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RFP/MPDO 2/5 Commuting parent Hamiltonians and decorrelation theorem #234

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@LionSR

What

Define commuting and nearest-neighbor commuting parent Hamiltonians (NNCPH). Prove the dimension-independent decorrelation ⟺ commuting Hamiltonian equivalence from Appendix D. Connect to the RFP theory (Thm 3.10(iii) ⟺ (i), gated on [Beigi]).

Files

  • TNLean/MPS/ParentHamiltonian/Commuting.leanIsCommutingParentHam, IsNNCPH, RFP connection
  • TNLean/MPS/ParentHamiltonian/Decorrelation.leanIsDecorrelated, decorrelation ⟺ commuting Ham
  • Blueprint: extend ch14 (§14.6 commuting PH, §14.7 decorrelation)

Key definitions

/-- Commuting parent Hamiltonian: local terms mutually commute. -/
def IsCommutingParentHam (A : MPSTensor d D) (L N : ℕ) : Prop :=
  ∀ i j : Fin N, localTerm A L N i * localTerm A L N j = localTerm A L N j * localTerm A L N i

/-- Nearest-neighbor commuting parent Hamiltonian (L = 2). -/
def IsNNCPH (A : MPSTensor d D) (N : ℕ) : Prop :=
  IsCommutingParentHam A 2 N

/-- Regions A and B are decorrelated w.r.t. subspace K if
    P_K O_A P_K^⊥ O_B P_K = 0 for all observables O_A, O_B. -/
def IsDecorrelated (P_K : ...) (H_A H_B : ...) : Prop := ...

Key statements

  1. Def 3.9 IsCommutingParentHam, IsNNCPH
  2. Thm 3.10(iii)⟹(i) nncph_implies_rfp: NNCPH ⟹ RFP — gated on [Beigi]
  3. Thm 3.10(i)⟹(iii) rfp_implies_nncph: RFP ⟹ NNCPH — follows from Thm 3.11 structural form
  4. Prop D.1 decorrelated_iff_commutingHam: K_{AXB} has commuting parent Ham ⟺ A, B decorrelated

Approach

Commuting.lean: IsCommutingParentHam is a predicate on the PH definitions from #191 (PR#201). The direction RFP ⟹ NNCPH is straightforward from the structural form (Thm 3.11, issue 1/5): RFP tensors generate product-of-entangled-pair states, whose parent Hamiltonians obviously commute. The reverse direction (NNCPH ⟹ RFP) uses [Beigi]'s result that ground spaces of commuting NN Hamiltonians in 1D with finite degeneracy are spanned by states of the form U^⊗N |φ⟩^⊗N that are locally orthogonal — hence RFP by Thm 3.11.

Decorrelation.lean: Self-contained, dimension-independent. The proof uses:

  • Support projectors P_{AX}, P_{XB} of partial traces of K_{AXB}
  • The decorