.
    default_value: "0.015"
    unit: Ry
    availability: ""
  - name: smearing_sigma_temp
    category: Electronic structure
    type: Real
    description: |
      Energy range for smearing, smearing_sigma = 1/2 kB smearing_sigma_temp.
    default_value: "2 * smearing_sigma / kB."
    unit: K
    availability: ""
  - name: mixing_type
    category: Electronic structure
    type: String
    description: |
      Charge mixing methods.
      * plain: Just simple mixing.
      * pulay: Standard Pulay method. P. Pulay Chemical Physics Letters, (1980)
      * broyden: Simplified modified Broyden method. D.D. Johnson Physical Review B (1988)

      In general, the convergence of the Broyden method is slightly faster than that of the Pulay method.
    default_value: broyden
    unit: ""
    availability: ""
  - name: mixing_beta
    category: Electronic structure
    type: Real
    description: |
      In general, the formula of charge mixing can be written as rho_new = rho_old + mixing_beta * drho, where rho_new represents the new charge density after charge mixing, rho_old represents the charge density in previous step, drho is obtained through various mixing methods, and mixing_beta is set by this parameter. A lower value of 'mixing_beta' results in less influence of drho on rho_new, making the self-consistent field (SCF) calculation more stable. However, it may require more steps to achieve convergence. We recommend the following options:
      * 0.8: nspin=1
      * 0.4: nspin=2 and nspin=4
      * 0: keep charge density unchanged, usually used for restarting with init_chg=file or testing.
      * 0.1 or less: if convergence of SCF calculation is difficult to reach, please try 0 < mixing_beta < 0.1.
      A progressive tuning strategy might help, for example, 0.4 -> 0.1 -> 0.025.

      Note: For low-dimensional large systems, the setup of mixing_beta=0.1, mixing_ndim=20, and mixing_gg0=1.0 usually works well.

      For spin-polarized calculations (nspin=2 or nspin=4) that are difficult to converge, try reducing both mixing_beta and mixing_beta_mag simultaneously, e.g., mixing_beta=0.1 and mixing_beta_mag=0.1 or lower.
    default_value: "0.8 for nspin=1, 0.4 for nspin=2 and nspin=4."
    unit: ""
    availability: ""
  - name: mixing_beta_mag
    category: Electronic structure
    type: Real
    description: |
      Mixing parameter of magnetic density.

      If SCF convergence is difficult with spin polarization (nspin=2 or nspin=4), try reducing both mixing_beta and mixing_beta_mag simultaneously, e.g., mixing_beta=0.1 and mixing_beta_mag=0.1 or lower.
    default_value: "4*mixing_beta, but the maximum value is 1.6."
    unit: ""
    availability: ""
  - name: mixing_ndim
    category: Electronic structure
    type: Integer
    description: |
      It indicates the mixing dimensions in Pulay or Broyden. Pulay and Broyden method use the density from previous mixing_ndim steps and do a charge mixing based on this density.

      For systems that are difficult to converge, one could try increasing the value of 'mixing_ndim' to enhance the stability of the self-consistent field (SCF) calculation.
    default_value: "8"
    unit: ""
    availability: ""
  - name: mixing_restart
    category: Electronic structure
    type: Real
    description: |
      If the density difference between input and output drho is smaller than mixing_restart, SCF will restart at next step which means SCF will restart by using output charge density from perivos iteration as input charge density directly, and start a new mixing. Notice that mixing_restart will only take effect once in one SCF.
    default_value: "0"
    unit: ""
    availability: ""
  - name: mixing_dmr
    category: Electronic structure
    type: Boolean
    description: |
      At n-th iteration which is calculated by drho<mixing_restart, SCF will start a mixing for real-space density matrix by using the same coefficiences as the mixing of charge density.
    default_value: "false"
    unit: ""
    availability: "mixing_restart>0"
  - name: mixing_gg0
    category: Electronic structure
    type: Real
    description: |
      Controls the Kerker preconditioner for charge-density mixing.
      * >0: Enables Kerker scaling to suppress long-wavelength (small-G) charge-density fluctuations. Setting mixing_gg0 = 1.0 is normally a good starting point. This setting has no effect when mixing_beta <= 0.1 because the charge-density Kerker preconditioner is bypassed.
      * 0: No Kerker scaling is performed.

      For systems that are difficult to converge, particularly metallic systems, enabling Kerker scaling may aid in achieving convergence.
    default_value: "1.0"
    unit: ""
    availability: ""
  - name: mixing_gg0_mag
    category: Electronic structure
    type: Real
    description: |
      Controls the Kerker preconditioner for magnetic-density mixing. It is disabled by default and is generally only recommended for systems whose magnetic density is difficult to converge.

      The magnetic-density Kerker preconditioner is bypassed when mixing_beta_mag <= 0.1, so mixing_gg0_mag has no effect in that regime. It is also unavailable when the charge-density Kerker preconditioner itself is bypassed.
    default_value: "0.0"
    unit: ""
    availability: ""
  - name: mixing_gg0_min
    category: Electronic structure
    type: Real
    description: |
      Sets the lower bound used by the Kerker filter. The lower bound is evaluated as mixing_gg0_min / mixing_beta for charge-density mixing and mixing_gg0_min / mixing_beta_mag for magnetic-density mixing.

      In the current implementation, the automatic bypass thresholds are fixed independently of mixing_gg0_min: charge-density Kerker is bypassed when mixing_beta <= 0.1, and magnetic-density Kerker is bypassed when mixing_beta_mag <= 0.1. Changing mixing_gg0_min does not change these thresholds or re-enable Kerker.
    default_value: "0.1"
    unit: ""
    availability: ""
  - name: mixing_angle
    category: Electronic structure
    type: Real
    description: |
      Normal broyden mixing can give the converged result for a given magnetic configuration. If one is not interested in the energies of a given magnetic configuration but wants to determine the ground state by relaxing the magnetic moments' directions, one cannot rely on the standard Broyden mixing algorithm. To enhance the ability to find correct magnetic configuration for non-colinear calculations, ABACUS implements a promising mixing method proposed by J. Phys. Soc. Jpn. 82 (2013) 114706. Here, mixing_angle is the angle mixing parameter. In fact, only mixing_angle=1.0 is implemented currently.
      * <=0: Normal broyden mixing
      * >0: Angle mixing for the modulus with mixing_angle=1.0
    default_value: "-10.0"
    unit: ""
    availability: nspin==4
  - name: mixing_tau
    category: Electronic structure
    type: Boolean
    description: |
      Whether to mix the kinetic energy density.
      * True: The kinetic energy density will also be mixed. It seems for general cases, SCF converges fine even without this mixing. However, if there is difficulty in converging SCF for meta-GGA, it might be helpful to turn this on.
      * False: The kinetic energy density will not be mixed.

      This setting takes effect only when the selected exchange-correlation functional uses the kinetic energy density, such as a meta-GGA or hybrid meta-GGA functional.
    default_value: "False"
    unit: ""
    availability: ""
  - name: mixing_dftu
    category: Electronic structure
    type: Boolean
    description: |
      Whether to mix the occupation matrices.
      * True: The occupation matrices will also be mixed by plain mixing. From experience this is not very helpful if the +U calculation does not converge.
      * False: The occupation matrices will not be mixed.
    default_value: "False"
    unit: ""
    availability: dft_plus_u==1
  - name: gamma_only
    category: Electronic structure
    type: Boolean
    description: |
      Whether to use gamma_only algorithm.
      * 0: more than one k-point is used and the ABACUS is slower compared to the gamma only algorithm.
      * 1: ABACUS uses gamma only, the algorithm is faster and you don't need to specify the k-points file.

      Note: If gamma_only is set to 1, the KPT file will be overwritten. So make sure to turn off gamma_only for multi-k calculations.
    default_value: "0"
    unit: ""
    availability: basis_type==lcao
  - name: scf_nmax
    category: Electronic structure
    type: Integer
    description: |
      This variable indicates the maximal iteration number for electronic iterations.
    default_value: "100"
    unit: ""
    availability: ""
  - name: scf_thr
    category: Electronic structure
    type: Real
    description: |
      It's the density threshold for electronic iteration. It represents the charge density error between two sequential densities from electronic iterations. Usually for local orbitals, usually 1e-6 may be accurate enough.
    default_value: "1.0e-9 (plane-wave basis), or 1.0e-7 (localized atomic orbital basis)."
    unit: "Ry if scf_thr_type=1, dimensionless if scf_thr_type=2"
    availability: ""
  - name: scf_ene_thr
    category: Electronic structure
    type: Real
    description: |
      It's the energy threshold for electronic iteration. It represents the total energy error between two sequential densities from electronic iterations.
    default_value: "-1.0. If the user does not set this parameter, it will not take effect."
    unit: eV
    availability: ""
  - name: scf_thr_type
    category: Electronic structure
    type: Integer
    description: |
      Choose the calculation method of convergence criterion.
      * 1: the criterion is defined in reciprocal space, which is used in SCF of PW basis with unit Ry.
      * 2: the criterion is defined in real space, where is the number of electron, which is used in SCF of LCAO with unit dimensionless.
    default_value: "1 (plane-wave basis), or 2 (localized atomic orbital basis)."
    unit: ""
    availability: ""
  - name: scf_os_stop
    category: Electronic structure
    type: Boolean
    description: |
      For systems that are difficult to converge, the SCF process may exhibit oscillations in charge density, preventing further progress toward the specified convergence criteria and resulting in continuous oscillation until the maximum number of steps is reached; this greatly wastes computational resources. To address this issue, this function allows ABACUS to terminate the SCF process early upon detecting oscillations, thus reducing subsequent meaningless calculations. The detection of oscillations is based on the slope of the logarithm of historical drho values. To this end, Least Squares Method is used to calculate the slope of the logarithmically taken drho for the previous scf_os_ndim iterations. If the calculated slope is larger than scf_os_thr, stop the SCF.

      * 0: The SCF will continue to run regardless of whether there is oscillation or not.
      * 1: If the calculated slope is larger than scf_os_thr, stop the SCF.
    default_value: "false"
    unit: ""
    availability: ""
  - name: scf_os_thr
    category: Electronic structure
    type: Real
    description: |
      The slope threshold to determine if the SCF is stuck in a charge density oscillation. If the calculated slope is larger than scf_os_thr, stop the SCF.
    default_value: "-0.01"
    unit: ""
    availability: ""
  - name: scf_os_ndim
    category: Electronic structure
    type: Integer
    description: |
      To determine the number of old iterations' drho used in slope calculations.
    default_value: mixing_ndim
    unit: ""
    availability: ""
  - name: sc_os_ndim
    category: Electronic structure
    type: Integer
    description: |
      To determine the number of old iterations to judge oscillation, it occured, more accurate lambda with DeltaSpin method would be calculated, only for PW base.
    default_value: "5"
    unit: ""
    availability: ""
  - name: lspinorb
    category: Electronic structure
    type: Boolean
    description: |
      Whether to consider spin-orbit coupling (SOC) effect in the calculation.
      * True: Consider spin-orbit coupling effect. When enabled:
        * nspin must be explicitly set to 4 (noncollinear spin representation)
        * Symmetry is automatically disabled (SOC breaks inversion symmetry)
        * Requires full-relativistic pseudopotentials with has_so=true in the UPF header
      * False: Do not consider spin-orbit coupling effect.
      * Common Error: "no soc upf used for lspinorb calculation" - ensure you are using full-relativistic pseudopotentials
    default_value: "False"
    unit: ""
    availability: ""
  - name: noncolin
    category: Electronic structure
    type: Boolean
    description: |
      Whether to allow non-collinear magnetic moments, where magnetization can point in arbitrary directions (x, y, z components) rather than being constrained to the z-axis.
      * True: Allow non-collinear polarization. When enabled:
        * nspin must be explicitly set to 4
        * Wave function dimension is doubled (npol=2), and the number of occupied states is doubled
        * Charge density has 4 components (Pauli spin matrices)
        * Cannot be used with gamma_only=true
        * Can be combined with lspinorb=true for SOC effects with non-collinear magnetism
      * False: Do not allow non-collinear polarization (magnetization constrained to z-axis).
      * Relationship with lspinorb:
        * noncolin=0, lspinorb=1: SOC with z-axis magnetism only (for non-magnetic materials with SOC)
        * noncolin=1, lspinorb=0: Non-collinear magnetism without SOC
        * noncolin=1, lspinorb=1: Both non-collinear magnetism and SOC
    default_value: "False"
    unit: ""
    availability: ""
  - name: soc_lambda
    category: Electronic structure
    type: Real
    description: |
      Modulates the strength of spin-orbit coupling effect. Sometimes, for some real materials, both scalar-relativistic and full-relativistic pseudopotentials cannot describe the exact spin-orbit coupling. Artificial modulation may help in such cases.

      soc_lambda, which has value range [0.0, 1.0], is used to modulate SOC effect:
      * soc_lambda 0.0: Scalar-relativistic case (no SOC)
      * soc_lambda 1.0: Full-relativistic case (full SOC)
      * Intermediate values: Partial-relativistic SOC (interpolation between scalar and full)

      Use case: When experimental or high-level theoretical results suggest that the SOC effect is weaker or stronger than what full-relativistic pseudopotentials predict, you can adjust this parameter to match the target behavior.
    default_value: "1.0"
    unit: ""
    availability: lspinorb==true
  - name: dfthalf_type
    category: Electronic structure
    type: Integer
    description: |
      DFT-1/2 type:
      * 0: DFT-1/2 is off.
      * 1: Shell DFT-1/2 method is used.
    default_value: "0"
    unit: ""
    availability: ""
  - name: pw_diag_thr
    category: Plane wave related variables
    type: Real
    description: |
      Only used when you use ks_solver = cg/dav/dav_subspace/bpcg. It indicates the threshold for the first electronic iteration, from the second iteration the pw_diag_thr will be updated automatically. For nscf calculations with planewave basis set, pw_diag_thr should be <= 1e-3.
    default_value: "0.01"
    unit: ""
    availability: ""
  - name: diago_smooth_ethr
    category: Plane wave related variables
    type: Boolean
    description: |
      If TRUE, the smooth threshold strategy, which applies a larger threshold (10e-5) for the empty states, will be implemented in the diagonalization methods. (This strategy should not affect total energy, forces, and other ground-state properties, but computational efficiency will be improved.) If FALSE, the smooth threshold strategy will not be applied.
    default_value: "false"
    unit: ""
    availability: ""
  - name: use_k_continuity
    category: Plane wave related variables
    type: Boolean
    description: |
      If TRUE, the wavefunctions at k-point will be initialized from the converged wavefunctions at the nearest k-point, which can speed up the SCF convergence. Only works for PW basis.
    default_value: "false"
    unit: ""
    availability: basis_type==pw
  - name: pw_diag_nmax
    category: Plane wave related variables
    type: Integer
    description: |
      Only useful when you use ks_solver = cg/dav/dav_subspace/bpcg. It indicates the maximal iteration number for cg/david/dav_subspace/bpcg method.
    default_value: "50"
    unit: ""
    availability: "basis_type==pw and ks_solver in [cg, dav, dav_subspace, bpcg]"
  - name: pw_diag_ndim
    category: Plane wave related variables
    type: Integer
    description: |
      Only useful when you use ks_solver = dav or ks_solver = dav_subspace. It indicates dimension of workspace(number of wavefunction packets, at least 2 needed) for the Davidson method. A larger value may yield a smaller number of iterations in the algorithm but uses more memory and more CPU time in subspace diagonalization.
    default_value: "4"
    unit: ""
    availability: ""
  - name: diago_cg_prec
    category: Plane wave related variables
    type: Integer
    description: |
      Preconditioner type for conjugate gradient diagonalization method.
    default_value: "1"
    unit: ""
    availability: ""
  - name: nb2d
    category: System variables
    type: Integer
    description: |
      In LCAO calculations, the Hamiltonian and overlap matrices are distributed across 2D processor grid. This parameter controls the 2D block size for distribution.
    default_value: "0"
    unit: ""
    availability: ""
  - name: lmaxmax
    category: Numerical atomic orbitals related variables
    type: Integer
    description: |
      If not equals to 2, then the maximum l channels on LCAO is set to lmaxmax. If 2, then the number of l channels will be read from the LCAO data sets. Normally no input should be supplied for this variable so that it is kept as its default.
    default_value: "2."
    unit: ""
    availability: ""
  - name: lcao_ecut
    category: Numerical atomic orbitals related variables
    type: Real
    description: |
      Energy cutoff (in Ry) for two-center integrals in LCAO. The two-center integration table are obtained via a k space integral whose upper limit is about sqrt(lcao_ecut).
    default_value: ecutwfc
    unit: ""
    availability: ""
  - name: lcao_dk
    category: Numerical atomic orbitals related variables
    type: Real
    description: |
      the interval of k points for two-center integrals. The two-center integration table are obtained via a k space integral on a uniform grid with spacing lcao_dk.
    default_value: "0.01"
    unit: Bohr
    availability: ""
  - name: lcao_dr
    category: Numerical atomic orbitals related variables
    type: Real
    description: |
      r spacing of the integration table of two-center integrals.
    default_value: "0.01"
    unit: Bohr
    availability: ""
  - name: lcao_rmax
    category: Numerical atomic orbitals related variables
    type: Real
    description: |
      Maximum distance for the two-center integration table.
    default_value: "30"
    unit: Bohr
    availability: ""
  - name: search_radius
    category: Numerical atomic orbitals related variables
    type: Real
    description: |
      Searching radius in finding the neighbouring atoms. By default the radius will be automatically determined by the cutoffs of orbitals and nonlocal beta projectors.
    default_value: "-1"
    unit: Bohr
    availability: ""
  - name: "bx"
    category: Numerical atomic orbitals related variables
    type: Integer
    description: |
      In the matrix operation of grid integral, bx/by/bz grids (in x, y, z directions) are treated as a whole as a matrix element. A different value will affect the calculation speed. The default is 0, which means abacus will automatically calculate these values.
    default_value: "0"
    unit: ""
    availability: ""
  - name: by
    category: Numerical atomic orbitals related variables
    type: Integer
    description: |
      In the matrix operation of grid integral, bx/by/bz grids (in x, y, z directions) are treated as a whole as a matrix element. A different value will affect the calculation speed. The default is 0, which means abacus will automatically calculate these values.
    default_value: "0"
    unit: ""
    availability: ""
  - name: bz
    category: Numerical atomic orbitals related variables
    type: Integer
    description: |
      In the matrix operation of grid integral, bx/by/bz grids (in x, y, z directions) are treated as a whole as a matrix element. A different value will affect the calculation speed. The default is 0, which means abacus will automatically calculate these values.
    default_value: "0"
    unit: ""
    availability: ""
  - name: elpa_num_thread
    category: Numerical atomic orbitals related variables
    type: Integer
    description: |
      Number of threads used in one elpa calculation.

      If the number is below 0 or 0 or beyond the max number of threads, all elpa calculation will be using all mpi threads
    default_value: "-1"
    unit: ""
    availability: ""
  - name: num_stream
    category: Numerical atomic orbitals related variables
    type: Integer
    description: |
      The number of CUDA streams used in LCAO calculations with GPU acceleration.
    default_value: "4"
    unit: ""
    availability: ""
  - name: bessel_nao_ecut
    category: NAOs
    type: String
    description: |
      "Energy cutoff" (in Ry) of spherical Bessel functions. The number of spherical Bessel functions that constitute the radial parts of NAOs is determined by sqrt(bessel_nao_ecut)*bessel_nao_rcut/.
    default_value: ecutwfc
    unit: ""
    availability: ""
  - name: bessel_nao_tolerence
    category: NAOs
    type: Real
    description: |
      Tolerance when searching for the zeros of spherical Bessel functions.
    default_value: "1.0e-12"
    unit: ""
    availability: ""
  - name: bessel_nao_rcut
    category: NAOs
    type: Vector of Real (N values)
    description: |
      Cutoff radius (in Bohr) and the common node of spherical Bessel functions used to construct the NAOs.
    default_value: "6.0"
    unit: ""
    availability: ""
  - name: bessel_nao_smooth
    category: NAOs
    type: Boolean
    description: |
      If True, NAOs will be smoothed near the cutoff radius. See bessel_nao_rcut and bessel_nao_sigma for parameters.
    default_value: "True"
    unit: ""
    availability: ""
  - name: bessel_nao_sigma
    category: NAOs
    type: Real
    description: |
      Smoothing range (in Bohr). See also bessel_nao_smooth.
    default_value: "0.1"
    unit: ""
    availability: ""
  - name: relax_method
    category: Geometry relaxation
    type: Vector of string
    description: |
      The method used for geometry optimization.

      First element (algorithm selection):
      * cg: Conjugate gradient (CG) algorithm.
      * bfgs: Broyden–Fletcher–Goldfarb–Shanno (BFGS) quasi-Newton algorithm.
      * lbfgs: Limited-memory BFGS algorithm, suitable for large systems.
      * cg_bfgs: Mixed method starting with CG and switching to BFGS when force convergence reaches relax_cg_thr.
      * sd: Steepest descent algorithm. Not recommended for production use.

      Optional second element:
      * cg 1: First optimize ionic positions at fixed cell, then update the cell, and repeat.
      * cg 2 or omitted: Simultaneously optimize ionic positions and cell parameters with line search (recommended).
      * bfgs 1: Traditional BFGS that updates the Hessian matrix B and then inverts it.
      * bfgs 2 or omitted: Default BFGS that directly updates the inverse Hessian (recommended).

      The second element is not accepted by other methods.

      [NOTE] In the 3.10-LTS version, the type of this parameter is std::string. It can be set to "cg", "bfgs", "cg_bfgs", "bfgs_trad", "lbfgs", "sd", "fire".
    default_value: cg 2
    unit: ""
    availability: ""
  - name: relax_scale_force
    category: Geometry relaxation
    type: Real
    description: |
      The paramether controls the size of the first conjugate gradient step. A smaller value means the first step along a new CG direction is smaller. This might be helpful for large systems, where it is safer to take a smaller initial step to prevent the collapse of the whole configuration.
    default_value: "0.5"
    unit: ""
    availability: "relax_method==\"cg 2\""
  - name: relax_nmax
    category: Geometry relaxation
    type: Integer
    description: |
      The maximal number of ionic iteration steps. If set to 0, the code performs a quick "dry run", stopping just after initialization. This is useful to check for input correctness and to have the summary printed.
    default_value: "1 for SCF, 50 for relax and cell-relax calcualtions"
    unit: ""
    availability: ""
  - name: relax_cg_thr
    category: Geometry relaxation
    type: Real
    description: |
      When relax_method is set to cg_bfgs, a mixed algorithm of conjugate gradient (CG) and Broyden–Fletcher–Goldfarb–Shanno (BFGS) is used. The ions first move according to the CG method, then switch to the BFGS method when the maximum force on atoms is reduced below this threshold.
    default_value: "0.5"
    unit: eV/Angstrom
    availability: relax_method==cg_bfgs
  - name: force_thr
    category: Geometry relaxation
    type: Real
    description: |
      Threshold of the force convergence. The threshold is compared with the largest force among all of the atoms. The recommended value for using atomic orbitals is 0.04 eV/Angstrom (0.0016 Ry/Bohr). The parameter is equivalent to force_thr_ev except for the unit, you can choose either you like.
    default_value: "0.001"
    unit: Ry/Bohr (25.7112 eV/Angstrom)
    availability: ""
  - name: force_thr_ev
    category: Geometry relaxation
    type: Real
    description: |
      Threshold of the force convergence. The threshold is compared with the largest force among all of the atoms. The recommended value for using atomic orbitals is 0.04 eV/Angstrom (0.0016 Ry/Bohr). The parameter is equivalent to force_thr except for the unit. You may choose either you like.
    default_value: "0.0257112"
    unit: eV/Angstrom (0.03889 Ry/Bohr)
    availability: ""
  - name: force_zero_out
    category: Geometry relaxation
    type: Real
    description: |
      The atomic forces that are smaller than force_zero_out will be treated as zero.
    default_value: "0.0"
    unit: eV/Angstrom
    availability: ""
  - name: relax_bfgs_w1
    category: Geometry relaxation
    type: Real
    description: |
      Controls the Wolfe condition for the Broyden–Fletcher–Goldfarb–Shanno (BFGS) algorithm used in geometry relaxation. This parameter sets the sufficient decrease condition (c1 in Wolfe conditions). For more information, see Phys. Chem. Chem. Phys., 2000, 2, 2177.
    default_value: "0.01"
    unit: ""
    availability: "relax_method in [bfgs, cg_bfgs]"
  - name: relax_bfgs_w2
    category: Geometry relaxation
    type: Real
    description: |
      Controls the Wolfe condition for the Broyden–Fletcher–Goldfarb–Shanno (BFGS) algorithm used in geometry relaxation. This parameter sets the curvature condition (c2 in Wolfe conditions). For more information, see Phys. Chem. Chem. Phys., 2000, 2, 2177.
    default_value: "0.5"
    unit: ""
    availability: "relax_method in [bfgs, cg_bfgs]"
  - name: relax_bfgs_rmax
    category: Geometry relaxation
    type: Real
    description: |
      Maximum allowed total displacement of all atoms during geometry optimization. The sum of atomic displacements can increase during optimization steps but cannot exceed this value.
    default_value: "0.8"
    unit: Bohr
    availability: "relax_method in [bfgs, cg_bfgs]"
  - name: relax_bfgs_rmin
    category: Geometry relaxation
    type: Real
    description: |
      Minimum allowed total displacement of all atoms. When the total atomic displacement falls below this value and force convergence is not achieved, the calculation will terminate. Note: This parameter is not used in the default BFGS algorithm (relax_method = bfgs 2 or bfgs).
    default_value: "1e-5"
    unit: Bohr
    availability: "relax_method==\"bfgs 1\""
  - name: relax_bfgs_init
    category: Geometry relaxation
    type: Real
    description: |
      Initial total displacement of all atoms in the first BFGS step. This sets the scale for the initial movement.
    default_value: "0.5"
    unit: Bohr
    availability: "relax_method in [bfgs, cg_bfgs]"
  - name: stress_thr
    category: Geometry relaxation
    type: Real
    description: |
      The threshold of the stress convergence. The threshold is compared with the largest component of the stress tensor.
    default_value: "0.5"
    unit: kbar
    availability: ""
  - name: press1
    category: Geometry relaxation
    type: Real
    description: |
      The external pressures along three axes. Positive input value is taken as compressive stress.
    default_value: "0"
    unit: kbar
    availability: ""
  - name: press2
    category: Geometry relaxation
    type: Real
    description: |
      The external pressures along three axes. Positive input value is taken as compressive stress.
    default_value: "0"
    unit: kbar
    availability: ""
  - name: press3
    category: Geometry relaxation
    type: Real
    description: |
      The external pressures along three axes. Positive input value is taken as compressive stress.
    default_value: "0"
    unit: kbar
    availability: ""
  - name: fixed_axes
    category: Geometry relaxation
    type: String
    description: |
      Specifies which cell degrees of freedom are fixed during variable-cell relaxation. The available options depend on relax_method:

      With relax_method = cg 2 (default), all options are available:
      * None: Default; all cell parameters can relax freely
      * volume: Relaxation with fixed volume (allows shape changes)
      * shape: Fix shape but allow volume changes (hydrostatic pressure only)
      * a: Fix the a-axis lattice vector during relaxation
      * b: Fix the b-axis lattice vector during relaxation
      * c: Fix the c-axis lattice vector during relaxation
      * ab: Fix both a and b axes during relaxation
      * ac: Fix both a and c axes during relaxation
      * bc: Fix both b and c axes during relaxation
      * abc: Fix all three lattice vectors during relaxation

      With relax_method set to cg 1, bfgs, lbfgs, sd, or cg_bfgs, None and a, b, c, ab, ac, bc, abc are available. The shape and volume options require cg 2.

      [NOTE] For VASP users, see the ISIF correspondence table in the geometry optimization documentation.
    default_value: None
    unit: ""
    availability: calculation==cell-relax
  - name: fixed_ibrav
    category: Geometry relaxation
    type: Boolean
    description: |
      * True: the lattice type will be preserved during relaxation. The lattice vectors are reconstructed to match the specified Bravais lattice type after each update.
      * False: No restrictions are exerted during relaxation in terms of lattice type

      [NOTE] Note: it is possible to use fixed_ibrav with fixed_axes, but please make sure you know what you are doing. For example, if we are doing relaxation of a simple cubic lattice (latname = "sc"), and we use fixed_ibrav along with fixed_axes = "volume", then the cell is never allowed to move and as a result, the relaxation never converges. When both are used, fixed_ibrav is applied first, then fixed_axes = "volume" rescaling is applied.
    default_value: "False"
    unit: ""
    availability: "relax_method==\"cg 2\" and latname!=none"
  - name: fixed_atoms
    category: Geometry relaxation
    type: Boolean
    description: |
      * True: The direct coordinates of atoms will be preserved during variable-cell relaxation.
      * False: No restrictions are exerted on positions of all atoms. However, users can still fix certain components of certain atoms by using the m keyword in STRU file. For the latter option, check the end of this instruction.
    default_value: "False"
    unit: ""
    availability: ""
  - name: md_type
    category: Molecular dynamics
    type: String
    description: |
      Control the algorithm to integrate the equation of motion for molecular dynamics (MD), see md.md in detail.

      * fire: a MD-based relaxation algorithm, named fast inertial relaxation engine.
      * nve: NVE ensemble with velocity Verlet algorithm.
      * nvt: NVT ensemble, see md_thermostat in detail.
      * npt: Nose-Hoover style NPT ensemble, see md_pmode in detail.
      * langevin: NVT ensemble with Langevin thermostat, see md_damp in detail.
      * msst: MSST method, see msst_direction, msst_vel, msst_qmass, msst_vis, msst_tscale in detail.
    default_value: nvt
    unit: ""
    availability: ""
  - name: md_nstep
    category: Molecular dynamics
    type: Integer
    description: |
      The total number of molecular dynamics steps.
    default_value: "10"
    unit: ""
    availability: ""
  - name: md_dt
    category: Molecular dynamics
    type: Real
    description: |
      The time step used in molecular dynamics calculations.
    default_value: "1.0"
    unit: fs
    availability: ""
  - name: md_thermostat
    category: Molecular dynamics
    type: String
    description: |
      Specify the temperature control method used in NVT ensemble.

      * nhc: Nose-Hoover chain, see md_tfreq and md_tchain in detail.
      * anderson: Anderson thermostat, see md_nraise in detail.
      * berendsen: Berendsen thermostat, see md_nraise in detail.
      * rescaling: velocity Rescaling method 1, see md_tolerance in detail.
      * rescale_v: velocity Rescaling method 2, see md_nraise in detail.
      * csvr: Canonical Sampling through Velocity Rescaling, see md_csvr_tau in detail.
    default_value: nhc
    unit: ""
    availability: ""
  - name: md_tfirst
    category: Molecular dynamics
    type: Real
    description: |
      The temperature used in molecular dynamics calculations.

      If md_tfirst is unset or less than zero, init_vel is autoset to be true. If init_vel is true, the initial temperature will be determined by the velocities read from STRU. In this case, if velocities are unspecified in STRU, the initial temperature is set to zero.

      If md_tfirst is set to a positive value and init_vel is true simultaneously, please make sure they are consistent, otherwise abacus will exit immediately.

      Note that md_tlast is only used in NVT/NPT simulations. If md_tlast is unset or less than zero, md_tlast is set to md_tfirst. If md_tlast is set to be different from md_tfirst, ABACUS will automatically change the temperature from md_tfirst to md_tlast.
    default_value: No default
    unit: K
    availability: ""
  - name: md_tlast
    category: Molecular dynamics
    type: Real
    description: |
      The temperature used in molecular dynamics calculations.

      If md_tfirst is unset or less than zero, init_vel is autoset to be true. If init_vel is true, the initial temperature will be determined by the velocities read from STRU. In this case, if velocities are unspecified in STRU, the initial temperature is set to zero.

      If md_tfirst is set to a positive value and init_vel is true simultaneously, please make sure they are consistent, otherwise abacus will exit immediately.

      Note that md_tlast is only used in NVT/NPT simulations. If md_tlast is unset or less than zero, md_tlast is set to md_tfirst. If md_tlast is set to be different from md_tfirst, ABACUS will automatically change the temperature from md_tfirst to md_tlast.
    default_value: No default
    unit: K
    availability: ""
  - name: md_prec_level
    category: Molecular dynamics
    type: Integer
    description: |
      Determine the precision level of variable-cell molecular dynamics calculations.
      * 0: FFT grids do not change, only G vectors and K vectors are changed due to the change of lattice vector. This level is suitable for cases where the variation of the volume and shape is not large, and the efficiency is relatively higher.
      * 2: FFT grids change per step. This level is suitable for cases where the variation of the volume and shape is large, such as the MSST method. However, accuracy comes at the cost of efficiency.
    default_value: "0"
    unit: ""
    availability: ""
  - name: md_restart
    category: Molecular dynamics
    type: Boolean
    description: |
      Control whether to restart molecular dynamics calculations and time-dependent density functional theory calculations.
      * True: ABACUS will read in {md_step}, then read in the corresponding STRU_MD_suffix/STRU/ automatically. For tddft, ABACUS will also read in WFC_NAO_K${kpoint} of the last step (You need to set out_wfc_lcao=1 and out_app_flag=0 to obtain this file).
      * False: ABACUS will start molecular dynamics calculations normally from the first step.
    default_value: "False"
    unit: ""
    availability: ""
  - name: md_restartfreq
    category: Molecular dynamics
    type: Integer
    description: |
      The output frequency of OUT.{suffix}/STRIU/, which are used to restart molecular dynamics calculations, see md_restart in detail.
    default_value: "5"
    unit: ""
    availability: ""
  - name: md_dumpfreq
    category: Molecular dynamics
    type: Integer
    description: |
      The output frequency of OUT.${suffix}/MD_dump in molecular dynamics calculations, which including the information of lattices and atoms.
    default_value: "1"
    unit: ""
    availability: ""
  - name: dump_force
    category: Molecular dynamics
    type: Boolean
    description: |
      Whether to output atomic forces into the file OUT.${suffix}/MD_dump.
    default_value: "True"
    unit: ""
    availability: ""
  - name: dump_vel
    category: Molecular dynamics
    type: Boolean
    description: |
      Whether to output atomic velocities into the file OUT.${suffix}/MD_dump.
    default_value: "True"
    unit: ""
    availability: ""
  - name: dump_virial
    category: Molecular dynamics
    type: Boolean
    description: |
      Whether to output lattice virials into the file OUT.${suffix}/MD_dump.
    default_value: "True"
    unit: ""
    availability: ""
  - name: md_seed
    category: Molecular dynamics
    type: Integer
    description: |
      The random seed to initialize random numbers used in molecular dynamics calculations.
      * < 0: No srand() function is called.
      * >= 0: The function srand(md_seed) is called.
    default_value: "-1"
    unit: ""
    availability: ""
  - name: md_tfreq
    category: Molecular dynamics
    type: Real
    description: |
      Control the frequency of temperature oscillations during the simulation. If it is too large, the temperature will fluctuate violently; if it is too small, the temperature will take a very long time to equilibrate with the atomic system.

      Note: It is a system-dependent empirical parameter, ranging from 1/(40*md_dt) to 1/(100*md_dt). An improper choice might lead to the failure of jobs.
    default_value: 1/40/md_dt
    unit: ""
    availability: ""
  - name: md_tchain
    category: Molecular dynamics
    type: Integer
    description: |
      Number of thermostats coupled with the particles in the NVT/NPT ensemble based on the Nose-Hoover style non-Hamiltonian equations of motion.
    default_value: "1"
    unit: ""
    availability: ""
  - name: md_pmode
    category: Molecular dynamics
    type: String
    description: |
      Determine the precision level of variable-cell molecular dynamics calculations.
      * 0: FFT grids do not change, only G vectors and K vectors are changed due to the change of lattice vector. This level is suitable for cases where the variation of the volume and shape is not large, and the efficiency is relatively higher.
      * 2: FFT grids change per step. This level is suitable for cases where the variation of the volume and shape is large, such as the MSST method. However, accuracy comes at the cost of efficiency.
    default_value: iso
    unit: ""
    availability: ""
  - name: ref_cell_factor
    category: Molecular dynamics
    type: Real
    description: |
      Construct a reference cell bigger than the initial cell. The reference cell has to be large enough so that the lattice vectors of the fluctuating cell do not exceed the reference lattice vectors during MD. Typically, 1.02 ~ 1.10 is sufficient. However, the cell fluctuations depend on the specific system and thermodynamic conditions. So users must test for a proper choice. This parameters should be used in conjunction with erf_ecut, erf_height, and erf_sigma.
    default_value: "1.0"
    unit: ""
    availability: ""
  - name: md_pcouple
    category: Molecular dynamics
    type: String
    description: |
      The coupled lattice vectors will scale proportionally in NPT ensemble based on the Nose-Hoover style non-Hamiltonian equations of motion.
      * none: Three lattice vectors scale independently.
      * xyz: Lattice vectors x, y, and z scale proportionally.
      * xy: Lattice vectors x and y scale proportionally.
      * xz: Lattice vectors x and z scale proportionally.
      * yz: Lattice vectors y and z scale proportionally.
    default_value: none
    unit: ""
    availability: ""
  - name: md_pfirst
    category: Molecular dynamics
    type: Real
    description: |
      The target pressure used in NPT ensemble simulations, the default value of md_plast is md_pfirst. If md_plast is set to be different from md_pfirst, ABACUS will automatically change the target pressure from md_pfirst to md_plast.
    default_value: "-1.0"
    unit: kbar
    availability: ""
  - name: md_plast
    category: Molecular dynamics
    type: Real
    description: |
      The target pressure used in NPT ensemble simulations, the default value of md_plast is md_pfirst. If md_plast is set to be different from md_pfirst, ABACUS will automatically change the target pressure from md_pfirst to md_plast.
    default_value: "-1.0"
    unit: kbar
    availability: ""
  - name: md_pfreq
    category: Molecular dynamics
    type: Real
    description: |
      The frequency of pressure oscillations during the NPT ensemble simulation. If it is too large, the pressure will fluctuate violently; if it is too small, the pressure will take a very long time to equilibrate with the atomic system.

      Note: It is a system-dependent empirical parameter. An improper choice might lead to the failure of jobs.
    default_value: 1/400/md_dt
    unit: ""
    availability: ""
  - name: md_pchain
    category: Molecular dynamics
    type: Integer
    description: |
      The number of thermostats coupled with the barostat in the NPT ensemble based on the Nose-Hoover style non-Hamiltonian equations of motion.
    default_value: "1"
    unit: ""
    availability: ""
  - name: lj_rule
    category: Molecular dynamics
    type: Integer
    description: |
      The Lennard-Jones potential between two atoms equals: $\sigma_k\sigma(i,j)$
    default_value: "2"
    unit: ""
    availability: ""
  - name: lj_eshift
    category: Molecular dynamics
    type: Boolean
    description: |
      It True, the LJ potential is shifted by a constant such that it is zero at the cut-off distance.
    default_value: "False"
    unit: ""
    availability: ""
  - name: lj_rcut
    category: Molecular dynamics
    type: Real
    description: |
      Cut-off radius for Leonard Jones potential, beyond which the interaction will be neglected. It can be a single value, which means that all pairs of atoms types share the same cut-off radius. Otherwise, it should be a multiple-component vector, containing values, see details in lj_rule.
    default_value: No default
    unit: Angstrom
    availability: ""
  - name: lj_epsilon
    category: Molecular dynamics
    type: Real
    description: |
      The vector representing the matrix for Leonard Jones potential. See details in lj_rule.
    default_value: No default
    unit: eV
    availability: ""
  - name: lj_sigma
    category: Molecular dynamics
    type: Real
    description: |
      The vector representing the matrix for Leonard Jones potential. See details in lj_rule.
    default_value: No default
    unit: Angstrom
    availability: ""
  - name: pot_file
    category: Molecular dynamics
    type: String
    description: |
      The filename of DP/NEP potential files, see md.md in detail.
    default_value: graph.pb
    unit: ""
    availability: ""
  - name: dp_rescaling
    category: Molecular dynamics
    type: Real
    description: |
      Rescaling factor to use a temperature-dependent DP. Energy, stress and force calculated by DP will be multiplied by this factor.
    default_value: "1.0"
    unit: ""
    availability: esolver_type==dp
  - name: dp_fparam
    category: Molecular dynamics
    type: Real
    description: |
      The frame parameter for dp potential. The array size is dim_fparam, then all frames are assumed to be provided with the same fparam.
    default_value: "{}"
    unit: ""
    availability: esolver_type==dp
  - name: dp_aparam
    category: Molecular dynamics
    type: Real
    description: |
      The atomic parameter for dp potential. The array size can be (1) natoms x dim_aparam, then all frames are assumed to be provided with the same aparam; (2) dim_aparam, then all frames and atoms are assumed to be provided with the same aparam.
    default_value: "{}"
    unit: ""
    availability: esolver_type==dp
  - name: msst_direction
    category: Molecular dynamics
    type: Integer
    description: |
      The direction of the shock wave in the MSST method.
      * 0: x direction
      * 1: y direction
      * 2: z direction
    default_value: "2"
    unit: ""
    availability: ""
  - name: msst_vel
    category: Molecular dynamics
    type: Real
    description: |
      The velocity of the shock wave in the MSST method.
    default_value: "0.0"
    unit: Angstrom/fs
    availability: ""
  - name: msst_vis
    category: Molecular dynamics
    type: Real
    description: |
      Artificial viscosity in the MSST method.
    default_value: "0.0"
    unit: "g/(mol*Angstrom*fs)"
    availability: ""
  - name: msst_tscale
    category: Molecular dynamics
    type: Real
    description: |
      The reduction percentage of the initial temperature used to compress volume in the MSST method.
    default_value: "0.01"
    unit: ""
    availability: ""
  - name: msst_qmass
    category: Molecular dynamics
    type: Real
    description: |
      Inertia of the extended system variable. You should set a number larger than 0.
    default_value: No default
    unit: ""
    availability: ""
  - name: md_damp
    category: Molecular dynamics
    type: Real
    description: |
      The damping parameter used to add fictitious force in the Langevin method.
    default_value: "1.0"
    unit: fs
    availability: ""
  - name: md_csvr_tau
    category: Molecular dynamics
    type: Real
    description: |
      The characteristic time scale for the CSVR (Canonical Sampling through Velocity Rescaling) thermostat. Larger values give weaker coupling, smaller values give stronger coupling. Recommended value: 100 * md_dt.
    default_value: "100.0"
    unit: fs
    availability: md_thermostat==csvr
  - name: md_tolerance
    category: Molecular dynamics
    type: Real
    description: |
      The temperature tolerance for velocity rescaling. Velocities are rescaled if the current and target temperature differ more than md_tolerance.
    default_value: "100.0"
    unit: K
    availability: ""
  - name: md_nraise
    category: Molecular dynamics
    type: Integer
    description: |
      * Anderson: The "collision frequency" parameter is given as 1/md_nraise.
      * Berendsen: The "rise time" parameter is given in units of the time step: tau = md_nraise*md_dt, so md_dt/tau = 1/md_nraise.
      * Rescale_v: Every md_nraise steps the current temperature is rescaled to the target temperature.
    default_value: "1"
    unit: ""
    availability: ""
  - name: cal_syns
    category: Molecular dynamics
    type: "Boolean [Integer](optional)"
    description: |
      Whether to calculate and output asynchronous overlap matrix for Hefei-NAMD interface. When enabled, calculates <phi(t-1)|phi(t)> by computing overlap between basis functions at atomic positions from previous time step and current time step. The overlap is calculated by shifting atom positions backward by velocity x md_dt. Output file: OUT.*/syns_nao.csr in CSR format.

      * 0 or false: disable
      * 1 or true: enable with default precision (8 digits)
      * 1 5: enable with custom precision (5 digits)

      [NOTE] Only works with LCAO basis and molecular dynamics calculations. Requires atomic velocities. Output starts from the second MD step (istep > 0).
    default_value: "False"
    unit: ""
    availability: ""
  - name: dmax
    category: Molecular dynamics
    type: Real
    description: |
      The maximum displacement of all atoms in one step. This parameter is useful when cal_syns = True.
    default_value: "0.01"
    unit: bohr
    availability: ""
  - name: of_kinetic
    category: "OFDFT: orbital free density functional theory"
    type: String
    description: |
      Kinetic energy functional type:
      * tf: Thomas-Fermi (TF) functional
      * vw: von Weizsacker (vW) functional
      * tf+: TF + vW functional
      * wt: Wang-Teter (WT) functional
      * ext-wt: Extended Wang-Teter functional
      * xwm: XWM functional
      * lkt: Luo-Karasiev-Trickey (LKT) functional
      * ml: Machine learning KEDF
      * mpn: MPN KEDF (automatically sets ml parameters)
      * cpn5: CPN5 KEDF (automatically sets ml parameters)
    default_value: wt
    unit: ""
    availability: esolver_type==ofdft
  - name: of_method
    category: "OFDFT: orbital free density functional theory"
    type: String
    description: |
      The optimization method used in OFDFT.
      * cg1: Polak-Ribiere. Standard CG algorithm.
      * cg2: Hager-Zhang (generally faster than cg1).
      * tn: Truncated Newton algorithm.
    default_value: tn
    unit: ""
    availability: esolver_type==ofdft
  - name: of_conv
    category: "OFDFT: orbital free density functional theory"
    type: String
    description: |
      Criterion used to check the convergence of OFDFT.
      * energy: Total energy changes less than of_tole.
      * potential: The norm of potential is less than of_tolp.
      * both: Both energy and potential must satisfy the convergence criterion.
    default_value: energy
    unit: ""
    availability: esolver_type==ofdft
  - name: of_tole
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Tolerance of the energy change for determining the convergence.
    default_value: "2e-6"
    unit: Ry
    availability: esolver_type==ofdft
  - name: of_tolp
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Tolerance of potential for determining the convergence.
    default_value: "1e-5"
    unit: Ry
    availability: esolver_type==ofdft
  - name: of_tf_weight
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Weight of TF KEDF (kinetic energy density functional).
    default_value: "1.0"
    unit: ""
    availability: "esolver_type==ofdft and of_kinetic in [tf, tf+, wt, ext-wt, xwm]"
  - name: of_vw_weight
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Weight of vW KEDF (kinetic energy density functional).
    default_value: "1.0"
    unit: ""
    availability: "esolver_type==ofdft and of_kinetic in [vw, tf+, wt, ext-wt, lkt, xwm]"
  - name: of_wt_alpha
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Parameter alpha of WT KEDF (kinetic energy density functional).
    default_value: ""
    unit: ""
    availability: "esolver_type==ofdft and of_kinetic in [wt, ext-wt]"
  - name: of_wt_beta
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Parameter beta of WT KEDF (kinetic energy density functional).
    default_value: ""
    unit: ""
    availability: "esolver_type==ofdft and of_kinetic in [wt, ext-wt]"
  - name: of_extwt_kappa
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Parameter kappa for EXT-WT KEDF.
    default_value: "1.0 / (2.0 * std::pow(4./3., 1./3.) - 1.0)"
    unit: ""
    availability: esolver_type==ofdft and of_kinetic==ext-wt
  - name: of_wt_rho0
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      The average density of system.
    default_value: "0.0"
    unit: Bohr^-3
    availability: esolver_type==ofdft and of_kinetic==wt
  - name: of_hold_rho0
    category: "OFDFT: orbital free density functional theory"
    type: Boolean
    description: |
      Whether to fix the average density rho0.
      * True: rho0 will be fixed even if the volume of system has changed, it will be set to True automatically if of_wt_rho0 is not zero.
      * False: rho0 will change if volume of system has changed.
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft and of_kinetic==wt
  - name: of_lkt_a
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Parameter a of LKT KEDF (kinetic energy density functional).
    default_value: "1.3"
    unit: ""
    availability: esolver_type==ofdft and of_kinetic==lkt
  - name: of_xwm_rho_ref
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Reference charge density for XWM kinetic energy functional. If set to 0, the program will use average charge density.
    default_value: "0.0"
    unit: ""
    availability: esolver_type==ofdft and of_kinetic==xwm
  - name: of_xwm_kappa
    category: "OFDFT: orbital free density functional theory"
    type: Real
    description: |
      Parameter for XWM kinetic energy functional. See PHYSICAL REVIEW B 100, 205132 (2019) for optimal values.
    default_value: "0.0"
    unit: ""
    availability: esolver_type==ofdft and of_kinetic==xwm
  - name: of_read_kernel
    category: "OFDFT: orbital free density functional theory"
    type: Boolean
    description: |
      Whether to read in the kernel file.
      * True: The kernel of WT KEDF (kinetic energy density functional) will be filled from the file specified by of_kernel_file.
      * False: The kernel of WT KEDF (kinetic energy density functional) will be filled from formula.
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft and of_kinetic==wt
  - name: of_kernel_file
    category: "OFDFT: orbital free density functional theory"
    type: String
    description: |
      The name of WT kernel file.
    default_value: WTkernel.txt
    unit: ""
    availability: esolver_type==ofdft and of_kinetic==wt and of_read_kernel==true
  - name: of_full_pw
    category: "OFDFT: orbital free density functional theory"
    type: Boolean
    description: |
      Whether to use full planewaves.
      * True: Ecut will be ignored while collecting planewaves, so that all planewaves will be used in FFT.
      * False: Only use the planewaves inside ecut, the same as KSDFT.
    default_value: "True"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_full_pw_dim
    category: "OFDFT: orbital free density functional theory"
    type: Integer
    description: |
      Specify the parity of FFT dimensions.
      * 0: either odd or even.
      * 1: odd only.
      * 2: even only.

      Note: Even dimensions may cause slight errors in FFT. It should be ignorable in ofdft calculation, but it may make Cardinal B-spline interpolation unstable, so please set of_full_pw_dim = 1 if nbspline != -1.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft and of_full_pw==true
  - name: of_ml_gene_data
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      Controls the generation of machine learning training data. When enabled, training data in .npy format will be saved in the directory OUT.${suffix}/.
    default_value: "False"
    unit: ""
    availability: esolver_type==ksdft and basis_type==pw
  - name: of_ml_device
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: String
    description: |
      Run Neural Network on GPU or CPU.
      * cpu: CPU
      * gpu: GPU
    default_value: cpu
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_feg
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Integer
    description: |
      The method to incorporate the Free Electron Gas (FEG) limit.
      * 0: Do not incorporate the FEG limit.
      * 1: Incorporate the FEG limit by translation.
      * 3: Incorporate the FEG limit by nonlinear transformation using softplus function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_nkernel
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Integer
    description: |
      Number of kernel functions.
    default_value: "1"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_kernel
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element specifies the type of the i-th kernel function.
      * 1: Wang-Teter kernel function.
      * 2: Modified Yukawa function, and alpha is specified by of_ml_yukawa_alpha.
      * 3: Truncated kinetic kernel (TKK), the file containing TKK is specified by of_ml_kernel_file.
    default_value: "1"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_kernel_scaling
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Real
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element specifies the RECIPROCAL of scaling parameter of the i-th kernel function.
    default_value: "1.0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_yukawa_alpha
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Real
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element specifies the parameter alpha of i-th kernel function. ONLY used for Yukawa kernel function.
    default_value: "1.0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_kernel_file
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of String
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element specifies the file containing the i-th kernel function. ONLY used for TKK.
    default_value: none
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_gamma
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      Local descriptor: gamma = (rho / rho0)^(1/3).
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_p
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      Semi-local descriptor: p = |nabla rho|^2 / [2 (3 pi^2)^(1/3) rho^(4/3)]^2.
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_q
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      Semi-local descriptor: q = nabla^2 rho / [4 (3 pi^2)^(2/3) rho^(5/3)].
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanhp
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      Semi-local descriptor: tanhp = tanh(chi_p * p).
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanhq
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      Semi-local descriptor: tanhq = tanh(chi_q * q).
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_chi_p
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Real
    description: |
      Hyperparameter chi_p: tanhp = tanh(chi_p * p).
    default_value: "1.0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_chi_q
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Real
    description: |
      Hyperparameter chi_q: tanhq = tanh(chi_q * q).
    default_value: "1.0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_gammanl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor gammanl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_pnl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor pnl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_qnl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor qnl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_xi
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor xi defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanhxi
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor tanhxi defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanhxi_nl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor tanhxi_nl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanh_pnl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor tanh_pnl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanh_qnl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor tanh_qnl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanhp_nl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor tanhp_nl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_tanhq_nl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Integer
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element controls the non-local descriptor tanhq_nl defined by the i-th kernel function.
    default_value: "0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_chi_xi
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Real
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element specifies the hyperparameter chi_xi of non-local descriptor tanhxi defined by the i-th kernel function.
    default_value: "1.0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_chi_pnl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Real
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element specifies the hyperparameter chi_pnl of non-local descriptor tanh_pnl defined by the i-th kernel function.
    default_value: "1.0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_chi_qnl
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Vector of Real
    description: |
      Containing nkernel (see of_ml_nkernel) elements. The i-th element specifies the hyperparameter chi_qnl of non-local descriptor tanh_qnl defined by the i-th kernel function.
    default_value: "1.0"
    unit: ""
    availability: esolver_type==ofdft
  - name: of_ml_local_test
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      FOR TEST. Read in the density, and output the F and Pauli potential.
    default_value: "False"
    unit: ""
    availability: esolver_type==ofdft
  - name: ml_exx
    category: "ML-KEDF: machine learning based kinetic energy density functional for OFDFT"
    type: Boolean
    description: |
      Whether to use machine learning based exact exchange (ML-EXX).
    default_value: "False"
    unit: ""
    availability: ""
  - name: method_sto
    category: Electronic structure (SDFT)
    type: Integer
    description: |
      Different methods to do stochastic DFT
      * 1: Calculate twice, this method cost less memory but is slower.
      * 2: Calculate once but needs much more memory. This method is much faster. Besides, it calculates with a smaller nche_sto. However, when the memory is not enough, only method 1 can be used.
      * other: use 2
    default_value: "2"
    unit: ""
    availability: esolver_type==sdft
  - name: nbands_sto
    category: Electronic structure (SDFT)
    type: Integer or string
    description: |
      The number of stochastic orbitals
      * 1-1000000: Perform stochastic DFT. Increasing the number of bands improves accuracy and reduces stochastic errors; To perform mixed stochastic-deterministic DFT, you should set nbands, which represents the number of KS orbitals.
      * 0: Invalid. Use all for the complete-basis SDFT mode.
      * all: All complete basis sets are used to replace stochastic orbitals with the Chebyshev method (CT), resulting in the same results as KSDFT without stochastic errors.
    default_value: "256"
    unit: ""
    availability: esolver_type==sdft
  - name: nche_sto
    category: Electronic structure (SDFT)
    type: Integer
    description: |
      Chebyshev expansion orders for stochastic DFT.
    default_value: "100"
    unit: ""
    availability: esolver_type==sdft
  - name: emin_sto
    category: Electronic structure (SDFT)
    type: Real
    description: |
      Trial energy to guess the lower bound of eigen energies of the Hamiltonian Operator.
    default_value: "0.0"
    unit: Ry
    availability: esolver_type==sdft
  - name: emax_sto
    category: Electronic structure (SDFT)
    type: Real
    description: |
      Trial energy to guess the upper bound of eigen energies of the Hamiltonian Operator.
    default_value: "0.0"
    unit: Ry
    availability: esolver_type==sdft
  - name: seed_sto
    category: Electronic structure (SDFT)
    type: Integer
    description: |
      The random seed to generate stochastic orbitals.
      * >= 0: Stochastic orbitals have the form of exp(i*theta), where theta is a uniform distribution in [0, 2*pi).
      * 0: the seed is decided by time(NULL).
      * <= -1: Stochastic orbitals have the form of +1 or -1 with equal probability.
      * -1: the seed is decided by time(NULL).
    default_value: "0"
    unit: ""
    availability: esolver_type==sdft
  - name: initsto_ecut
    category: Electronic structure (SDFT)
    type: Real
    description: |
      Stochastic wave functions are initialized in a large box generated by "4*initsto_ecut". initsto_ecut should be larger than ecutwfc. In this method, SDFT results are the same when using different cores. Besides, coefficients of the same G are the same when ecutwfc is rising to initsto_ecut. If it is smaller than ecutwfc, it will be turned off.
    default_value: "0.0"
    unit: Ry
    availability: esolver_type==sdft
  - name: initsto_freq
    category: Electronic structure (SDFT)
    type: Integer
    description: |
      Frequency (once each initsto_freq steps) to generate new stochastic orbitals when running md.
      * positive integer: Update stochastic orbitals
      * 0: Never change stochastic orbitals.
    default_value: "0"
    unit: ""
    availability: esolver_type==sdft
  - name: npart_sto
    category: Electronic structure (SDFT)
    type: Integer
    description: |
      Make memory cost to 1/npart_sto times of the previous one when running the post process of SDFT like DOS or conductivities.
    default_value: "1"
    unit: ""
    availability: esolver_type==sdft and ((method_sto==2 and out_dos==1) or (basis_type==pw and cal_cond==true))
  - name: deepks_out_labels
    category: DeePKS
    type: Integer
    description: |
      Print labels and descriptors for DeePKS in OUT.${suffix}. The names of these files start with "deepks".
      * 0 : No output.
      * 1 : Output intermediate files needed during DeePKS training.
      * 2 : Output target labels for label preperation. The label files are named as deepks_<property>.npy or deepks_<property>.csr, where the units and formats are the same as label files <property>.npy or <property>.csr required for training, except that the first dimension (nframes) is excluded. System structrue files are also given in deepks_atom.npy and deepks_box.npy in the unit of Bohr, which means lattice_constant should be set to 1 when training.

      [NOTE] When deepks_out_labels equals 1, the path of a numerical descriptor (an orb file) is needed to be specified under the NUMERICAL_DESCRIPTOR tag in the STRU file. This is not needed when deepks_out_labels equals 2.
    default_value: "0"
    unit: ""
    availability: basis_type==lcao
  - name: deepks_out_freq_elec
    category: DeePKS
    type: Integer
    description: |
      When deepks_out_freq_elec is greater than 0, print labels and descriptors for DeePKS in OUT.${suffix}/DeePKS_Labels_Elec per deepks_out_freq_elec electronic iterations, with suffix _e* to distinguish different steps. Often used with deepks_out_labels equals 1.
    default_value: "0"
    unit: ""
    availability: basis_type==lcao
  - name: deepks_out_base
    category: DeePKS
    type: String
    description: |
      Print labels and descriptors calculated by base functional ( determined by deepks_out_base ) and target functional ( determined by dft_functional ) for DeePKS in per deepks_out_freq_elec electronic iterations. The SCF process, labels and descriptors output of the target functional are all consistent with those when the target functional is used alone. The only additional output under this configuration is the labels of the base functional. Often used with deepks_out_labels equals 1.
    default_value: None
    unit: ""
    availability: "basis_type==lcao and deepks_out_freq_elec>0"
  - name: deepks_scf
    category: DeePKS
    type: Boolean
    description: |
      perform self-consistent field iteration in DeePKS method

      [NOTE] A trained, traced model file is needed.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: deepks_equiv
    category: DeePKS
    type: Boolean
    description: |
      whether to use equivariant version of DeePKS

      [NOTE] The equivariant version of DeePKS-kit is still under development, so this feature is currently only intended for internal usage.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: deepks_model
    category: DeePKS
    type: String
    description: |
      the path of the trained, traced neural network model file generated by deepks-kit
    default_value: None
    unit: ""
    availability: basis_type==lcao and deepks_scf==true
  - name: bessel_descriptor_lmax
    category: DeePKS
    type: Integer
    description: |
      the maximum angular momentum of the Bessel functions generated as the projectors in DeePKS - NOte: To generate such projectors, set calculation type to gen_bessel in ABACUS. See also calculation.
    default_value: "2"
    unit: ""
    availability: calculation==gen_bessel
  - name: bessel_descriptor_ecut
    category: DeePKS
    type: String
    description: |
      energy cutoff of Bessel functions
    default_value: same as ecutwfc
    unit: Ry
    availability: calculation==gen_bessel
  - name: bessel_descriptor_tolerence
    category: DeePKS
    type: Real
    description: |
      tolerance for searching the zeros of Bessel functions
    default_value: "1.0e-12"
    unit: ""
    availability: calculation==gen_bessel
  - name: bessel_descriptor_rcut
    category: DeePKS
    type: Real
    description: |
      cutoff radius of Bessel functions
    default_value: "6.0"
    unit: Bohr
    availability: calculation==gen_bessel
  - name: bessel_descriptor_smooth
    category: DeePKS
    type: Boolean
    description: |
      smooth the Bessel functions at radius cutoff
    default_value: "False"
    unit: ""
    availability: calculation==gen_bessel
  - name: bessel_descriptor_sigma
    category: DeePKS
    type: Real
    description: |
      smooth parameter at the cutoff radius of projectors
    default_value: "0.1"
    unit: Bohr
    availability: calculation==gen_bessel
  - name: deepks_bandgap
    category: DeePKS
    type: Integer
    description: |
      include bandgap label for DeePKS training
      * 0: Don't include bandgap label
      * 1: Include target bandgap label (see deepks_band_range for more details)
      * 2: Include multiple bandgap label (see deepks_band_range for more details)
      * 3: Used for systems containing H atoms. Here HOMO is defined as the max occupation except H atoms and the bandgap label is the energy between HOMO and (HOMO + 1)
    default_value: "0"
    unit: ""
    availability: basis_type==lcao and deepks_scf==true
  - name: deepks_band_range
    category: DeePKS
    type: "Integer*2"
    description: |
      The first value should not be larger than the second one and the meaning differs in different cases below
      * deepks_bandgap is 1: Bandgap label is the energy between LUMO + deepks_band_range[0] and LUMO + deepks_band_range[1]. If not set, it will calculate energy between HOMO and LUMO states.
      * deepks_bandgap is 2: Bandgap labels are energies between HOMO and all states in range [LUMO + deepks_band_range[0], LUMO + deepks_band_range[1]] (Thus there are deepks_band_range[1] - deepks_band_range[0] + 1 bandgaps in total). If HOMO is included in the setting range, it will be ignored since it will always be zero and has no valuable messages (deepks_band_range[1] - deepks_band_range[0] bandgaps in this case). NOTICE: The set range can be greater than, less than, or include the value of HOMO. In the bandgap label, we always calculate the energy of the state in the set range minus the energy of HOMO state, so the bandgap can be negative if the state is lower than HOMO.
    default_value: "-1 0"
    unit: ""
    availability: "basis_type==lcao and deepks_scf==true and deepks_bandgap in [1, 2]"
  - name: deepks_v_delta
    category: DeePKS
    type: Integer
    description: |
      Include V_delta/V_delta_R (Hamiltonian in k/real space) label for DeePKS training. When deepks_out_labels is true and deepks_v_delta > 0 (k space), ABACUS will output deepks_hbase.npy, deepks_vdelta.npy and deepks_htot.npy(htot=hbase+vdelta). When deepks_out_labels is true and deepks_v_delta < 0 (real space), ABACUS will output deepks_hrtot.csr, deepks_hrdelta.csr. Some more files output for different settings. NOTICE: To match the unit Normally used in DeePKS, the unit of Hamiltonian in k space is Hartree. However, currently in R space the unit is still Ry.
      * deepks_v_delta = 1: deepks_vdpre.npy, which is used to calculate V_delta during DeePKS training.
      * deepks_v_delta = 2: deepks_phialpha.npy and deepks_gevdm.npy, which can be used to calculate deepks_vdpre.npy. A recommanded method for memory saving.
      * deepks_v_delta = -1: deepks_vdrpre.npy, which is used to calculate V_delta_R during DeePKS training.
      * deepks_v_delta = -2: deepks_phialpha_r.npy and deepks_gevdm.npy, which can be used to calculate deepks_vdrpre.npy. A recommanded method for memory saving.
    default_value: "0"
    unit: ""
    availability: basis_type==lcao
  - name: deepks_out_unittest
    category: DeePKS
    type: Boolean
    description: |
      generate files for constructing DeePKS unit test

      [NOTE] Not relevant when running actual calculations. When set to 1, ABACUS needs to be run with only 1 process.
    default_value: "False"
    unit: ""
    availability: ""
  - name: estep_per_md
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Integer
    description: |
      The number of electronic propagation steps between two ionic steps.
    default_value: "1"
    unit: ""
    availability: ""
  - name: td_dt
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Real
    description: |
      The time step used for electronic propagation. If td_dt is not specified, it is set to md_dt / estep_per_md. If td_dt is specified explicitly, md_dt is reset to td_dt * estep_per_md.
    default_value: md_dt / estep_per_md
    unit: fs
    availability: ""
  - name: td_edm
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Integer
    description: |
      Method used to calculate the energy-density matrix for the overlap contribution to forces in LCAO RT-TDDFT.
      * 0: Use $\mathrm{EDM}_{\boldsymbol{k}}=\frac{1}{2}\left(S_{\boldsymbol{k}}^{-1}H_{\boldsymbol{k}}\rho_{\boldsymbol{k}}+\rho_{\boldsymbol{k}}H_{\boldsymbol{k}}S_{\boldsymbol{k}}^{-1}\right)$.
      * 1: Use the ground-state eigenvalue-weighted expression $\mathrm{EDM}_{\mu\nu,\boldsymbol{k}}=\sum_i w_{i\boldsymbol{k}}\epsilon_{i\boldsymbol{k}}C_{\mu i,\boldsymbol{k}}C_{\nu i,\boldsymbol{k}}^*$. This expression is deprecated for RT-TDDFT and is generally not valid when the propagated wave functions are not Hamiltonian eigenstates.
    default_value: "0"
    unit: ""
    availability: ""
  - name: td_print_eij
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Real
    description: |
      Controls output of the propagated-state Hamiltonian matrix elements $E_{ij}=\Braket{\psi_i | \hat{H} | \psi_j}$ to the running log. The printed band indices $i$ and $j$ are one-based global indices. Both the threshold and the printed matrix elements are in Ry.
      * $\lt 0$: Disable the output.
      * $\geqslant 0$: Print an element when either $\left|\operatorname{Re}E_{ij}\right|$ or $\left|\operatorname{Im}E_{ij}\right|$ is greater than or equal to td_print_eij.
    default_value: "-1"
    unit: Ry
    availability: ""
  - name: td_propagator
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Integer
    description: |
      Method used to propagate the electronic states in a nonorthogonal LCAO basis. The formulas below use Hartree atomic units, with $S$, $H$, and $\Delta t=\mathtt{td\_dt}$ evaluated as required by each approximation.
      * 0: Crank-Nicolson through an explicitly constructed evolution matrix, $U=\left[S+\mathrm{i}H\Delta t/2\right]^{-1}\left[S-\mathrm{i}H\Delta t/2\right]$.
      * 1: Fourth-order Taylor approximation to the exponential. With $\mathcal{A}=-\mathrm{i}S^{-1}H\Delta t$, $U=I+\mathcal{A}+\mathcal{A}^2/2+\mathcal{A}^3/6+\mathcal{A}^4/24$.
      * 2: Enforced time-reversal symmetry (ETRS), $U(t+\Delta t,t)=\exp\left[-\mathrm{i}S^{-1}H(t+\Delta t)\Delta t/2\right]\exp\left[-\mathrm{i}S^{-1}H(t)\Delta t/2\right]$. In the implementation, each exponential is replaced by the fourth-order Taylor polynomial from method 1 evaluated with a half time step.
      * 3: Crank-Nicolson by directly solving $\left[S+\mathrm{i}H\Delta t/2\right]\psi(t+\Delta t)=\left[S-\mathrm{i}H\Delta t/2\right]\psi(t)$.

      [NOTE] GPU execution currently supports only method 0 in both single-GPU and multi-GPU solver configurations. CPU execution supports methods 0 through 3.
    default_value: "0"
    unit: ""
    availability: ""
  - name: td_vext
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Boolean
    description: |
      Controls whether a time-dependent external electric field is applied.
      * True: Add a laser-material interaction (external electric field).
      * False: No external electric field.
    default_value: "False"
    unit: ""
    availability: ""
  - name: td_vext_dire
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Integer
    description: |
      Specifies one absolute Cartesian direction for each external electric field when td_vext is enabled. Unlike the ground-state efield_dir parameter, these directions are not defined by lattice or reciprocal-lattice vectors. The number of values must equal that of td_ttype, and repeated directions are allowed; fields assigned to the same direction are added. For example, td_vext_dire 1 2 applies one field along Cartesian x and one along Cartesian y.
      * 1: The external field direction is along the x-axis.
      * 2: The external field direction is along the y-axis.
      * 3: The external field direction is along the z-axis.
    default_value: "1"
    unit: ""
    availability: ""
  - name: td_stype
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Integer
    description: |
      Type of electric field in the space domain, i.e. the gauge of the electric field.
      * 0: Length gauge.
      * 1: Velocity gauge.
      * 2: Hybrid gauge. See J. Chem. Theory Comput. 2025, 21, 3335-3341 for more information.
    default_value: "0"
    unit: ""
    availability: ""
  - name: td_ttype
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Integer
    description: |
      Specifies one time-domain type for each external electric field. Its number of values must equal that of td_vext_dire. Parameters belonging to each type must provide exactly one value for every occurrence of that type, in occurrence order; fields with a repeated direction are added.

      The formulas below use Hartree atomic units. For every ordinary input frequency $f$, $\omega=2\pi f$; $\Delta t=\mathtt{td\_dt}$; and $E_0$ denotes the corresponding amplitude parameter. A step-valued parameter $n_q$ represents the physical time $t_q=n_q\Delta t$.
      * 0: Gaussian pulse, $E(t)=E_0\cos\left[\omega(t-t_0)+\varphi\right]\mathrm{e}^{-(t-t_0)^2/(2\sigma^2)}$, where $t_0=\mathtt{td\_gauss\_t0}\Delta t$.
      * 1: Trapezoid pulse, $E(t)=E_0g(t)\cos(\omega t+\varphi)$. With $t_1=\mathtt{td\_trape\_t1}\Delta t$, $t_2=\mathtt{td\_trape\_t2}\Delta t$, and $t_3=\mathtt{td\_trape\_t3}\Delta t$, the envelope is $g(t)=t/t_1$ for $0\leqslant t\lt t_1$, $g(t)=1$ for $t_1\leqslant t\lt t_2$, $g(t)=(t_3-t)/(t_3-t_2)$ for $t_2\leqslant t\lt t_3$, and $g(t)=0$ otherwise.
      * 2: Trigonometric pulse, $E(t)=E_0\cos(\omega_1t+\varphi_1)\sin^2(\omega_2t+\varphi_2)$.
      * 3: Heaviside pulse defined on electronic steps. With $n_0=\mathtt{td\_heavi\_t0}$, $E(n)=E_0$ for $n\lt n_0$ and $E(n)=0$ for $n\geqslant n_0$.
      * 4: Finite-support supersine pulse. For $t_{\mathrm{s}}\lt t\lt t_{\mathrm{e}}$, the envelope is $f(t)=\left\{\sin\left[\pi\frac{t-t_{\mathrm{s}}}{t_{\mathrm{e}}-t_{\mathrm{s}}}\right]\right\}^{\frac{\pi}{\sigma}\left|\frac{t-t_{\mathrm{s}}}{t_{\mathrm{e}}-t_{\mathrm{s}}}-\frac{1}{2}\right|}$ and the electric field is $E(t)=E_0\left\{f(t)\cos\left[\omega\left(t-\frac{t_{\mathrm{s}}+t_{\mathrm{e}}}{2}\right)+\varphi\right]+\frac{\dot{f}(t)}{\omega}\sin\left[\omega\left(t-\frac{t_{\mathrm{s}}+t_{\mathrm{e}}}{2}\right)+\varphi\right]\right\}$. The corresponding analytic vector potential is $\boldsymbol{A}(t)=-\frac{E_0}{\omega}f(t)\sin\left[\omega\left(t-\frac{t_{\mathrm{s}}+t_{\mathrm{e}}}{2}\right)+\varphi\right]\hat{\boldsymbol{e}}$, with $\boldsymbol{E}(t)=-\partial\boldsymbol{A}(t)/\partial t$. The envelope, electric field, and vector potential are zero at the pulse boundaries and outside the interval.

      In the velocity and hybrid gauges, ABACUS obtains the vector potential actually used in propagation by Simpson integration of the selected electric fields, including the supersine field, so a residual at the numerical-quadrature accuracy scale may remain.
    default_value: "0"
    unit: ""
    availability: ""
  - name: td_tstart
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Integer
    description: |
      First electronic step at which the time-dependent electric field is active. The interval from td_tstart through td_tend includes both endpoints. On each active step $n$, the velocity and hybrid gauges integrate the field over $[n\Delta t,(n+1)\Delta t]$, where $\Delta t=\mathtt{td\_dt}$.
    default_value: "1"
    unit: ""
    availability: ""
  - name: td_tend
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Integer
    description: |
      Last electronic step at which the time-dependent electric field is active. The interval from td_tstart through td_tend includes both endpoints. On each active step $n$, the velocity and hybrid gauges integrate the field over $[n\Delta t,(n+1)\Delta t]$, where $\Delta t=\mathtt{td\_dt}$.
    default_value: "1000"
    unit: ""
    availability: ""
  - name: td_lcut1
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Real
    description: |
      Lower fractional-coordinate cutoff for the periodic spatial modulation used in the length gauge. Let $c_1=\mathtt{td\_lcut1}$, $c_2=\mathtt{td\_lcut2}$, $D=c_2-c_1$, and $G=c_1+1-c_2$. For a fractional coordinate $x$, the field factor is $\eta(x)=1$ when $c_1\leqslant x\lt c_2$ and $\eta(x)=-D/G$ elsewhere. The reversed outer interval makes the potential periodic and continuous and gives the field zero cell average.
    default_value: "0.05"
    unit: ""
    availability: ""
  - name: td_lcut2
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Real
    description: |
      Upper fractional-coordinate cutoff for the periodic spatial modulation used in the length gauge. Let $c_1=\mathtt{td\_lcut1}$, $c_2=\mathtt{td\_lcut2}$, $D=c_2-c_1$, and $G=c_1+1-c_2$. For a fractional coordinate $x$, the field factor is $\eta(x)=1$ when $c_1\leqslant x\lt c_2$ and $\eta(x)=-D/G$ elsewhere. The reversed outer interval makes the potential periodic and continuous and gives the field zero cell average.
    default_value: "0.95"
    unit: ""
    availability: ""
  - name: td_gauss_freq
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Ordinary frequency $f$ in the Gaussian-pulse formula, with $\omega=2\pi f$. Supply exactly one value for each td_ttype 0 occurrence, in occurrence order.
    default_value: "22.13"
    unit: 1/fs
    availability: td_ttype contains 0
  - name: td_gauss_phase
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Carrier phase $\varphi$ in the Gaussian-pulse formula. Supply exactly one value for each td_ttype 0 occurrence, in occurrence order.
    default_value: "0.0"
    unit: rad
    availability: td_ttype contains 0
  - name: td_gauss_sigma
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Nonzero standard deviation $\sigma$ of the Gaussian envelope. Supply exactly one value for each td_ttype 0 occurrence, in occurrence order.
    default_value: "30.0"
    unit: fs
    availability: td_ttype contains 0
  - name: td_gauss_t0
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electronic-step position of the Gaussian center, which defines $t_0=\mathtt{td\_gauss\_t0}\Delta t$. Supply exactly one value for each td_ttype 0 occurrence, in occurrence order.
    default_value: "100"
    unit: ""
    availability: td_ttype contains 0
  - name: td_gauss_amp
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electric-field scale $E_0$ in the Gaussian-pulse formula. Supply exactly one value for each td_ttype 0 occurrence, in occurrence order.
    default_value: "0.25"
    unit: V/Angstrom
    availability: td_ttype contains 0
  - name: td_trape_freq
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Ordinary carrier frequency $f$ in the trapezoid-pulse formula, with $\omega=2\pi f$. Supply exactly one value for each td_ttype 1 occurrence, in occurrence order.
    default_value: "1.60"
    unit: 1/fs
    availability: td_ttype contains 1
  - name: td_trape_phase
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Carrier phase $\varphi$ in the trapezoid-pulse formula. Supply exactly one value for each td_ttype 1 occurrence, in occurrence order.
    default_value: "0.0"
    unit: rad
    availability: td_ttype contains 1
  - name: td_trape_t1
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electronic step defining the end of the linear rise, $t_1=\mathtt{td\_trape\_t1}\Delta t$. Each field must satisfy td_trape_t1 <= td_trape_t2 <= td_trape_t3. Supply exactly one value for each td_ttype 1 occurrence, in occurrence order.
    default_value: "1875"
    unit: ""
    availability: td_ttype contains 1
  - name: td_trape_t2
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electronic step defining the end of the plateau, $t_2=\mathtt{td\_trape\_t2}\Delta t$. Each field must satisfy td_trape_t1 <= td_trape_t2 <= td_trape_t3. Supply exactly one value for each td_ttype 1 occurrence, in occurrence order.
    default_value: "5625"
    unit: ""
    availability: td_ttype contains 1
  - name: td_trape_t3
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electronic step defining the end of the linear fall, $t_3=\mathtt{td\_trape\_t3}\Delta t$. Each field must satisfy td_trape_t1 <= td_trape_t2 <= td_trape_t3. Supply exactly one value for each td_ttype 1 occurrence, in occurrence order.
    default_value: "7500"
    unit: ""
    availability: td_ttype contains 1
  - name: td_trape_amp
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electric-field scale $E_0$ in the trapezoid-pulse formula. Supply exactly one value for each td_ttype 1 occurrence, in occurrence order.
    default_value: "2.74"
    unit: V/Angstrom
    availability: td_ttype contains 1
  - name: td_trigo_freq1
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      First ordinary frequency $f_1$ in the trigonometric-pulse formula, with $\omega_1=2\pi f_1$. Supply exactly one value for each td_ttype 2 occurrence, in occurrence order.
    default_value: "1.164656"
    unit: 1/fs
    availability: td_ttype contains 2
  - name: td_trigo_freq2
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Second ordinary frequency $f_2$ in the trigonometric-pulse formula, with $\omega_2=2\pi f_2$. Supply exactly one value for each td_ttype 2 occurrence, in occurrence order.
    default_value: "0.029116"
    unit: 1/fs
    availability: td_ttype contains 2
  - name: td_trigo_phase1
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Carrier phase $\varphi_1$ in the cosine factor of the trigonometric-pulse formula. Supply exactly one value for each td_ttype 2 occurrence, in occurrence order.
    default_value: "0.0"
    unit: rad
    availability: td_ttype contains 2
  - name: td_trigo_phase2
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Envelope phase $\varphi_2$ in the sine-squared factor of the trigonometric-pulse formula. Supply exactly one value for each td_ttype 2 occurrence, in occurrence order.
    default_value: "0.0"
    unit: rad
    availability: td_ttype contains 2
  - name: td_trigo_amp
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electric-field scale $E_0$ in the trigonometric-pulse formula. Supply exactly one value for each td_ttype 2 occurrence, in occurrence order.
    default_value: "2.74"
    unit: V/Angstrom
    availability: td_ttype contains 2
  - name: td_heavi_t0
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electronic switch step $n_0$ in the Heaviside-pulse definition. The field is $E_0$ for $n\lt n_0$ and zero for $n\geqslant n_0$. Supply exactly one value for each td_ttype 3 occurrence, in occurrence order.
    default_value: "100"
    unit: ""
    availability: td_ttype contains 3
  - name: td_heavi_amp
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electric-field scale $E_0$ in the Heaviside-pulse definition. Supply exactly one value for each td_ttype 3 occurrence, in occurrence order.
    default_value: "1.0"
    unit: V/Angstrom
    availability: td_ttype contains 3
  - name: td_supsine_amp
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Carrier electric-field scale $E_0$ of each supersine pulse. This is not a normalization of the complete waveform maximum, because the envelope-derivative term also contributes. Supply exactly one value for each td_ttype 4 occurrence, in occurrence order.
    default_value: "0.27"
    unit: V/Angstrom
    availability: td_ttype contains 4
  - name: td_supsine_freq
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Nonzero ordinary carrier frequency $f$ of each supersine pulse, with $\omega=2\pi f$. Supply exactly one value for each td_ttype 4 occurrence, in occurrence order.
    default_value: "0.18737028625"
    unit: 1/fs
    availability: td_ttype contains 4
  - name: td_supsine_phase
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Electric-field carrier phase $\varphi$ at the center of each supersine envelope. A value of 0 places a cosine carrier maximum at the envelope center. Supply exactly one value for each td_ttype 4 occurrence, in occurrence order.
    default_value: "0.0"
    unit: rad
    availability: td_ttype contains 4
  - name: td_supsine_sigma
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of Real
    description: |
      Dimensionless shape parameter $\sigma$ of each supersine envelope. It must satisfy $0\lt\sigma\lt\pi/2$ so that the electric field approaches zero at the pulse boundaries. Supply exactly one value for each td_ttype 4 occurrence, in occurrence order.
    default_value: "0.75"
    unit: ""
    availability: td_ttype contains 4
  - name: td_supsine_tstart
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of String
    description: |
      Integer electronic step at the left, exactly zero boundary of each supersine pulse, defining $t_{\mathrm{s}}=\mathtt{td\_supsine\_tstart}\Delta t$. Supply exactly one integer or default token for each td_ttype 4 occurrence, in occurrence order; each default token inherits td_tstart. The complete pulse support must lie inside the inclusive global td_tstart to td_tend interval; hard truncation of a supersine pulse is rejected.
    default_value: default
    unit: ""
    availability: td_ttype contains 4
  - name: td_supsine_tend
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Vector of String
    description: |
      Integer electronic step at the right, exactly zero boundary of each supersine pulse, defining $t_{\mathrm{e}}=\mathtt{td\_supsine\_tend}\Delta t$. Supply exactly one integer or default token for each td_ttype 4 occurrence, in occurrence order; each default token inherits td_tend. The complete pulse support must lie inside the inclusive global td_tstart to td_tend interval; hard truncation of a supersine pulse is rejected.
    default_value: default
    unit: ""
    availability: td_ttype contains 4
  - name: init_vecpot_file
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Boolean
    description: |
      Selects the source of the Cartesian vector potential used by LCAO RT-TDDFT.
      * True: Read vector_pot.txt from the calculation working directory. Each non-comment line must contain four columns: a conventionally one-based electronic-step label followed by $A_x$, $A_y$, and $A_z$ in atomic units. Rows are consumed sequentially; the first column is read as a label and is not used for lookup. If propagation continues beyond the available rows, the last row is reused.
      * False: Obtain the vector potential by integrating the configured electric field.
    default_value: "False"
    unit: ""
    availability: ""
  - name: ocp
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Boolean
    description: |
      Controls fixed band occupations. In calculations other than LCAO RT-TDDFT, fixed values are applied during electronic-state setup. In LCAO RT-TDDFT, the initial ground-state SCF determines occupations normally, and fixed values from ocp_set are applied during the subsequent real-time propagation steps.
      * True: Use the fixed occupations specified by ocp_set during propagation.
      * False: Keep the occupations determined by the initial SCF.
    default_value: "False"
    unit: ""
    availability: ""
  - name: ocp_set
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: String
    description: |
      Fixed occupation weights used when ocp is true. Values are assigned band by band for each k-point, following k-point order. In LCAO RT-TDDFT, the initial ground-state SCF uses its normally determined occupations, and this array is applied only during subsequent real-time propagation steps. The repetition syntax N*x expands to N copies of x.
      * Example: 1 10*1 0 1 expands to 13 values, with the 12th value equal to 0 and all other values equal to 1.
      * After expansion, the array length must equal nks * nbands.
      * The sum of all weights must equal nelec; otherwise the calculation terminates with an error.
    default_value: None
    unit: ""
    availability: ""
  - name: of_cd
    category: "TDOFDFT: time dependent orbital free density functional theory"
    type: Boolean
    description: |
      Added the current dependent(CD) potential. (https://doi.org/10.1103/PhysRevB.98.144302)
      * True: Added the CD potential.
      * False: Not added the CD potential.
    default_value: "False"
    unit: ""
    availability: esolver_type==tdofdft
  - name: of_mcd_alpha
    category: "TDOFDFT: time dependent orbital free density functional theory"
    type: Real
    description: |
      The value of the parameter alpha in modified CD potential method. mCDPotential=alpha*CDPotential (proposed in paper PhysRevB.98.144302)
    default_value: "1.0"
    unit: ""
    availability: esolver_type==tdofdft
  - name: xc_kernel
    category: Linear Response TDDFT
    type: String
    description: |
      The exchange-correlation kernel used in the calculation. Currently supported: RPA, LDA, PBE, HSE, HF.
    default_value: LDA
    unit: ""
    availability: ""
  - name: lr_init_xc_kernel
    category: Linear Response TDDFT
    type: "Vector of String (>=1 values)"
    description: |
      The method to initalize the xc kernel.
      * "default": Calculate xc kernel from the ground-state charge density.
      * "file": Read the xc kernel on grid from the provided files. The following words should be the paths of ".cube" files, where the first 1 (nspin==1) or 3 (nspin==2, namely spin-aa, spin-ab and spin-bb) will be read in. The parameter xc_kernel will be invalid. Now only LDA-type kernel is supported as the potential will be calculated by directly multiplying the transition density.
      * "from_charge_file": Calculate fxc from the charge density read from the provided files. The following words should be the paths of ".cube" files, where the first nspin files will be read in.
    default_value: "\"default\""
    unit: ""
    availability: ""
  - name: lr_solver
    category: Linear Response TDDFT
    type: String
    description: |
      The method to solve the Casida equation in LR-TDDFT under Tamm-Dancoff approximation (TDA).
      * dav/dav_subspace/cg: Construct and diagonalize the Hamiltonian matrix iteratively with Davidson/Non-ortho-Davidson/CG algorithm.
      * lapack: Construct the full matrix and directly diagonalize with LAPACK.
      * spectrum: Calculate absorption spectrum only without solving Casida equation.
    default_value: dav
    unit: ""
    availability: ""
  - name: lr_thr
    category: Linear Response TDDFT
    type: Real
    description: |
      The convergence threshold of iterative diagonalization solver for LR-TDDFT. It is a pure-math number with the same meaning as pw_diag_thr, but since the Casida equation is a one-shot eigenvalue problem, it is also the convergence threshold of LR-TDDFT.
    default_value: "1e-2"
    unit: ""
    availability: ""
  - name: nocc
    category: Linear Response TDDFT
    type: Integer
    description: |
      The number of occupied orbitals (up to HOMO) used in the LR-TDDFT calculation.
      * Note: If the value is illegal ( > nelec/2 or <= 0), it will be autoset to nelec/2.
    default_value: nband
    unit: ""
    availability: ""
  - name: nvirt
    category: Linear Response TDDFT
    type: Integer
    description: |
      The number of virtual orbitals (starting from LUMO) used in the LR-TDDFT calculation.
    default_value: "1"
    unit: ""
    availability: ""
  - name: lr_nstates
    category: Linear Response TDDFT
    type: Integer
    description: |
      The number of 2-particle states to be solved.
    default_value: "0"
    unit: ""
    availability: ""
  - name: lr_unrestricted
    category: Linear Response TDDFT
    type: Boolean
    description: |
      Whether to use unrestricted construction for LR-TDDFT (the matrix size will be doubled).
      * True: Always use unrestricted LR-TDDFT.
      * False: Use unrestricted LR-TDDFT only when the system is open-shell.
    default_value: "False"
    unit: ""
    availability: ""
  - name: abs_wavelen_range
    category: Linear Response TDDFT
    type: Real Real
    description: |
      The range of the wavelength for the absorption spectrum calculation.
    default_value: 0.0 0.0
    unit: nm
    availability: ""
  - name: out_wfc_lr
    category: Linear Response TDDFT
    type: Boolean
    description: |
      Whether to output the eigenstates (excitation energy) and eigenvectors (excitation amplitude) of the LR-TDDFT calculation. The output files are OUT.{suffix}/Excitation_Amplitude_${processor_rank}.dat.
    default_value: "False"
    unit: ""
    availability: ""
  - name: abs_gauge
    category: Linear Response TDDFT
    type: String
    description: |
      Whether to use length or velocity gauge to calculate the absorption spectrum in LR-TDDFT.
    default_value: velocity
    unit: ""
    availability: ""
  - name: abs_broadening
    category: Linear Response TDDFT
    type: Real
    description: |
      The broadening factor for the absorption spectrum calculation.
    default_value: "0.01"
    unit: ""
    availability: ""
  - name: bse_tda
    category: Bethe-Salpeter Equation
    type: String
    description: |
      Whether the Tamm-Dancoff approximation is used: 'tda', 'full', or 'both'.
    default_value: tda
    unit: ""
    availability: ""
  - name: bse_spin_types
    category: Bethe-Salpeter Equation
    type: "Vector of String (>=1 values)"
    description: |
      Spin types for a closed-shell calculation in one task: 'singlet', 'triplet', and the test modes 'rpa' and 'ipa'.
    default_value: singlet triplet
    unit: ""
    availability: ""
  - name: bse_mem_save
    category: Bethe-Salpeter Equation
    type: Boolean
    description: |
      Whether to save memory by adding V and W directly to the BSE matrix. When enabled, bse_ri_hartree is enabled and bse_continue is reset to 0.
    default_value: "false"
    unit: ""
    availability: ""
  - name: bse_ri_hartree
    category: Bethe-Salpeter Equation
    type: Boolean
    description: |
      Whether to use the RI approximation for the Hartree term in BSE.
    default_value: "true"
    unit: ""
    availability: ""
  - name: bse_use_fine_kgrid
    category: Bethe-Salpeter Equation
    type: Integer
    description: |
      Fine k-grid mode for BSE: 0 uses the coarse k-grid, 1 uses a uniform fine k-grid, and 2 uses a non-uniform fine k-grid. Modes 1 and 2 require band_kpath_info, band_KS_eigenvector_k_{index}.txt, KS_band_spin_{index}.txt, and GW_band_spin_{index}.txt.
    default_value: "0"
    unit: ""
    availability: ""
  - name: bse_q_approx_mode
    category: Bethe-Salpeter Equation
    type: Integer
    description: |
      q-to-k-pair mapping mode: 0 uses exact mapping, 1 uses the coarse q-grid approximation, and 2 uses exact for Γ-close q-points and coarse for other q-points.
    default_value: "0"
    unit: ""
    availability: ""
  - name: bse_q_approx_threshold
    category: Bethe-Salpeter Equation
    type: Real
    description: |
      Threshold radius in Bohr^-1 for exact q-to-k-pair mapping when bse_q_approx_mode is 2.
    default_value: "0.1"
    unit: ""
    availability: ""
  - name: out_bse_ab
    category: Bethe-Salpeter Equation
    type: Boolean
    description: |
      Whether to output the AB matrix to a file.
    default_value: "false"
    unit: ""
    availability: ""
  - name: bse_continue
    category: Bethe-Salpeter Equation
    type: Integer
    description: |
      Step from which to continue a previous BSE calculation: 0 starts a new calculation; 1 reads A_V; 2 reads A_V and A_W; 3 reads A_V, A_W, and B_V; 4 reads A_V, A_W, B_V, and B_W.
    default_value: "0"
    unit: ""
    availability: ""
  - name: plot_istate
    category: Linear Response TDDFT
    type: Integer
    description: |
      The index of the excited state to plot, starting from 0.
    default_value: "0"
    unit: ""
    availability: ""
  - name: exciton_plot_type
    category: Linear Response TDDFT
    type: String
    description: |
      Exciton density represented when lr_solver is 'plot': 'average' integrates out the other particle, while 'conditional' fixes one particle at exciton_fixed_coordinate and plots a slice of the other particle's density.
    default_value: average
    unit: ""
    availability: ""
  - name: exciton_plot_format
    category: Linear Response TDDFT
    type: String
    description: |
      The exciton-density output format. Average density supports cube, slice, and both; conditional density supports slice only.
    default_value: cube
    unit: ""
    availability: lr_solver==plot
  - name: exciton_fixed_coordinate
    category: Linear Response TDDFT
    type: Vector of Real (6 values)
    description: |
      Cartesian coordinates in Bohr used by conditional exciton plotting, in the order hole_x hole_y hole_z electron_x electron_y electron_z.
    default_value: 0.0 0.0 0.0 0.0 0.0 0.0
    unit: ""
    availability: ""
  - name: exciton_slice_plane
    category: Linear Response TDDFT
    type: String
    description: |
      Pair of lattice-vector directions spanning the cross section: 'ab', 'bc', or 'ca'.
    default_value: "ab"
    unit: ""
    availability: ""
  - name: exciton_slice_pos
    category: Linear Response TDDFT
    type: Real
    description: |
      Offset in Bohr along the remaining lattice-vector direction: c for an ab slice, a for bc, and b for ca.
    default_value: "0.0"
    unit: ""
    availability: ""
  - name: exciton_slice_npoints
    category: Linear Response TDDFT
    type: Integer
    description: |
      Target in-plane grid resolution. The final grid uses a uniform number of points per primitive cell over `exciton_slice_range` and includes both endpoints.
    default_value: "200"
    unit: ""
    availability: ""
  - name: exciton_slice_range
    category: Linear Response TDDFT
    type: Vector of Integer (4 values)
    description: |
      The in-plane primitive-cell range of an exciton slice: ustart uend vstart vend. The end values are exclusive cell boundaries, while grid data include both range endpoints.
    default_value: "-1 2 -1 2"
    unit: primitive cells
    availability: "lr_solver==plot and exciton_plot_format in [slice, both]"
  - name: out_freq_ion
    category: Output information
    type: Integer
    description: |
      Controls the output interval in ionic steps. When set to a positive integer, information such as charge density, local potential, electrostatic potential, Hamiltonian matrix, overlap matrix, density matrix, Mulliken population analysis, and structure files (STRU{istep} or STRU{istep}.cif, when out_stru is 1 or 2) is printed every n ionic steps.

      [NOTE] In RT-TDDFT calculations, this parameter is inactive; output frequency is instead controlled by out_freq_td.
    default_value: "0"
    unit: ""
    availability: ""
  - name: out_freq_td
    category: Output information
    type: Integer
    description: |
      Controls the output interval in completed electronic evolution steps during RT-TDDFT calculations. When set to a positive integer n, detailed information (see out_freq_ion) is printed every n electron time-evolution steps (i.e., every STEP OF ELECTRON EVOLVE). For example, if you wish to output information once per ionic step, you should set out_freq_td equal to estep_per_md, since one ionic step corresponds to estep_per_md electronic evolution steps.

      [NOTE] This parameter is only active in RT-TDDFT mode (esolver_type = tddft). It has no effect in ground-state calculations.
    default_value: "0"
    unit: ""
    availability: ""
  - name: out_freq_elec
    category: Output information
    type: Integer
    description: |
      Output the charge density (only binary format, controlled by out_chg), wavefunction (controlled by out_wfc_pw) per out_freq_elec electronic iterations. Note that they are always output when converged or reach the maximum iterations scf_nmax.
    default_value: scf_nmax
    unit: ""
    availability: ""
  - name: out_chg
    category: Output information
    type: "Integer \\[Integer\\](optional)"
    description: |
      The first integer controls whether to output the charge density on real space grids:
          - 1: Output the charge density (in Bohr^-3) on real space grids into the density files in the folder `OUT.${suffix}`. The files are named as:
              - nspin = 1: `chg.cube`;
              - nspin = 2: `chgs1.cube`, and `chgs2.cube`;
              - nspin = 4: `chgs1.cube`, `chgs2.cube`, `chgs3.cube`, and `chgs4.cube`;
              - When using the Meta-GGA functional, additional files containing the kinetic energy density are also output:
                  - nspin = 1: `tau.cube`;
                  - nspin = 2: `taus1.cube`, and `taus2.cube`;
                  - nspin = 4: `taus1.cube`, `taus2.cube`, `taus3.cube`, and `taus4.cube`;
          - 2: On top of 1, also output the initial charge density files. The files are named as:
              - out_freq_ion = 0:
                  - nspin = 1: `chg_ini.cube`;
                  - nspin = 2: `chgs1_ini.cube` and `chgs2_ini.cube`;
                  - nspin = 4: `chgs1_ini.cube`, `chgs2_ini.cube`, `chgs3_ini.cube`, and `chgs4_ini.cube`;
                  - output at every step (overwrite same file)
              - out_freq_ion > 0:
                  - nspin = 1: `chgg{geom_step}_ini.cube` (e.g., `chgg1_ini.cube`);
                  - nspin = 2: `chgs1g{geom_step}_ini.cube` and `chgs2g{geom_step}_ini.cube`;
                  - nspin = 4: `chgs1g{geom_step}_ini.cube`, `chgs2g{geom_step}_ini.cube`, `chgs3g{geom_step}_ini.cube`, and `chgs4g{geom_step}_ini.cube`.
                  - output every out_freq_ion steps
              Here, {geom_step} denotes the geometry step index, starting from 1 (geom_step = istep + 1).
          - -1: Disable the charge density auto-back-up file `{suffix}-CHARGE-DENSITY.restart`, useful for large systems.

      The second integer controls the precision of the charge density output. If not given, `3` is used as default. For restarting from this file and other high-precision calculations, `10` is recommended.

      In molecular dynamics simulations, the output frequency is controlled by out_freq_ion.

      [NOTE] In the 3.10-LTS version, the file names are SPIN1_CHG.cube and SPIN1_CHG_INI.cube, etc.
    default_value: 0 3
    unit: ""
    availability: ""
  - name: out_pot
    category: Output information
    type: "Integer \\[Integer\\](optional)"
    description: |
      * 1: Output the total local potential (i.e., local pseudopotential + Hartree potential + XC potential + external electric field (if exists) + dipole correction potential (if exists) + ...) on real space grids (in Ry) into files in the folder OUT.{suffix}. The files are named as:
       * nspin = 1: pots1.cube;
       * nspin = 2: pots1.cube and pots2.cube;
       * nspin = 4: pots1.cube, pots2.cube, pots3.cube, and pots4.cube
      * 2: Output the electrostatic potential on real space grids into OUT.{suffix}/pot_es.cube. The Python script named tools/02_postprocessing/average_pot/aveElecStatPot.py can be used to calculate the average electrostatic potential along the z-axis and outputs it into ElecStaticPot_AVE. Please note that the total local potential refers to the local component of the self-consistent potential, excluding the non-local pseudopotential. The distinction between the local potential and the electrostatic potential is as follows: local potential = electrostatic potential + XC potential.
      * 3: Apart from 1, also output the total local potential of the initial charge density. The files are named as:
       * out_freq_ion = 0:
         * nspin = 1: `pot_ini.cube`;
         * nspin = 2: `pots1_ini.cube` and `pots2_ini.cube`;
         * nspin = 4: `pots1_ini.cube`, `pots2_ini.cube`, `pots3_ini.cube`, and `pots4_ini.cube`;
         * output at every step (overwrite same file)
       * out_freq_ion > 0:
         * nspin = 1: `potg{geom_step}_ini.cube` (e.g., `potg1_ini.cube`);
         * nspin = 2: `pots1g{geom_step}_ini.cube` and `pots2g{geom_step}_ini.cube`;
         * nspin = 4: `pots1g{geom_step}_ini.cube`, `pots2g{geom_step}_ini.cube`, `pots3g{geom_step}_ini.cube`, and `pots4g{geom_step}_ini.cube`.
         * output every out_freq_ion steps
       Here, {geom_step} denotes the geometry step index, starting from 1 (geom_step = istep + 1).

      The optional second integer controls the output precision. If not provided, the default precision is 8.

      In molecular dynamics calculations, the output frequency is controlled by out_freq_ion.

      [NOTE] In the 3.10-LTS version, the file names are SPIN1_POT.cube and SPIN1_POT_INI.cube, etc.
    default_value: "0"
    unit: ""
    availability: ""
  - name: out_dmk
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to output the density matrix for each k-point into files in the folder OUT.${suffix}. For current develop versions, out_dmk writes *_nao.txt files and includes a g{istep} index in the file name:
          * For gamma only case:
           * nspin = 1 and 4: dmg1_nao.txt;
           * nspin = 2: dms1g1_nao.txt and dms2g1_nao.txt for the two spin channels.
          * For multi-k points case:
           * nspin = 1 and 4: dmk1g1_nao.txt, dmk2g1_nao.txt, ...;
           * nspin = 2: dmk1s1g1_nao.txt... and dmk1s2g1_nao.txt... for the two spin channels.

          Here, g{istep} denotes the geometry/step index in the output file name.

          [NOTE] Version difference (develop vs 3.10-LTS):
          * In develop, out_dmk supports both gamma-only and multi-k-point density-matrix output.
          * In 3.10-LTS, the corresponding keyword is out_dm, and the output files are SPIN1_DM and SPIN2_DM, etc.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: out_dmr
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to output the density matrix with Bravias lattice vector R index into files in the folder OUT.${suffix}. The files are named as dmr{s}{spin index}{g}{geometry index}{_nao} + {".csr"}. Here, 's' refers to spin, where s1 means spin up channel while s2 means spin down channel, and the sparse matrix format 'csr' is mentioned in out_hsr. Finally, if out_app_flag is set to false, the file name contains the optional 'g' index for each ionic step that may have different geometries, and if out_app_flag is set to true, the density matrix with respect to Bravias lattice vector R accumulates during ionic steps:
      * nspin = 1: dmrs1_nao.csr;
      * nspin = 2: dmrs1_nao.csr and dmrs2_nao.csr for the two spin channels.

      [NOTE] In the 3.10-LTS version, the parameter is named out_dm1, and the file names are data-DMR-sparse_SPIN0.csr and data-DMR-sparse_SPIN1.csr, etc.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao and gamma_only==0
  - name: out_wfc_pw
    category: Output information
    type: Integer
    description: |
      Whether to output the electronic wavefunction coefficients into files and store them in the folder OUT.${suffix}. The files are named as wf{k}{k-point index}{s}{spin index}{g}{geometry index}{e}{electronic iteration index}{_pw} + {".txt"/".dat"}. Here, the s index refers to spin but the label will not show up for non-spin-polarized calculations, where s1 means spin up channel while s2 means spin down channel, and s4 refers to spinor wave functions that contains both spin channels with spin-orbital coupling or noncollinear calculations enabled. For scf or nscf calculations, g index will not appear, but the g index appears for geometry relaxation and molecular dynamics, where one can use the out_freq_ion command to control. To print out the electroinc wave functions every few SCF iterations, use the out_freq_elec command and the e index will appear in the file name.
      * 0: no output
      * 1: (txt format)
       * non-gamma-only with nspin=1: wfk1_pw.txt, wfk2_pw.txt, ...;
       * non-gamma-only with nspin=2: wfk1s1_pw.txt, wfk1s2_pw.txt, wfk2s1_pw.txt, wfk2s2_pw.txt, ...;
       * non-gamma-only with nspin=4: wfk1s4_pw.txt, wfk2s4_pw.txt, ...;
      * 2: (binary format)
       * non-gamma-only with nspin=1: wfk1_pw.dat, wfk2_pw.dat, ...;
       * non-gamma-only with nspin=2: wfk1s1_pw.dat, wfk1s2_pw.dat, wfk2s1_pw.dat, wfk2s2_pw.dat, ...;
       * non-gamma-only with nspin=4: wfk1s4_pw.dat, wfk2s4_pw.dat, ...;

      [NOTE] In the 3.10-LTS version, the file names are WAVEFUNC1.dat, WAVEFUNC2.dat, etc.
    default_value: "0"
    unit: ""
    availability: basis_type==pw or (basis_type==lcao and calculation==get_wf)
  - name: out_wfc_lcao
    category: Output information
    type: Integer
    description: |
      Whether to output the electronic wavefunction coefficients into files and store them in the folder OUT.${suffix}. The files are named as wf{s}{spin index}{k(optional)}{k-point index}{g(optional)}{geometry index1}{_nao} + {".txt"/".dat"}. Here, 's' refers to spin, where s1 means spin up channel while s2 means spin down channel, and 's12' refer to spinor wave functions that contains both spin channels with spin-orbital coupling or noncollinear calculations enabled. In addition, if 'gamma_only' is set to 0, then the optinoal k-point sampling index appears with the k-point index attached to the electronic wave function file names. Finally, if out_app_flag is set to false, the file name contains the optional 'g' index for each ionic step that may have different geometries, and if out_app_flag is set to true, the wave functions accumulate during ionic steps. If the out_app_flag is set to false, a new folder named WFC will be created, and the wave function files will be saved into it.
      * 0: no output
      * 1: (txt format)
       * gamma-only: wfs1_nao.txt or wfs2_nao.txt, ...;
       * non-gamma-only: wfs1k1_nao.txt or wfs1k2_nao.txt, ...;
      * 2: (binary format)
       * gamma-only: wfs1_nao.dat or wfs2_nao.dat, ...;
       * non-gamma-only: wfs1k1_nao.dat or wfs1k2_nao.dat, ....

      The corresponding sequence of the orbitals can be seen in Basis Set.

      Also controled by out_freq_ion and out_app_flag.

      [NOTE] In the 3.10-LTS version, the file names are WFC_NAO_GAMMA1_ION1.txt and WFC_NAO_K1_ION1.txt, etc.
    default_value: "0"
    unit: ""
    availability: basis_type==lcao
  - name: out_dos
    category: Output information
    type: Integer
    description: |
      Whether to output the density of states (DOS). For more information, refer to the dos.md.
      * 0: no output
      * 1: output the density of states (DOS)
       * nspin=1 or 4: doss1g{geom}_{basis}.txt, where geom is the geometry index when cell changes or ions move while basis is either pw or nao.
       * nspin=2: doss1g{geom}_{basis}.txt and doss2g{geom}_{basis}.txt for two spin channles.
      * 2: (LCAO) output the density of states (DOS) and the projected density of states (PDOS)
      * 3: output the Fermi surface file (fermi.bxsf) in BXSF format that can be visualized by XCrySDen
    default_value: "0"
    unit: ""
    availability: ""
  - name: out_ldos
    category: Output information
    type: "Integer \\[Integer\\](optional)"
    description: |
      Whether to output the local density of states (LDOS), optionally output precision can be set by a second parameter, default is 3.
      * 0: no output
      * 1: output the partial charge density for given bias (controlled by stm_bias) in cube file format, which can be used to plot scanning tunneling spectroscopys to mimick STM images using the Python script plot.py.
      * 2: output LDOS along a line in real space (controlled by ldos_line). Parameters used to control DOS output are also valid for LDOS.
      * 3: output both two LDOS modes above.
    default_value: "0"
    unit: ""
    availability: ""
  - name: out_band
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to output the eigenvalues of the Hamiltonian matrix (in eV) into the running log during electronic iterations and into a file at the end of calculations. The former can be used with the 'out_freq_elec' parameter while the latter option allows the output precision to be set via a second parameter, with a default value of 8. The output file names are:
       * nspin = 1 or 4: eig.txt;
       * nspin = 2: eigs1.txt and eigs2.txt;
       * For more information, refer to the band.md
    default_value: "False"
    unit: ""
    availability: ""
  - name: out_proj_band
    category: Output information
    type: Boolean
    description: |
      Whether to output the projected band structure. For more information, refer to the band.md
    default_value: "False"
    unit: ""
    availability: ""
  - name: out_stru
    category: Output information
    type: Integer
    description: |
      Controls the output of structure files per ionic step in geometry relaxation calculations. The files are written to the OUT.{suffix}/ directory. Each file corresponds to the structure at RELAX STEP ${istep}, i.e., the structure for which that step's energy was computed (before the relax move), and includes a header comment with the ABACUS version, timestamp, energy, and stress tensor. When out_freq_ion is positive, the numbered files STRU{istep} (or STRU{istep}.cif) are written every out_freq_ion steps; when out_freq_ion is 0, no numbered files are output.
          - 0: No structure files are output.
          - 1: ABACUS STRU format files are output. The latest structure is written to STRU_NOW (overwritten each step), the numbered file STRU{istep} (e.g., STRU1, STRU2) is written every out_freq_ion steps (when out_freq_ion is positive), and the final converged structure is written to STRU_FINAL. No CIF files are output.
          - 2: CIF format files are output. The latest structure is written to STRU_NOW.cif (overwritten each step), the numbered file STRU{istep}.cif (e.g., STRU1.cif, STRU2.cif) is written every out_freq_ion steps (when out_freq_ion is positive), and the final converged structure is written to STRU_FINAL.cif. No non-CIF files are output.
      [NOTE] For backward compatibility, true/false (case insensitive) are accepted and converted to 1/0.
    default_value: "1"
    unit: ""
    availability: ""
  - name: out_level
    category: Output information
    type: String
    description: |
      Control the output level of information in OUT.{calculation}.log.
      * ie: electronic iteration level, which prints useful information for electronic iterations;
      * i: geometry relaxation level, which prints some information for geometry relaxations additionally;
      * m: molecular dynamics level, which does not print some information for simplicity.
    default_value: ie
    unit: ""
    availability: ""
  - name: out_hsk
    category: Output information
    type: "Integer \\[Integer\\](optional)"
    description: |
      Output the upper triangular part of the Hamiltonian and overlap matrices in reciprocal space for each k-point into files in the directory OUT.${suffix}. The first integer selects the format:
      * 0: disabled;
      * 1: text output; the optional second integer controls precision and defaults to 8;
      * 2: binary output in the native ABACUS .dat format;
      * 3: NPZ output, which is not implemented for H(k)/S(k).

      The output is also controlled by out_freq_ion and out_app_flag. For more information, refer to hs_matrix.md.
      * Gamma-only, nspin = 1: hk_nao.txt for the Hamiltonian matrix and sk_nao.txt for the overlap matrix.
      * Gamma-only, nspin = 2: hks1_nao.txt and hks2_nao.txt for the two spin channels of the Hamiltonian matrix, and sk_nao.txt for the overlap matrix. Only one overlap matrix is written because it is identical for both spin channels.
      * Gamma-only, nspin = 4: not available with the gamma-only algorithm.
      * Multi-k, nspin = 1: hk1_nao.txt for the Hamiltonian matrix and sk1_nao.txt for the overlap matrix at the first k-point.
      * Multi-k, nspin = 2: hk1s1_nao.txt and hk1s2_nao.txt for the two spin channels of the Hamiltonian matrix, and sk1_nao.txt for the overlap matrix at the first k-point. Only one overlap matrix is written because it is identical for both spin channels.
      * Multi-k, nspin = 4: hk1s4_nao.txt for the spinor Hamiltonian matrix and sk1_nao.txt for the spinor overlap matrix at the first k-point.
      For binary output, the same names use the .dat suffix. Each native binary record contains the matrix dimension as an int followed by the row-major upper triangle. Gamma-only elements are doubles; multi-k and spinor elements are pairs of doubles containing the real and imaginary parts. Native integer representation and byte order are used.
      When out_app_flag is true, the first ionic step truncates the file and later steps append complete records.
      When out_app_flag is false, g followed by the one-based ionic-step index is inserted before _nao, for example hk1s1g1_nao.txt.

      [NOTE] In the 3.10-LTS version, the file names are data-0-H and data-0-S, etc.
    default_value: 0 8
    unit: Ry
    availability: basis_type==lcao
  - name: out_mat_hs
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Legacy alias for out_hsk 1, which outputs Hamiltonian and overlap matrices in reciprocal space for each k-point. The optional second integer controls text precision. If both out_hsk and out_mat_hs are present, out_hsk takes precedence.
    default_value: False 8
    unit: Ry
    availability: basis_type==lcao
  - name: out_hsr
    category: Output information
    type: "Integer \\[Integer\\](optional)"
    description: |
      Output Hamiltonian and overlap matrices in real space, indexed by the Bravais lattice vector R, in the directory OUT.${suffix}. The first integer selects the format:
      * 0: disabled;
      * 1: text CSR output; the optional second integer controls precision and defaults to 8;
      * 2: native binary CSR output using .dat files;
      * 3: NPZ output using hrs1_nao.npz, hrs2_nao.npz when needed, and sr_nao.npz.

      For multi-k calculations, the output contains the individual real-space blocks stored for the Bravais lattice vectors R. For gamma-only calculations, the internal real-space contributions are folded into a single R = (0, 0, 0) block. This folded result cannot recover the original R-resolved contributions or interpolate arbitrary k points. Terms added only while constructing H(k) are not guaranteed to be present.

      For binary output, each file uses the same basename as text output with a .dat suffix. Every native record contains the zero-based ionic step, matrix dimension, and number of R blocks as ints. Each R block contains three int coordinates, an int nonzero count, native double values (real/imaginary double pairs for complex matrices), int column indices, and long long row pointers. Native integer representation and byte order are used. When out_app_flag is true, the first ionic step truncates the file and later steps append complete records.

      [NOTE] In the 3.10-LTS version, the file names are data-HR-sparse_SPIN0.csr and data-SR-sparse_SPIN0.csr, etc.
    default_value: 0 8
    unit: Ry
    availability: basis_type==lcao
  - name: out_mat_hs2
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Legacy alias for out_hsr 1, which outputs Hamiltonian and overlap matrices in real space indexed by the Bravais lattice vector R. The optional second integer controls text precision. If both out_hsr and out_mat_hs2 are present, out_hsr takes precedence.
    default_value: False 8
    unit: Ry
    availability: basis_type==lcao
  - name: out_mat_tk
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to print the upper triangular part of the kinetic matrices for each k-point into OUT.${suffix}/tks1ki_nao.txt, where i is the index of k points. One may optionally provide a second parameter to specify the precision.

      [NOTE] In the 3.10-LTS version, the file names are data-TR-sparse_SPIN0.csr, etc.
    default_value: "False [8]"
    unit: Ry
    availability: basis_type==lcao
  - name: out_mat_r
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to print the matrix representation of the position matrix into files named rxrs1_nao.csr, ryrs1_nao.csr, rzrs1_nao.csr in the directory OUT.${suffix}. The optional second parameter controls text output precision. If calculation is set to get_s, the position matrix can be obtained without scf iterations. For more information, please refer to position_matrix.md.

      [NOTE] In the 3.10-LTS version, the file name is data-rR-sparse.csr.
    default_value: False 8
    unit: Bohr
    availability: basis_type==lcao and gamma_only==0
  - name: out_mat_t
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Generate files containing the kinetic energy matrix. The optional second parameter controls text output precision. The format will be the same as the Hamiltonian matrix and overlap matrix as mentioned in out_hsr. The name of the files will be trs1_nao.csr and so on. Also controled by out_freq_ion and out_app_flag.

      [NOTE] In the 3.10-LTS version, the file name is data-TR-sparse_SPIN0.csr.
    default_value: False 8
    unit: Ry
    availability: basis_type==lcao and gamma_only==0
  - name: out_mat_dh
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the derivatives of the Hamiltonian matrix. The format will be the same as the Hamiltonian matrix and overlap matrix as mentioned in out_hsr. The name of the files will be dhrxs1_nao.csr, dhrys1_nao.csr, dhrzs1_nao.csr and so on. Also controled by out_freq_ion and out_app_flag.

      Format: <enable> [precision] [iat1 iat2 ...]. The first value (0/1) enables/disables output. The second optional value sets the output precision (default: 8). Starting from the third value, 1-based atom indices can be listed to restrict output to derivatives with respect to those specific atoms only; if no atom indices are given, all atoms are written.

      [NOTE] In the 3.10-LTS version, the file name is data-dHRx-sparse_SPIN0.csr and so on.
    default_value: 0 8
    unit: Ry/Bohr
    availability: basis_type==lcao and gamma_only==0
  - name: out_mat_dh_t
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the derivatives of the kinetic energy matrix dT/dR.

      See out_mat_dh for format details (enable, precision, atom indices).
    default_value: 0 8
    unit: Ry/Bohr
    availability: ""
  - name: out_mat_dh_vl
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the derivatives of the local pseudopotential matrix dV^L/dR.

      See out_mat_dh for format details.
    default_value: 0 8
    unit: Ry/Bohr
    availability: ""
  - name: out_mat_dh_vnl
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the derivatives of the nonlocal pseudopotential matrix dV^NL/dR.

      See out_mat_dh for format details.
    default_value: 0 8
    unit: Ry/Bohr
    availability: ""
  - name: out_mat_dh_vh
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the derivatives of the Hartree matrix dV^H/dR.

      See out_mat_dh for format details.
    default_value: 0 8
    unit: Ry/Bohr
    availability: ""
  - name: out_mat_dh_vxc
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the derivatives of the XC matrix dV^XC/dR.

      See out_mat_dh for format details.
    default_value: 0 8
    unit: Ry/Bohr
    availability: ""
  - name: out_mat_dh_exx
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the derivatives of the exact-exchange matrix dV^EXX/dR.

      See out_mat_dh for format details.
    default_value: 0 8
    unit: Ry/Bohr
    availability: ""
  - name: out_mat_h_t
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the kinetic energy matrix T(R) in CSR format.

      See out_hsr for format details.
    default_value: 0 8
    unit: Ry
    availability: ""
  - name: out_mat_h_vnl
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the nonlocal pseudopotential matrix Vnl(R) in CSR format.

      See out_hsr for format details.
    default_value: 0 8
    unit: Ry
    availability: ""
  - name: out_mat_h_vl
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the local pseudopotential matrix Vl(R) in CSR format.

      See out_hsr for format details.
    default_value: 0 8
    unit: Ry
    availability: ""
  - name: out_mat_h_vh
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the Hartree matrix Vh(R) in CSR format.

      See out_hsr for format details.
    default_value: 0 8
    unit: Ry
    availability: ""
  - name: out_mat_h_vxc
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the XC matrix Vxc(R) in CSR format.

      See out_hsr for format details.
    default_value: 0 8
    unit: Ry
    availability: ""
  - name: out_mat_h_exx
    category: Output information
    type: Integer
    description: |
      Whether to print files containing the exact-exchange matrix Vexx(R) in CSR format.

      See out_hsr for format details.
    default_value: 0 8
    unit: Ry
    availability: ""
  - name: out_mat_ds
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to print files containing the derivatives of the overlap matrix. The optional second parameter controls text output precision. The format will be the same as the overlap matrix as mentioned in out_mat_dh. The name of the files will be dsxrs1_nao.csr and so on. Also controled by out_freq_ion and out_app_flag. This feature can be used with calculation get_s.

      [NOTE] In the 3.10-LTS version, the file name is data-dSRx-sparse_SPIN0.csr and so on.
    default_value: False 8
    unit: Ry/Bohr
    availability: basis_type==lcao and gamma_only==0
  - name: out_mat_xc
    category: Output information
    type: Boolean
    description: |
      Whether to print the upper triangular part of the exchange-correlation matrices in Kohn-Sham orbital representation: for each k point into files in the directory OUT.i_nao.txt, where {suffix}/vxc_out.dat. If EXX is calculated, the local and EXX part of band energy will also be printed in OUT.{suffix}/vxc_exx_out.dat, respectively. All the vxc_out.dat files contains 3 integers (nk, nspin, nband) followed by nk*nspin*nband lines of energy Hartree and eV.

      [NOTE] In the 3.10-LTS version, the file name is k-$k-Vxc and so on.
    default_value: "False"
    unit: Ry
    availability: "basis_type in [lcao, lcao_in_pw]"
  - name: out_mat_xc2
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to print the exchange-correlation matrices in numerical orbital representation: in CSR format in the directory OUT.${suffix}. The name of the files will be vxcrs1_nao.csr and so on.

      [NOTE] In the 3.10-LTS version, the file name is Vxc_R_spin$s and so on.
    default_value: False 8
    unit: Ry
    availability: basis_type==lcao
  - name: out_mat_l
    category: Output information
    type: "Boolean \\[Integer\\](optional)"
    description: |
      Whether to print the expectation value of the angular momentum operator , , and in the basis of the localized atomic orbitals. The files are named OUT.{suffix}_Lx.dat, OUT.{suffix}_Ly.dat, and OUT.{suffix}_Lz.dat. The second integer controls the precision of the output.
    default_value: False 8
    unit: ""
    availability: basis_type==lcao
  - name: out_xc_r
    category: Output information
    type: "Integer \\[Integer\\](optional)"
    description: |
      The first integer controls whether to output the exchange-correlation (in Bohr^-3) on real space grids using Libxc to folder OUT.${suffix}:
      * 0: rho, amag, sigma, exc
      * 1: vrho, vsigma
      * 2: v2rho2, v2rhosigma, v2sigma2
      * 3: v3rho3, v3rho2sigma, v3rhosigma2, v3sigma3
      * 4: v4rho4, v4rho3sigma, v4rho2sigma2, v4rhosigma3, v4sigma4 The meaning of the files is presented in Libxc

      The second integer controls the precision of the charge density output, if not given, will use 3 as default.

      The circle order of the charge density on real space grids is: x is the outer loop, then y and finally z (z is moving fastest).
    default_value: "-1 3"
    unit: ""
    availability: ""
  - name: out_eband_terms
    category: Output information
    type: Boolean
    description: |
      Whether to print the band energy terms separately in the file OUT.{term}_out.dat. The terms include the kinetic, pseudopotential (local + nonlocal), Hartree and exchange-correlation (including exact exchange if calculated).
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: out_hr_npz
    category: Output information
    type: Boolean
    description: |
      Whether to print Hamiltonian matrices H(R) in NPZ format as hrs1_nao.npz and, for nspin = 2, hrs2_nao.npz. This feature does not work for gamma-only calculations.
    default_value: "False"
    unit: Ry
    availability: basis_type==lcao and gamma_only==0
  - name: out_hsr_npz
    category: Output information
    type: Boolean
    description: |
      Legacy alias for out_hsr 3, writing hrs1_nao.npz, hrs2_nao.npz when needed, and sr_nao.npz. If both out_hsr and out_hsr_npz are present, out_hsr takes precedence. Gamma-only calculations write the folded R = (0, 0, 0) representation.
    default_value: "False"
    unit: Ry
    availability: basis_type==lcao
  - name: out_dm_npz
    category: Output information
    type: Boolean
    description: |
      Whether to print density matrices DM(R) in npz format. This feature does not work for gamma-only calculations.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao and gamma_only==0
  - name: out_mul
    category: Output information
    type: Boolean
    description: |
      Whether to print the Mulliken population analysis result into OUT.${suffix}/mulliken.txt. In molecular dynamics calculations, the output frequency is controlled by out_freq_ion.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: out_app_flag
    category: Output information
    type: Boolean
    description: |
      Whether to output r(R), H(R), S(R), T(R), dH(R), dS(R), and wfc matrices in an append manner during molecular dynamics calculations. Check input parameters out_mat_r, out_hsr, out_mat_t, out_mat_dh, out_hsk and out_wfc_lcao for more information.
    default_value: "true"
    unit: ""
    availability: basis_type==lcao and gamma_only==0
  - name: out_ndigits
    category: Output information
    type: Integer
    description: |
      Controls the length of decimal part of output data, such as charge density, Hamiltonian matrix, Overlap matrix and so on.
    default_value: "8"
    unit: ""
    availability: basis_type==lcao and out_hsk==1
  - name: out_element_info
    category: Output information
    type: Boolean
    description: |
      Whether to print element information into files in the directory OUT.{element_label}, including pseudopotential and orbital information of the element (in atomic Ryberg units).
    default_value: "False"
    unit: ""
    availability: ""
  - name: restart_save
    category: Output information
    type: Boolean
    description: |
      Whether to save charge density files per ionic step, which are used to restart calculations. According to the value of read_file_dir:
      * auto: These files are saved in folder OUT.{read_file_dir}/restart/.

      If EXX(exact exchange) is calculated (i.e. dft_fuctional==hse/hf/pbe0/scan0 or rpa==True), the Hexx(R) files for each processor will also be saved in the above folder, which can be read in EXX calculation with restart_load==True.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: rpa
    category: Output information
    type: Boolean
    description: |
      Generate output files used in rpa calculations.

      [NOTE] If symmetry is set to 1, additional files containing the necessary information for exploiting symmetry in the subsequent rpa calculation will be output: irreducible_sector.txt, symrot_k.txt and symrot_R.txt.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: rpa_out_vel
    category: Output information
    type: Boolean
    description: |
       Velocity matrix in KS basis (in unit of eV *Angstrom). Loop layer: spin -> k -> direction -> KS_basis1 -> KS_basis2.
    default_value: "False"
    unit: "eV * A"
    availability: basis_type==lcao
  - name: rpa_outdir
    category: Output information
    type: String
    description: |
      The directory to save files for LibRPA.
    default_value: "\"OUT.librpa\""
    unit: ""
    availability: basis_type==lcao
  - name: out_pchg
    category: Output information
    type: String
    description: |
      Selects electronic states for partial (band-decomposed) charge-density output using a space-separated string of `0`s and `1`s, where `1` selects a state and `0` skips it. Repetition follows the `ocp_set` syntax, for example `1 4*0 5*1 0`; the expanded list must not exceed `nbands`. Each output represents a complete one-particle state rather than its SCF occupation. The spin degeneracy is 2 for `nspin=1` and 1 for `nspin=2` or `nspin=4`. For `nspin=1`, `s1` contains the charge density. For `nspin=2`, `s1` and `s2` contain the spin-up and spin-down charge densities, respectively. For `nspin=4`, `s1`, `s2`, `s3`, and `s4` respectively contain $\rho_0$, $m_x$, $m_y$, and $m_z$. With `if_separate_k=true`, files are named `pchgi[state]s[component]k[kpoint].cube`; otherwise, the weighted k-point sum is named `pchgi[state]s[component].cube`.

      [NOTE] Enabling symmetry may produce unintended partial charge densities because of reduced k-point weights and real-space symmetry operations. If the desired symmetry treatment is uncertain, set `symmetry = -1`. Use the same symmetry setting as in the SCF calculation.
    default_value: none
    unit: ""
    availability: basis_type==pw or (basis_type==lcao and calculation==get_pchg)
  - name: out_wfc_norm
    category: Output information
    type: String
    description: |
      Selects electronic states for real-space wavefunction-modulus output using the selection syntax and complete-state normalization of `out_pchg`. For `nspin=1`, `s1` contains the wavefunction modulus. For `nspin=2`, `s1` and `s2` contain the spin-up and spin-down wavefunction moduli, respectively. For `nspin=4`, `s1` contains the total spinor modulus. Files are named `wfi[state]s[spin]k[kpoint].cube`.
    default_value: none
    unit: ""
    availability: basis_type==pw or (basis_type==lcao and calculation==get_wf)
  - name: out_wfc_re_im
    category: Output information
    type: String
    description: |
      Selects electronic states for real-space wavefunction real- and imaginary-part output using the selection syntax and complete-state normalization of `out_pchg`. For `nspin=1`, `s1` contains the wavefunction. For `nspin=2`, `s1` and `s2` contain the spin-up and spin-down wavefunctions, respectively. For `nspin=4`, `s1` and `s2` contain the upper and lower spinor components, respectively. Files are named `wfi[state]s[spin]k[kpoint][re/im].cube`.
    default_value: none
    unit: ""
    availability: basis_type==pw or (basis_type==lcao and calculation==get_wf)
  - name: if_separate_k
    category: Output information
    type: Boolean
    description: |
      Specifies whether to write partial charge densities for individual k-points or merge them.
    default_value: "false"
    unit: ""
    availability: "(basis_type==pw and out_pchg!=none) or (basis_type==lcao and calculation==get_pchg and gamma_only==0)"
  - name: out_elf
    category: Output information
    type: "Integer \\[Integer\\](optional)"
    description: |
      Whether to output the electron localization function (ELF) in the folder `OUT.${suffix}`. The files are named as
      * nspin = 1:
          * elftot.cube: ${\rm{ELF}} = \frac{1}{1+\chi^2}$, $\chi = \frac{\frac{1}{2}\sum_{i}{f_i |\nabla\psi_{i}|^2} - \frac{|\nabla\rho|^2}{8\rho}}{\frac{3}{10}(3\pi^2)^{2/3}\rho^{5/3}}$;
      * nspin = 2:
          * elfs1.cube, elfs2.cube: ${\rm{ELF}}_\sigma = \frac{1}{1+\chi_\sigma^2}$, $\chi_\sigma = \frac{\frac{1}{2}\sum_{i}{f_i |\nabla\psi_{i,\sigma}|^2} - \frac{|\nabla\rho_\sigma|^2}{8\rho_\sigma}}{\frac{3}{10}(6\pi^2)^{2/3}\rho_\sigma^{5/3}}$;
          * elftot.cube: ${\rm{ELF}} = \frac{1}{1+\chi^2}$, $\chi = \frac{\frac{1}{2}\sum_{i,\sigma}{f_i |\nabla\psi_{i,\sigma}|^2} - \sum_{\sigma}{\frac{|\nabla\rho_\sigma|^2}{8\rho_\sigma}}}{\sum_{\sigma}{\frac{3}{10}(6\pi^2)^{2/3}\rho_\sigma^{5/3}}}$;
      * nspin = 4 (noncollinear):
          * elftot.cube: ELF for total charge density, ${\rm{ELF}} = \frac{1}{1+\chi^2}$, $\chi = \frac{\frac{1}{2}\sum_{i}{f_i |\nabla\psi_{i}|^2} - \frac{|\nabla\rho|^2}{8\rho}}{\frac{3}{10}(3\pi^2)^{2/3}\rho^{5/3}}$

      When `out_freq_ion > 0`, a geometry step suffix `g{#}` is appended to the file names (e.g., `elftotg1.cube`, `elfs1g1.cube`).

      The second integer controls the precision of the kinetic energy density output, if not given, will use 3 as default. For purpose restarting from this file and other high-precision involved calculation, recommend to use 10.

      In molecular dynamics calculations, the output frequency is controlled by out_freq_ion.
    default_value: 0 3
    unit: ""
    availability: "esolver_type in [ksdft, ofdft]"
  - name: out_spillage
    category: Output information
    type: Integer
    description: |
      This output is only intentively needed by the ABACUS numerical atomic orbital generation workflow. This parameter is used to control whether to output the overlap integrals between truncated spherical Bessel functions (TSBFs) and plane-wave basis expanded wavefunctions (named as OVERLAP_Q), and between TSBFs (named as OVERLAP_Sq), also their first order derivatives. The output files are named starting with orb_matrix. A value of 2 would enable the output.
    default_value: "0"
    unit: ""
    availability: esolver_type==ksdft and basis_type==pw
  - name: out_dipole
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Boolean
    description: |
      Controls electric-dipole output. In RT-TDDFT, each enabled spin channel is written to OUT.{suffix}/dipole_s[spin].txt using a one-based spin number. Every row contains the one-based electronic-step index followed by the Cartesian electronic-dipole components $P_x$, $P_y$, and $P_z$ in atomic units. The running log additionally reports the electronic, ionic, and total dipoles and the norm of the total dipole.
      * True: Output the electric dipole information.
      * False: Do not output the electric dipole information.
    default_value: "False"
    unit: ""
    availability: ""
  - name: out_current
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Integer
    description: |
      Controls the current-density output method for LCAO RT-TDDFT. Output rows contain the one-based electronic-step index followed by $J_x$, $J_y$, and $J_z$ in atomic units.
      * 0: Do not output current.
      * 1: Explicitly construct the velocity operator from the momentum, vector-potential, and KB nonlocal-pseudopotential terms using two-center and spherical-grid integrals: $\hat{v}_{\alpha}=-\mathrm{i}\nabla_{\alpha}+A_{\alpha}(t)+\mathrm{i}\left[\widetilde{V}_{\mathrm{NL}}^{\mathrm{KB}},r_{\alpha}\right]$, where $\widetilde{V}_{\mathrm{NL}}^{\mathrm{KB}}=\mathrm{e}^{-\mathrm{i}\boldsymbol{A}(t)\cdot\boldsymbol{r}}\hat{V}_{\mathrm{NL}}^{\mathrm{KB}}\mathrm{e}^{\mathrm{i}\boldsymbol{A}(t)\cdot\boldsymbol{r}}$. $\boldsymbol{A}(t)$ is nonzero only for the velocity gauge (td_stype=1); otherwise $\boldsymbol{A}(t)=0$. Other nonlocal Hamiltonian terms, such as EXX, are not included explicitly. The total current is written to OUT.{suffix}/current_tot.txt.
      * 2: Use the full Hamiltonian to construct the generalized velocity matrix in a nonorthogonal NAO basis, $\widetilde{v}_{\alpha}=\partial_{\alpha}H+\mathrm{i}HS^{-1}\mathcal{R}_{\alpha}-\mathrm{i}\mathcal{R}_{\alpha}S^{-1}H-HS^{-1}\partial_{\alpha}S$. This includes all contributions available in the real-space Hamiltonian matrix when enabled. This method is more general but more expensive. The total current is written to OUT.{suffix}/current_tot_comm.txt.
    default_value: "0"
    unit: ""
    availability: basis_type==lcao and esolver_type==tddft
  - name: out_current_k
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Boolean
    description: |
      Controls whether LCAO RT-TDDFT current density is also resolved by spin and k-point. The total-current file is always written when out_current is 1 or 2.
      * True: In addition to the total, out_current=1 writes OUT.{suffix}/current_s[spin]k[kpoint].txt; out_current=2 writes OUT.{suffix}/current_s[spin]k[kpoint]_comm.txt. Both use one-based spin and k-point numbers, with k-points numbered independently within each spin channel. Each row contains the one-based electronic-step index followed by $J_x$, $J_y$, and $J_z$ in atomic units.
      * False: Output only current_tot.txt for out_current=1 or current_tot_comm.txt for out_current=2.
    default_value: "False"
    unit: ""
    availability: "basis_type==lcao and esolver_type==tddft and out_current>0"
  - name: out_efield
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Boolean
    description: |
      Controls time-dependent electric-field output. For each configured field, OUT.{suffix}/efield_[index].txt contains two columns: physical time in fs and the field value in V/Angstrom. The one-based field index follows the occurrence order shared by td_ttype and td_vext_dire, so fields assigned to the same direction remain in separate files. At initialization, a fresh calculation with md_restart=False truncates the files corresponding to the currently configured fields, whereas a calculation with md_restart=True preserves them and appends new samples.
      * True: Output electric-field values on active electronic steps.
      * False: Do not output electric-field values.
    default_value: "False"
    unit: ""
    availability: esolver_type==tddft and td_vext==true
  - name: out_vecpot
    category: "RT-TDDFT: Real-Time Time-Dependent Density Functional Theory"
    type: Boolean
    description: |
      Controls Cartesian vector-potential output for LCAO RT-TDDFT. OUT.{suffix}/vector_pot.txt contains four columns: the one-based electronic-step index followed by $A_x$, $A_y$, and $A_z$ in atomic units. At initialization, a fresh calculation with md_restart=False truncates the file and writes a new header, whereas a calculation with md_restart=True preserves a nonempty existing file and appends new samples. If the restart output file is missing or empty, a new file with a header is created.
      * True: Write vector-potential samples on electronic propagation steps.
      * False: Do not output the vector potential.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao and esolver_type==tddft
  - name: cal_symm_repr
    category: System variables
    type: "Integer \\[Integer\\](optional)"
    description: |
      Whether to print the matrix representation of symmetry operation to running log file. If the first value is given as 1, then all matrix representations will be printed. The second optional parameter controls the precision (number of digits) to print, default is 3, which is enough for a quick check.
    default_value: 1 3
    unit: ""
    availability: ""
  - name: spillage_outdir
    category: Input files
    type: String
    description: |
      The directory to save the spillage files.
    default_value: "\"./\""
    unit: ""
    availability: basis_type==pw
  - name: dos_edelta_ev
    category: Density of states
    type: Real
    description: |
      The step size in writing Density of States (DOS)
    default_value: "0.01"
    unit: eV
    availability: ""
  - name: dos_sigma
    category: Density of states
    type: Real
    description: |
      The width of the Gaussian factor when obtaining smeared Density of States (DOS)
    default_value: "0.07"
    unit: eV
    availability: ""
  - name: dos_scale
    category: Density of states
    type: Real
    description: |
      Defines the energy range of DOS output as (emax-emin)*(1+dos_scale), centered at (emax+emin)/2. This parameter will be used when dos_emin and dos_emax are not set.
    default_value: "0.01"
    unit: eV
    availability: ""
  - name: dos_emin_ev
    category: Density of states
    type: Real
    description: |
      The minimal range for Density of States (DOS)
      * If set, "dos_scale" will be ignored.
    default_value: Minimal eigenenergy of
    unit: eV
    availability: ""
  - name: dos_emax_ev
    category: Density of states
    type: Real
    description: |
      The maximal range for Density of States (DOS)
      * If set, "dos_scale" will be ignored.
    default_value: Maximal eigenenergy of
    unit: eV
    availability: ""
  - name: dos_nche
    category: Density of states
    type: Integer
    description: |
      The order of Chebyshev expansions when using Stochastic Density Functional Theory (SDFT) to calculate DOS.
    default_value: "100"
    unit: ""
    availability: ""
  - name: stm_bias
    category: Density of states
    type: Real Real(optional) Integer(optional)
    description: |
      The bias voltage used to calculate local density of states to simulate scanning tunneling microscope, see details in out_ldos. When using three parameters:

      * The first parameter specifies the initial bias voltage value.
      * The second parameter defines the voltage increment (step size between consecutive bias values).
      * The third parameter determines the total number of voltage points
    default_value: "1.0"
    unit: V
    availability: ""
  - name: ldos_line
    category: Density of states
    type: "Real*6 Integer(optional)"
    description: |
      Specify the path of the three-dimensional space and display LDOS in the form of a two-dimensional color chart, see details in out_ldos. The first three paramenters are the direct coordinates of the start point, the next three paramenters are the direct coordinates of the end point, and the final one is the number of points along the path, whose default is 100.
    default_value: 0.0 0.0 0.0 0.0 0.0 1.0 100
    unit: ""
    availability: ""
  - name: cal_cond
    category: Electronic conductivities
    type: Boolean
    description: |
      Whether to calculate electronic conductivities.
    default_value: "False"
    unit: ""
    availability: basis_type==pw
  - name: cond_che_thr
    category: Electronic conductivities
    type: Real
    description: |
      Control the error of Chebyshev expansions for conductivities.
    default_value: "1e-8"
    unit: ""
    availability: esolver_type==sdft
  - name: cond_dw
    category: Electronic conductivities
    type: Real
    description: |
      Frequency interval () for frequency-dependent conductivities.
    default_value: "0.1"
    unit: eV
    availability: basis_type==pw
  - name: cond_wcut
    category: Electronic conductivities
    type: Real
    description: |
      Cutoff frequency for frequency-dependent conductivities.
    default_value: "10.0"
    unit: eV
    availability: basis_type==pw
  - name: cond_dt
    category: Electronic conductivities
    type: Real
    description: |
      Time interval () to integrate Onsager coefficients.
    default_value: "0.02"
    unit: a.u.
    availability: basis_type==pw
  - name: cond_dtbatch
    category: Electronic conductivities
    type: Integer
    description: |
      exp(iH\dt\cond_dtbatch) is expanded with Chebyshev expansion to calculate conductivities. It is faster but costs more memory.
      * If cond_dtbatch = 0: Autoset this parameter to make expansion orders larger than 100.
    default_value: "0"
    unit: ""
    availability: esolver_type==sdft
  - name: cond_smear
    category: Electronic conductivities
    type: Integer
    description: |
      Smearing method for conductivities
      * 1: Gaussian smearing
      * 2: Lorentzian smearing
    default_value: "1"
    unit: ""
    availability: ""
  - name: cond_fwhm
    category: Electronic conductivities
    type: Real
    description: |
      FWHM for conductivities. For Gaussian smearing, ; for Lorentzian smearing, .
    default_value: "0.4"
    unit: eV
    availability: basis_type==pw
  - name: cond_nonlocal
    category: Electronic conductivities
    type: Boolean
    description: |
      Whether to consider nonlocal potential correction when calculating velocity matrix .
      * True: .
      * False: .
    default_value: "True"
    unit: ""
    availability: basis_type==pw
  - name: berry_phase
    category: Berry phase and wannier90 interface
    type: Boolean
    description: |
      Controls the calculation of Berry phase
      * true: Calculate Berry phase.
      * false: Do not calculate Berry phase.
    default_value: "false"
    unit: ""
    availability: ""
  - name: gdir
    category: Berry phase and wannier90 interface
    type: Integer
    description: |
      The direction of the polarization in the lattice vector for Berry phase calculation
      * 1: Calculate the polarization in the direction of the lattice vector a_1 defined in the STRU file.
      * 2: Calculate the polarization in the direction of the lattice vector a_2 defined in the STRU file.
      * 3: Calculate the polarization in the direction of the lattice vector a_3 defined in the STRU file.
    default_value: "3"
    unit: ""
    availability: ""
  - name: towannier90
    category: Berry phase and wannier90 interface
    type: Boolean
    description: |
      Controls the generation of files for the Wannier90 code.
      * 1: Generate files for the Wannier90 code.
      * 0: Do not generate files for the Wannier90 code.
    default_value: "0"
    unit: ""
    availability: ""
  - name: nnkpfile
    category: Berry phase and wannier90 interface
    type: String
    description: |
      The file name generated when running "wannier90 -pp ..." command
    default_value: seedname.nnkp
    unit: ""
    availability: ""
  - name: wannier_method
    category: Berry phase and wannier90 interface
    type: Integer
    description: |
      Only available on LCAO basis, using different methods to generate "\.mmn" file and "\.amn" file.
      * 1: Calculated using the lcao_in_pw method, the calculation accuracy can be improved by increasing ecutwfc to maintain consistency with the pw basis set results.
      * 2: The overlap between atomic orbitals is calculated using grid integration. The radial grid points are generated using the Gauss-Legendre method, while the spherical grid points are generated using the Lebedev-Laikov method.
    default_value: "1"
    unit: ""
    availability: ""
  - name: wannier_spin
    category: Berry phase and wannier90 interface
    type: String
    description: |
      The spin direction for the Wannier function calculation when nspin is set to 2
      * up: Calculate spin up for the Wannier function.
      * down: Calculate spin down for the Wannier function.
    default_value: up
    unit: ""
    availability: ""
  - name: out_wannier_mmn
    category: Berry phase and wannier90 interface
    type: Boolean
    description: |
      Write the "*.mmn" file or not.
      * 0: don't write the "*.mmn" file.
      * 1: write the "*.mmn" file.
    default_value: "1"
    unit: ""
    availability: ""
  - name: out_wannier_amn
    category: Berry phase and wannier90 interface
    type: Boolean
    description: |
      Write the "*.amn" file or not.
      * 0: don't write the "*.amn" file.
      * 1: write the "*.amn" file.
    default_value: "1"
    unit: ""
    availability: ""
  - name: out_wannier_eig
    category: Berry phase and wannier90 interface
    type: Boolean
    description: |
      Write the "*.eig" file or not.
      * 0: don't write the "*.eig" file.
      * 1: write the "*.eig" file.
    default_value: "1"
    unit: ""
    availability: ""
  - name: out_wannier_unk
    category: Berry phase and wannier90 interface
    type: Boolean
    description: |
      Write the "UNK.*" file or not.
      * 0: don't write the "UNK.*" file.
      * 1: write the "UNK.*" file.
    default_value: "0"
    unit: ""
    availability: ""
  - name: out_wannier_wvfn_formatted
    category: Berry phase and wannier90 interface
    type: Boolean
    description: |
      Write the "UNK.*" file in ASCII format or binary format.
      * 0: write the "UNK.*" file in binary format.
      * 1: write the "UNK.*" file in ASCII format (text file format).
    default_value: "1"
    unit: ""
    availability: ""
  - name: efield_flag
    category: Electric field and dipole correction
    type: Boolean
    description: |
      Added the electric field.
      * True: A saw-like potential simulating an electric field is added to the bare ionic potential.
      * False: Not added the electric field.
    default_value: "False"
    unit: ""
    availability: ""
  - name: dip_cor_flag
    category: Electric field and dipole correction
    type: Boolean
    description: |
      Added a dipole correction to the bare ionic potential.
      * True: A dipole correction is also added to the bare ionic potential.
      * False: A dipole correction is not added to the bare ionic potential.

      [NOTE] Note: If you do not want any electric field, the parameter efield_amp should be set to zero. This should ONLY be used in a slab geometry for surface calculations, with the discontinuity FALLING IN THE EMPTY SPACE.
    default_value: "False"
    unit: ""
    availability: efield_flag==true
  - name: efield_dir
    category: Electric field and dipole correction
    type: Integer
    description: |
      The direction of the electric field or dipole correction is parallel to the reciprocal lattice vector, so the potential is constant in planes defined by FFT grid points, efield_dir can set to 0, 1 or 2.
      * 0: parallel to the first reciprocal lattice vector
      * 1: parallel to the second reciprocal lattice vector
      * 2: parallel to the third reciprocal lattice vector
    default_value: "2"
    unit: ""
    availability: efield_flag==true
  - name: efield_pos_max
    category: Electric field and dipole correction
    type: Real
    description: |
      Position of the maximum of the saw-like potential along crystal axis efield_dir, within the unit cell, 0 <= efield_pos_max < 1.
    default_value: Autoset to center of vacuum - width of vacuum / 20
    unit: ""
    availability: efield_flag==true
  - name: efield_pos_dec
    category: Electric field and dipole correction
    type: Real
    description: |
      Zone in the unit cell where the saw-like potential decreases, 0 < efield_pos_dec < 1.
    default_value: Autoset to width of vacuum / 10
    unit: ""
    availability: efield_flag==true
  - name: efield_amp
    category: Electric field and dipole correction
    type: Real
    description: |
      Amplitude of the electric field. The saw-like potential increases with slope efield_amp in the region from efield_pos_max+efield_pos_dec-1) to (efield_pos_max), then decreases until (efield_pos_max+efield_pos_dec), in units of the crystal vector efield_dir.

      [NOTE] Note: The change of slope of this potential must be located in the empty region, or else unphysical forces will result.
    default_value: "0.0"
    unit: "a.u., 1 a.u. = 51.4220632*10^10 V/m."
    availability: efield_flag==true
  - name: gate_flag
    category: Gate field (compensating charge)
    type: Boolean
    description: |
      Controls the addition of compensating charge by a charged plate for charged cells.
      * true: A charged plate is placed at the zgate position to add compensating charge. The direction is determined by efield_dir.
      * false: No compensating charge is added.
    default_value: "false"
    unit: ""
    availability: ""
  - name: zgate
    category: Gate field (compensating charge)
    type: Real
    description: |
      Position of the charged plate in the unit cell
    default_value: "0.5"
    unit: Unit cell size
    availability: ""
  - name: block
    category: Gate field (compensating charge)
    type: Boolean
    description: |
      Controls the addition of a potential barrier to prevent electron spillover.
      * true: A potential barrier is added from block_down to block_up with a height of block_height. If dip_cor_flag is set to true, efield_pos_dec is used to smoothly increase and decrease the potential barrier.
      * false: No potential barrier is added.
    default_value: "false"
    unit: ""
    availability: ""
  - name: block_down
    category: Gate field (compensating charge)
    type: Real
    description: |
      Lower beginning of the potential barrier
    default_value: "0.45"
    unit: Unit cell size
    availability: ""
  - name: block_up
    category: Gate field (compensating charge)
    type: Real
    description: |
      Upper beginning of the potential barrier
    default_value: "0.55"
    unit: Unit cell size
    availability: ""
  - name: block_height
    category: Gate field (compensating charge)
    type: Real
    description: |
      Height of the potential barrier
    default_value: "0.1"
    unit: Rydberg
    availability: ""
  - name: imp_sol
    category: Implicit solvation model
    type: Boolean
    description: |
      Calculate implicit solvation correction
    default_value: "False"
    unit: ""
    availability: ""
  - name: eb_k
    category: Implicit solvation model
    type: Real
    description: |
      The relative permittivity of the bulk solvent, 80 for water
    default_value: "80"
    unit: ""
    availability: imp_sol==true
  - name: tau
    category: Implicit solvation model
    type: Real
    description: |
      The effective surface tension parameter that describes the cavitation, the dispersion, and the repulsion interaction between the solute and the solvent which are not captured by the electrostatic terms
    default_value: "1.0798e-05"
    unit: ""
    availability: ""
  - name: sigma_k
    category: Implicit solvation model
    type: Real
    description: |
      The width of the diffuse cavity that is implicitly determined by the electronic structure of the solute
    default_value: "0.6"
    unit: ""
    availability: ""
  - name: nc_k
    category: Implicit solvation model
    type: Real
    description: |
      The value of the electron density at which the dielectric cavity forms
    default_value: "0.00037"
    unit: ""
    availability: ""
  - name: vdw_method
    category: vdW correction
    type: String
    description: |
      Specifies the method used for Van der Waals (VdW) correction. Available options are:
      * d2: Grimme's D2 dispersion correction method
      * d3_0: Grimme's DFT-D3(0) dispersion correction method (zero-damping)
      * d3_bj: Grimme's DFTD3(BJ) dispersion correction method (BJ-damping)
      * d4: Grimme's DFT-D4 dispersion correction method using the external DFT-D4 library
      * none: no vdW correction

      [NOTE] ABACUS supports automatic setting of DFT-D3 parameters for common functionals. To benefit from this feature, please specify the parameter dft_functional explicitly, otherwise the autoset procedure will crash. If not satisfied with the built-in parameters, any manual setting on vdw_s6, vdw_s8, vdw_a1 and vdw_a2 will overwrite the automatic values.
    default_value: none
    unit: ""
    availability: ""
  - name: vdw_d4_xc
    category: vdW correction
    type: String
    description: |
      Functional name used to load DFT-D4 damping parameters from the DFT-D4 library.
      If set to default, ABACUS infers the functional name from dft_functional or pseudopotential metadata.
    default_value: default
    unit: ""
    availability: vdw_method==d4
  - name: vdw_d4_model
    category: vdW correction
    type: String
    description: |
      DFT-D4 dispersion model used by the external DFT-D4 library.
      Available options are:
      * d4: standard D4 model
      * d4s: smooth D4S model
    default_value: "d4"
    unit: ""
    availability: vdw_method==d4
  - name: vdw_s6
    category: vdW correction
    type: String
    description: |
      This scale factor is used to optimize the interaction energy deviations in van der Waals (vdW) corrected calculations. The recommended values of this parameter are dependent on the chosen vdW correction method and the DFT functional being used. For DFT-D2, the recommended values are 0.75 (PBE), 1.2 (BLYP), 1.05 (B-P86), 1.0 (TPSS), and 1.05 (B3LYP). If not set, will use values of PBE functional. For DFT-D3, recommended values with different DFT functionals can be found on the here. If not set, will search in ABACUS built-in dataset based on the dft_functional keywords. User set value will overwrite the searched value.
    default_value: ""
    unit: ""
    availability: "vdw_method in [d2, d3_0, d3_bj]"
  - name: vdw_s8
    category: vdW correction
    type: String
    description: |
      This scale factor is relevant for D3(0) and D3(BJ) van der Waals (vdW) correction methods. The recommended values of this parameter with different DFT functionals can be found on the webpage. If not set, will search in ABACUS built-in dataset based on the dft_functional keywords. User set value will overwrite the searched value.
    default_value: ""
    unit: ""
    availability: "vdw_method in [d3_0, d3_bj]"
  - name: vdw_a1
    category: vdW correction
    type: String
    description: |
      This damping function parameter is relevant for D3(0) and D3(BJ) van der Waals (vdW) correction methods. The recommended values of this parameter with different DFT functionals can be found on the webpage. If not set, will search in ABACUS built-in dataset based on the dft_functional keywords. User set value will overwrite the searched value.
    default_value: ""
    unit: ""
    availability: "vdw_method in [d3_0, d3_bj]"
  - name: vdw_a2
    category: vdW correction
    type: String
    description: |
      This damping function parameter is only relevant for D3(0) and D3(BJ) van der Waals (vdW) correction methods. The recommended values of this parameter with different DFT functionals can be found on the webpage. If not set, will search in ABACUS built-in dataset based on the dft_functional keywords. User set value will overwrite the searched value.
    default_value: ""
    unit: ""
    availability: "vdw_method in [d3_0, d3_bj]"
  - name: vdw_d
    category: vdW correction
    type: Real
    description: |
      Controls the damping rate of the damping function in the DFT-D2 method.
    default_value: "20"
    unit: ""
    availability: vdw_method==d2
  - name: vdw_abc
    category: vdW correction
    type: Boolean
    description: |
      Determines whether three-body terms are calculated for DFT-D3 methods.
      * True: ABACUS will calculate the three-body term.
      * False: The three-body term is not included.
    default_value: "False"
    unit: ""
    availability: "vdw_method in [d3_0, d3_bj]"
  - name: vdw_c6_file
    category: vdW correction
    type: String
    description: |
      Specifies the name of the file containing parameters for each element when using the D2 method. If not set, ABACUS uses the default parameters (Jnm6/mol) stored in the program. To manually set the parameters, provide a file containing the parameters. An example is given by:

      H 0.1 Si 9.0

      Namely, each line contains the element name and the corresponding parameter.
    default_value: default
    unit: ""
    availability: vdw_method==d2
  - name: vdw_c6_unit
    category: vdW correction
    type: String
    description: |
      Specifies the unit of the provided parameters in the D2 method. Available options are:
      * Jnm6/mol (J nm^6/mol)
      * eVA (eV Angstrom)
    default_value: Jnm6/mol
    unit: ""
    availability: "vdw_method==d2 and vdw_c6_file!=default"
  - name: vdw_r0_file
    category: vdW correction
    type: String
    description: |
      Specifies the name of the file containing parameters for each element when using the D2 method. If not set, ABACUS uses the default parameters (Angstrom) stored in the program. To manually set the parameters, provide a file containing the parameters. An example is given by:

      Li 1.0 Cl 2.0

      Namely, each line contains the element name and the corresponding parameter.
    default_value: default
    unit: ""
    availability: vdw_method==d2
  - name: vdw_r0_unit
    category: vdW correction
    type: String
    description: |
      Specifies the unit for the parameters in the D2 method when manually set by the user. Available options are:
      * A (Angstrom)
      * Bohr
    default_value: "A"
    unit: ""
    availability: "vdw_method==d2 and vdw_r0_file!=default"
  - name: vdw_cutoff_type
    category: vdW correction
    type: String
    description: |
      Determines the method used for specifying the cutoff radius in periodic systems when applying Van der Waals correction. Available options are:
      * radius: The supercell is selected within a sphere centered at the origin with a radius defined by vdw_cutoff_radius.
      * period: The extent of the supercell is explicitly specified using the vdw_cutoff_period keyword.
    default_value: radius
    unit: ""
    availability: ""
  - name: vdw_cutoff_radius
    category: vdW correction
    type: String
    description: |
      Defines the radius of the cutoff sphere when vdw_cutoff_type is set to radius. The default values depend on the chosen vdw_method.
    default_value: ""
    unit: defined by vdw_radius_unit (default Bohr)
    availability: vdw_cutoff_type==radius
  - name: vdw_radius_unit
    category: vdW correction
    type: String
    description: |
      Specify the unit of vdw_cutoff_radius. Available options are:
      * A(Angstrom)
      * Bohr
    default_value: Bohr
    unit: ""
    availability: vdw_cutoff_type==radius
  - name: vdw_cutoff_width2
    category: vdW correction
    type: Real
    description: |
      Width of the smooth switching region for the two-body pairwise dispersion real-space cutoff.
      A value of zero disables smoothing for the two-body contribution.
    default_value: "0.05"
    unit: Bohr
    availability: vdw_method==d4
  - name: vdw_cutoff_width3
    category: vdW correction
    type: Real
    description: |
      Width of the smooth switching region for the three-body Axilrod-Teller-Muto (ATM) dispersion real-space cutoff.
      A value of zero disables smoothing for the three-body contribution.
    default_value: "0.05"
    unit: Bohr
    availability: vdw_method==d4
  - name: vdw_cutoff_period
    category: vdW correction
    type: Integer Integer Integer
    description: |
      The three integers supplied here explicitly specify the extent of the supercell in the directions of the three basis lattice vectors.
    default_value: 3 3 3
    unit: ""
    availability: vdw_cutoff_type==period
  - name: vdw_cn_thr
    category: vdW correction
    type: Real
    description: |
      The cutoff radius when calculating coordination numbers.
    default_value: "40"
    unit: "defined by vdw_cn_thr_unit (default: Bohr)"
    availability: "vdw_method in [d3_0, d3_bj, d4]"
  - name: vdw_cn_thr_unit
    category: vdW correction
    type: String
    description: |
      Unit of the coordination number cutoff (vdw_cn_thr). Available options are:
      * A(Angstrom)
      * Bohr
    default_value: Bohr
    unit: ""
    availability: ""
  - name: exx_fock_alpha
    category: Exact Exchange (Common)
    type: Real
    description: |
      Fraction of full-ranged Fock exchange $1/r$ in range-separated hybrid functionals.
    default_value: see hybrid_func_params
    unit: ""
    availability: ""
  - name: exx_erfc_alpha
    category: Exact Exchange (Common)
    type: Real
    description: |
      Fraction of short-ranged Fock exchange $\mathrm{erfc}(\omega r)/r$ in range-separated hybrid functionals.
    default_value: see hybrid_func_params
    unit: ""
    availability: ""
  - name: exx_erfc_omega
    category: Exact Exchange (Common)
    type: Real
    description: |
      Range-separation parameter $\omega$ in the short-ranged Fock term $\mathrm{erfc}(\omega r)/r$.
    default_value: see hybrid_func_params
    unit: ""
    availability: ""
  - name: exx_separate_loop
    category: Exact Exchange (Common)
    type: Boolean
    description: |
      There are two types of iterative approaches provided by ABACUS to evaluate Fock exchange.
      * False: Start with a GGA-Loop, and then Hybrid-Loop, in which EXX Hamiltonian is updated with electronic iterations.
      * True: A two-step method is employed, i.e. in the inner iterations, density matrix is updated, while in the outer iterations, is calculated based on density matrix that converges in the inner iteration.
    default_value: "True"
    unit: ""
    availability: ""
  - name: exx_hybrid_step
    category: Exact Exchange (Common)
    type: Integer
    description: |
      The maximal iteration number of the outer-loop, where the Fock exchange is calculated
    default_value: "100"
    unit: ""
    availability: exx_separate_loop==1
  - name: exx_mixing_beta
    category: Exact Exchange (Common)
    type: Real
    description: |
      Mixing parameter for densty matrix in each iteration of the outer-loop
    default_value: "1.0"
    unit: ""
    availability: exx_separate_loop==1
  - name: exx_fock_lambda
    category: Exact Exchange (LCAO in PW)
    type: Real
    description: |
      It is used to compensate for divergence points at G=0 in the evaluation of Fock exchange using lcao_in_pw method.
    default_value: "0.3"
    unit: ""
    availability: basis_type==lcao_in_pw
  - name: exx_pca_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      To accelerate the evaluation of four-center integrals (), the product of atomic orbitals are expanded in the basis of auxiliary basis functions (ABF): . The size of the ABF (i.e. number of ) is reduced using principal component analysis. When a large PCA threshold is used, the number of ABF will be reduced, hence the calculation becomes faster. However, this comes at the cost of computational accuracy. A relatively safe choice of the value is 1e-4.
    default_value: "1E-4"
    unit: ""
    availability: ""
  - name: exx_c_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      See also the entry exx_pca_threshold. Smaller components (less than exx_c_threshold) of the matrix are neglected to accelerate calculation. The larger the threshold is, the faster the calculation and the lower the accuracy. A relatively safe choice of the value is 1e-4.
    default_value: "1E-4"
    unit: ""
    availability: ""
  - name: exx_cs_inv_thr
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      By default, the Coulomb matrix inversion required for obtaining LRI coefficients is performed using LU decomposition. However, this approach may suffer from numerical instabilities when a large set of auxiliary basis functions (ABFs) is employed. When exx_cs_inv_thr > 0, the inversion is instead carried out via matrix diagonalization. Eigenvalues smaller than exx_cs_inv_thr are discarded to improve numerical stability. A relatively safe and commonly recommended value is 1e-5.
    default_value: "-1"
    unit: ""
    availability: ""
  - name: exx_v_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      See also the entry exx_pca_threshold. With the approximation , the four-center integral in Fock exchange is expressed as , where is a double-center integral. Smaller values of the V matrix can be truncated to accelerate calculation. The larger the threshold is, the faster the calculation and the lower the accuracy. A relatively safe choice of the value is 0, i.e. no truncation.
    default_value: "1E-1"
    unit: ""
    availability: ""
  - name: exx_dm_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      The Fock exchange can be expressed as where D is the density matrix. Smaller values of the density matrix can be truncated to accelerate calculation. The larger the threshold is, the faster the calculation and the lower the accuracy. A relatively safe choice of the value is 1e-4.
    default_value: "1E-4"
    unit: ""
    availability: ""
  - name: exx_c_grad_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      See also the entry exx_pca_threshold. is used in force. Smaller components (less than exx_c_grad_threshold) of the matrix are neglected to accelerate calculation. The larger the threshold is, the faster the calculation and the lower the accuracy. A relatively safe choice of the value is 1e-4.
    default_value: "1E-4"
    unit: ""
    availability: ""
  - name: exx_v_grad_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      See also the entry exx_pca_threshold. With the approximation , the four-center integral in Fock exchange is expressed as , where is a double-center integral. is used in force. Smaller values of the V matrix can be truncated to accelerate calculation. The larger the threshold is, the faster the calculation and the lower the accuracy. A relatively safe choice of the value is 0, i.e. no truncation.
    default_value: "1E-1"
    unit: ""
    availability: ""
  - name: exx_c_grad_r_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      See also the entry exx_pca_threshold. is used in stress. Smaller components (less than exx_c_grad_r_threshold) of the matrix are neglected to accelerate calculation. The larger the threshold is, the faster the calculation and the lower the accuracy. A relatively safe choice of the value is 1e-4.
    default_value: "1E-4"
    unit: ""
    availability: ""
  - name: exx_v_grad_r_threshold
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      See also the entry exx_pca_threshold. With the approximation , the four-center integral in Fock exchange is expressed as , where is a double-center integral. is used in force and stress. Smaller values of the V matrix can be truncated to accelerate calculation. The larger the threshold is, the faster the calculation and the lower the accuracy. A relatively safe choice of the value is 0, i.e. no truncation.
    default_value: "1E-1"
    unit: ""
    availability: ""
  - name: exx_ccp_rmesh_times
    category: Exact Exchange (LCAO)
    type: String
    description: |
      This parameter determines how many times larger the radial mesh required for calculating Columb potential is to that of atomic orbitals. The value should be larger than 0. Reducing this value can effectively increase the speed of self-consistent calculations using hybrid functionals.
    default_value: ""
    unit: ""
    availability: ""
  - name: exx_opt_orb_lmax
    category: Exact Exchange (LCAO)
    type: Integer
    description: |
      The maximum l of the spherical Bessel functions, when the radial part of opt-ABFs are generated as linear combinations of spherical Bessel functions. A reasonable choice is 2.
    default_value: "0"
    unit: ""
    availability: calculation==gen_opt_abfs
  - name: exx_opt_orb_ecut
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      The cut-off of plane wave expansion, when the plane wave basis is used to optimize the radial ABFs. A reasonable choice is 60.
    default_value: "0"
    unit: Ry
    availability: calculation==gen_opt_abfs
  - name: exx_opt_orb_tolerence
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      The threshold when solving for the zeros of spherical Bessel functions. A reasonable choice is 1e-12.
    default_value: "1E-12"
    unit: ""
    availability: calculation==gen_opt_abfs
  - name: exx_real_number
    category: Exact Exchange (LCAO)
    type: String
    description: |
      * True: Enforce LibRI to use double data type.
      * False: Enforce LibRI to use complex data type. Setting it to True can effectively improve the speed of self-consistent calculations with hybrid functionals.
    default_value: depends on the gamma_only option
    unit: ""
    availability: ""
  - name: exx_singularity_correction
    category: Exact Exchange (LCAO)
    type: String
    description: |
      * spencer: see Phys. Rev. B 77, 193110 (2008).
      * revised_spencer: see Phys. Rev. Mater. 5, 013807 (2021). Set the scheme of Coulomb singularity correction.
    default_value: default
    unit: ""
    availability: ""
  - name: rpa_ccp_rmesh_times
    category: Exact Exchange (LCAO)
    type: Real
    description: |
      How many times larger the radial mesh required is to that of atomic orbitals in the postprocess calculation of the bare Coulomb matrix for RPA, GW, etc.
    default_value: "10"
    unit: ""
    availability: ""
  - name: exx_symmetry_realspace
    category: Exact Exchange (LCAO)
    type: Boolean
    description: |
      * False: only rotate k-space density matrix D(k) from irreducible k-points to accelerate diagonalization
      * True: rotate both D(k) and Hexx(R) to accelerate both diagonalization and EXX calculation
    default_value: "True"
    unit: ""
    availability: "symmetry==1 and (dft_functional in [hse, hf, pbe0, scan0] or (basis_type==lcao and rpa==true))"
  - name: out_ri_cv
    category: Exact Exchange (LCAO)
    type: Boolean
    description: |
      Whether to output the coefficient tensor C(R) and ABFs-representation Coulomb matrix V(R) for each atom pair and cell in real space.
    default_value: "false"
    unit: ""
    availability: ""
  - name: dft_plus_u
    category: DFT+U correction
    type: Integer
    description: |
      Determines whether to calculate the plus U correction, which is especially important for correlated electrons.
      * 1: Calculate plus U correction with radius-adjustable localized projections (with parameter onsite_radius).
      * 2: Calculate plus U correction using first zeta of NAOs as projections (this is old method for testing).
      * 0: Do not calculate plus U correction.
    default_value: "0"
    unit: ""
    availability: ""
  - name: dft_plus_dmft
    category: DFT+U correction
    type: Boolean
    description: |
      Whether to enable DFT+DMFT calculation. True: DFT+DMFT; False: standard DFT calculation.
    default_value: "False"
    unit: ""
    availability: basis_type==lcao
  - name: orbital_corr
    category: DFT+U correction
    type: Vector of Integer (n values where n is the number of atomic types)
    description: |
      Specifies which orbits need plus U correction for each atom type ( for atom type 1, 2, 3, respectively).
      * -1: The plus U correction will not be calculated for this atom.
      * 1: For p-electron orbits, the plus U correction is needed.
      * 2: For d-electron orbits, the plus U correction is needed.
      * 3: For f-electron orbits, the plus U correction is needed.
    default_value: "-1"
    unit: ""
    availability: ""
  - name: hubbard_u
    category: DFT+U correction
    type: Vector of Real (n values where n is the number of atomic types)
    description: |
      Specifies the Hubbard Coulomb interaction parameter U (eV) in plus U correction, which should be specified for each atom unless the Yukawa potential is used.

      [NOTE] Note: Since only the simplified scheme by Duradev is implemented, the 'U' here is actually U-effective, which is given by Hubbard U minus Hund J.
    default_value: "0.0"
    unit: ""
    availability: ""
  - name: yukawa_potential
    category: DFT+U correction
    type: Boolean
    description: |
      Determines whether to use the local screen Coulomb potential method to calculate the values of U and J.
      * True: hubbard_u does not need to be specified.
      * False: hubbard_u does need to be specified.
    default_value: "False"
    unit: ""
    availability: ""
  - name: yukawa_lambda
    category: DFT+U correction
    type: Real
    description: |
      The screen length of Yukawa potential. If left to default, the screen length will be calculated as an average of the entire system. It's better to stick to the default setting unless there is a very good reason.
    default_value: Calculated on the fly.
    unit: ""
    availability: dft_plus_u==1 and yukawa_potential==true
  - name: uramping
    category: DFT+U correction
    type: Real
    description: |
      Once uramping > 0.15 eV. DFT+U calculations will start SCF with U = 0 eV, namely normal LDA/PBE calculations. Once SCF restarts when drho<mixing_restart, U value will increase by uramping eV. SCF will repeat above calcuations until U values reach target defined in hubbard_u. As for uramping=1.0 eV, the recommendations of mixing_restart is around 5e-4.
    default_value: "-1.0."
    unit: eV
    availability: "dft_plus_u==1 and mixing_restart>0"
  - name: omc
    category: DFT+U correction
    type: Integer
    description: |
      The parameter controls the form of occupation matrix control used.
      * 0: No occupation matrix control is performed, and the onsite density matrix will be calculated from wavefunctions in each SCF step.
      * 1: The first SCF step will use an initial density matrix read from a file named dm_onsite_ini.txt, but for later steps, the onsite density matrix will be updated.
      * 2: The same onsite density matrix from dm_onsite_ini.txt will be used throughout the entire calculation.

      [NOTE] The easiest way to create dm_onsite_ini.txt is to run a DFT+U calculation with out_chg=1, look for a file named dm_onsite.txt in the OUT.prefix directory, copy and rename it to dm_onsite_ini.txt. The file dm_onsite_ini.txt should be placed in the directory specified by read_file_dir. The format of the file is rather straight-forward.
    default_value: "0"
    unit: ""
    availability: ""
  - name: onsite_radius
    category: DFT+U correction
    type: Real
    description: |
      * The onsite_radius parameter facilitates modulation of the single-zeta portion of numerical atomic orbitals used for DFT+U projections.
      * The modulation algorithm applies a smooth truncation to the orbital tail followed by normalization. A representative profile is $f(r)=\frac{1}{2}\left[1+\operatorname{erf}\!\left(\frac{r_c-r}{\sigma}\right)\right]$, where $r_c$ is the cutoff radius and $\sigma=\gamma r_c$ controls smoothness.
    default_value: "3.0"
    unit: Bohr
    availability: dft_plus_u==1
  - name: sc_mag_switch
    category: Spin-Constrained DFT
    type: Boolean
    description: |
      Switch to control spin-constrained DFT calculation
    default_value: "False"
    unit: ""
    availability: ""
  - name: decay_grad_switch
    category: Spin-Constrained DFT
    type: Boolean
    description: |
      Switch to control gradient break condition in spin-constrained DFT
    default_value: "False"
    unit: ""
    availability: ""
  - name: sc_thr
    category: Spin-Constrained DFT
    type: Real
    description: |
      Convergence criterion of spin-constrained iteration (RMS) in uB
    default_value: "1.0e-6"
    unit: uB
    availability: sc_mag_switch==true
  - name: nsc
    category: Spin-Constrained DFT
    type: Integer
    description: |
      Maximal number of spin-constrained iteration
    default_value: "100"
    unit: ""
    availability: sc_mag_switch==true
  - name: nsc_min
    category: Spin-Constrained DFT
    type: Integer
    description: |
      Minimum number of spin-constrained iteration
    default_value: "2"
    unit: ""
    availability: sc_mag_switch==true
  - name: alpha_trial
    category: Spin-Constrained DFT
    type: Real
    description: |
      Initial trial step size for lambda in eV/uB^2
    default_value: "0.01"
    unit: eV/uB^2
    availability: sc_mag_switch==true
  - name: sccut
    category: Spin-Constrained DFT
    type: Real
    description: |
      Maximal step size for lambda in eV/uB
    default_value: "3.0"
    unit: eV/uB
    availability: sc_mag_switch==true
  - name: sc_drop_thr
    category: Spin-Constrained DFT
    type: Real
    description: |
      Convergence criterion ratio of lambda iteration in Spin-constrained DFT
    default_value: "1.0e-2"
    unit: ""
    availability: sc_mag_switch==true
  - name: sc_scf_thr
    category: Spin-Constrained DFT
    type: Real
    description: |
      Density error threshold for inner loop of spin-constrained SCF
    default_value: "1.0e-4"
    unit: ""
    availability: sc_mag_switch==true
  - name: sc_direction_only
    category: Spin-Constrained DFT
    type: Boolean
    description: |
      When true, only the direction of the magnetic moment is constrained to the target direction, while the magnitude is allowed to vary freely. This is useful for studying magnetic anisotropy or when the magnitude of the moment is determined by the electronic structure rather than an external constraint.

      When false (default), both the direction and magnitude of the magnetic moment are constrained to the target values.
    default_value: "False"
    unit: ""
    availability: sc_mag_switch==true
  - name: sc_lambda_strategy
    category: Spin-Constrained DFT
    type: String
    description: |
      Lambda update strategy for spin-constrained DFT:
      * bfgs: BFGS quasi-Newton method
      * linear_response: linear response (Scheme B)
      * augmented_lagrangian: augmented Lagrangian (Scheme C)
      * hybrid_delayed: hybrid delayed update (Scheme D)
      * linear_scan: linear sweep of lambda for testing magnetic moment response
    default_value: bfgs
    unit: ""
    availability: sc_mag_switch==true
  - name: sc_scan_lambda_start
    category: Spin-Constrained DFT
    type: Float
    description: |
      Starting lambda value for linear_scan strategy. Only used when sc_lambda_strategy=linear_scan.
    default_value: "0.0"
    unit: eV/uB
    availability: sc_mag_switch==true and sc_lambda_strategy==linear_scan
  - name: sc_scan_lambda_end
    category: Spin-Constrained DFT
    type: Float
    description: |
      Ending lambda value for linear_scan strategy. Only used when sc_lambda_strategy=linear_scan.
    default_value: "1.0"
    unit: eV/uB
    availability: sc_mag_switch==true and sc_lambda_strategy==linear_scan
  - name: sc_scan_steps
    category: Spin-Constrained DFT
    type: Integer
    description: |
      Number of lambda values to scan. Only used when sc_lambda_strategy=linear_scan.
    default_value: "20"
    unit: ""
    availability: sc_mag_switch==true and sc_lambda_strategy==linear_scan
  - name: qo_switch
    category: Quasiatomic Orbital (QO) analysis
    type: Boolean
    description: |
      Whether to let ABACUS output QO analysis required files
    default_value: "False"
    unit: ""
    availability: ""
  - name: qo_basis
    category: Quasiatomic Orbital (QO) analysis
    type: String
    description: |
      Type of QO basis function:
      * hydrogen: hydrogen-like basis
      * pswfc: read basis from pseudopotential
      * szv: single-zeta valence basis
    default_value: szv
    unit: ""
    availability: ""
  - name: qo_strategy
    category: Quasiatomic Orbital (QO) analysis
    type: Vector of String (1 or n values where n is the number of atomic types)
    description: |
      Strategy to generate radial orbitals for QO analysis. For hydrogen: energy-valence, for pswfc and szv: all
    default_value: "for hydrogen: energy-valence, for pswfc and szv: all"
    unit: ""
    availability: ""
  - name: qo_screening_coeff
    category: Quasiatomic Orbital (QO) analysis
    type: Vector of Real (n values where n is the number of atomic types; 1 value allowed for qo_basis=pswfc)
    description: |
      The screening coefficient for each atom type to rescale the shape of radial orbitals
    default_value: "0.1"
    unit: Bohr^-1
    availability: ""
  - name: qo_thr
    category: Quasiatomic Orbital (QO) analysis
    type: Real
    description: |
      The convergence threshold determining the cutoff of generated orbital. Lower threshold will yield orbital with larger cutoff radius.
    default_value: "1.0e-6"
    unit: ""
    availability: ""
  - name: pexsi_npole
    category: PEXSI
    type: Integer
    description: |
      The number of poles used in the pole expansion method, should be a even number.
    default_value: "40"
    unit: ""
    availability: ""
  - name: pexsi_inertia
    category: PEXSI
    type: Boolean
    description: |
      Whether inertia counting is used at the very beginning.
    default_value: "True"
    unit: ""
    availability: ""
  - name: pexsi_nmax
    category: PEXSI
    type: Integer
    description: |
      Maximum number of PEXSI iterations after each inertia counting procedure.
    default_value: "80"
    unit: ""
    availability: ""
  - name: pexsi_comm
    category: PEXSI
    type: Boolean
    description: |
      Whether to construct PSelInv communication pattern.
    default_value: "True"
    unit: ""
    availability: ""
  - name: pexsi_storage
    category: PEXSI
    type: Boolean
    description: |
      Whether to use symmetric storage space used by the Selected Inversion algorithm for symmetric matrices.
    default_value: "True"
    unit: ""
    availability: ""
  - name: pexsi_ordering
    category: PEXSI
    type: Integer
    description: |
      Ordering strategy for factorization and selected inversion. 0: Parallel ordering using ParMETIS, 1: Sequential ordering using METIS, 2: Multiple minimum degree ordering
    default_value: "0"
    unit: ""
    availability: ""
  - name: pexsi_row_ordering
    category: PEXSI
    type: Integer
    description: |
      Row permutation strategy for factorization and selected inversion, 0: No row permutation, 1: Make the diagonal entry of the matrix larger than the off-diagonal entries.
    default_value: "1"
    unit: ""
    availability: ""
  - name: pexsi_nproc
    category: PEXSI
    type: Integer
    description: |
      Number of processors for PARMETIS. Only used if pexsi_ordering == 0.
    default_value: "1"
    unit: ""
    availability: ""
  - name: pexsi_symm
    category: PEXSI
    type: Boolean
    description: |
      Whether the matrix is symmetric.
    default_value: "True"
    unit: ""
    availability: ""
  - name: pexsi_trans
    category: PEXSI
    type: Boolean
    description: |
      Whether to factorize the transpose of the matrix.
    default_value: "False"
    unit: ""
    availability: ""
  - name: pexsi_method
    category: PEXSI
    type: Integer
    description: |
      The pole expansion method to be used. 1 for Cauchy Contour Integral method, 2 for Moussa optimized method.
    default_value: "1"
    unit: ""
    availability: ""
  - name: pexsi_nproc_pole
    category: PEXSI
    type: Integer
    description: |
      The point parallelizaion of PEXSI. Recommend two points parallelization.
    default_value: "1"
    unit: ""
    availability: ""
  - name: pexsi_temp
    category: PEXSI
    type: Real
    description: |
      Temperature in Fermi-Dirac distribution, in Ry, should have the same effect as the smearing sigma when smearing method is set to Fermi-Dirac.
    default_value: "0.015"
    unit: ""
    availability: ""
  - name: pexsi_gap
    category: PEXSI
    type: Real
    description: |
      Spectral gap, this can be set to be 0 in most cases.
    default_value: "0"
    unit: ""
    availability: ""
  - name: pexsi_delta_e
    category: PEXSI
    type: Real
    description: |
      Upper bound for the spectral radius of S^{-1}H.
    default_value: "20"
    unit: ""
    availability: ""
  - name: pexsi_mu_lower
    category: PEXSI
    type: Real
    description: |
      Initial guess of lower bound for mu.
    default_value: "-10"
    unit: ""
    availability: ""
  - name: pexsi_mu_upper
    category: PEXSI
    type: Real
    description: |
      Initial guess of upper bound for mu.
    default_value: "10"
    unit: ""
    availability: ""
  - name: pexsi_mu
    category: PEXSI
    type: Real
    description: |
      Initial guess for mu (for the solver).
    default_value: "0"
    unit: ""
    availability: ""
  - name: pexsi_mu_thr
    category: PEXSI
    type: Real
    description: |
      Stopping criterion in terms of the chemical potential for the inertia counting procedure.
    default_value: "0.05"
    unit: ""
    availability: ""
  - name: pexsi_mu_expand
    category: PEXSI
    type: Real
    description: |
      If the chemical potential is not in the initial interval, the interval is expanded by this value.
    default_value: "0.3"
    unit: ""
    availability: ""
  - name: pexsi_mu_guard
    category: PEXSI
    type: Real
    description: |
      Safe guard criterion in terms of the chemical potential to reinvoke the inertia counting procedure.
    default_value: "0.2"
    unit: ""
    availability: ""
  - name: pexsi_elec_thr
    category: PEXSI
    type: Real
    description: |
      Stopping criterion of the PEXSI iteration in terms of the number of electrons compared to numElectronExact.
    default_value: "0.001"
    unit: ""
    availability: ""
  - name: pexsi_zero_thr
    category: PEXSI
    type: Real
    description: |
      if the absolute value of CCS matrix element is less than this value, it will be considered as zero.
    default_value: "1e-10"
    unit: ""
    availability: ""
  - name: out_alllog
    category: Output information
    type: Boolean
    description: |
      Whether to print information into individual logs from all ranks in an MPI run.
      * True: Information from each rank will be written into individual files named OUT.{calculation}_{suffix}/running_${calculation}.log.
    default_value: "False"
    unit: ""
    availability: ""
  - name: nurse
    category: Variables useful for debugging
    type: Integer
    description: |
      Debugging flag for developers
    default_value: "0"
    unit: ""
    availability: ""
  - name: t_in_h
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to include kinetic term in obtaining the Hamiltonian matrix.
      * 0: No.
      * 1: Yes.
    default_value: "1"
    unit: ""
    availability: ""
  - name: vl_in_h
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to include local pseudopotential term in obtaining the Hamiltonian matrix.
      * 0: No.
      * 1: Yes.
    default_value: "1"
    unit: ""
    availability: ""
  - name: vnl_in_h
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to include non-local pseudopotential term in obtaining the Hamiltonian matrix.
      * 0: No.
      * 1: Yes.
    default_value: "1"
    unit: ""
    availability: ""
  - name: vh_in_h
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to include Hartree potential term in obtaining the Hamiltonian matrix.
      * 0: No.
      * 1: Yes.
    default_value: "1"
    unit: ""
    availability: ""
  - name: vion_in_h
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to include local ionic potential term in obtaining the Hamiltonian matrix.
      * 0: No.
      * 1: Yes.
    default_value: "1"
    unit: ""
    availability: ""
  - name: test_force
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to output the detailed components in forces.
      * 0: No.
      * 1: Yes.
    default_value: "0"
    unit: ""
    availability: ""
  - name: test_stress
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to output the detailed components in stress.
      * 0: No.
      * 1: Yes.
    default_value: "0"
    unit: ""
    availability: ""
  - name: test_skip_ewald
    category: Variables useful for debugging
    type: Boolean
    description: |
      Specify whether to skip the calculation of the ewald energy.
      * 0: No.
      * 1: Yes.
    default_value: "0"
    unit: ""
    availability: ""
  - name: ri_hartree_benchmark
    category: Linear Response TDDFT
    type: String
    description: |
      Whether to use the RI approximation for the Hartree term in LR-TDDFT for benchmark (with FHI-aims/ABACUS read-in style)
    default_value: none
    unit: ""
    availability: ""
  - name: aims_nbasis
    category: Linear Response TDDFT
    type: A number(ntype) of Integers
    description: |
      Atomic basis set size for each atom type (with the same order as in STRU) in FHI-aims.
    default_value: "{} (empty list, where ABACUS use its own basis set size)"
    unit: ""
    availability: ri_hartree_benchmark==aims
  - name: rdmft
    category: Reduced Density Matrix Functional Theory
    type: Boolean
    description: |
      Whether to perform rdmft calculation (reduced density matrix funcional theory). The physical quantities that RDMFT temporarily expects to output are the kinetic energy, total energy, and 1-RDM of the system in the ground state, etc.
    default_value: "false"
    unit: ""
    availability: ""
  - name: rdmft_power_alpha
    category: Reduced Density Matrix Functional Theory
    type: Real
    description: |
      The alpha parameter of power-functional(or other exx-type/hybrid functionals) which used in RDMFT, g(occ_number) = occ_number^alpha
    default_value: "0.656"
    unit: ""
    availability: ""
  - name: "exxace"
    category: Exact Exchange (PW)
    type: Boolean
    description: |
      Whether to use the ACE method (https://doi.org/10.1021/acs.jctc.6b00092) to accelerate the calculation the Fock exchange matrix. Should be set to true most of the time.
      * True: Use the ACE method to calculate the Fock exchange operator.
      * False: Use the traditional method to calculate the Fock exchange operator.
    default_value: "True"
    unit: ""
    availability: exx_separate_loop==true
  - name: exx_gamma_extrapolation
    category: Exact Exchange (PW)
    type: Boolean
    description: |
      Whether to use the gamma point extrapolation method to calculate the Fock exchange operator. See https://doi.org/10.1103/PhysRevB.79.205114 for details. Should be set to true most of the time.
    default_value: "True"
    unit: ""
    availability: ""
  - name: ecutexx
    category: Exact Exchange (PW)
    type: Real
    description: |
      The energy cutoff for EXX (Fock) exchange operator in plane wave basis calculations. Reducing ecutexx below ecutrho may significantly accelerate EXX computations. This speed improvement comes with a reduced numerical accuracy in the exchange energy calculation.
    default_value: same as ecutrho
    unit: Ry
    availability: ""
  - name: exx_thr_type
    category: Exact Exchange (PW)
    type: String
    description: |
      The type of threshold used to judge whether the outer loop has converged in the separate loop EXX calculation.
      * energy: use the change of exact exchange energy to judge convergence.
      * density: if the change of charge density difference between two successive outer loop iterations is seen as converged according to scf_thr, then the outer loop is seen as converged.
    default_value: density
    unit: ""
    availability: ""
  - name: exx_ene_thr
    category: Exact Exchange (PW)
    type: Real
    description: |
      The threshold for the change of exact exchange energy to judge convergence of the outer loop in the separate loop EXX calculation.
    default_value: "1e-5"
    unit: Ry
    availability: exx_thr_type==energy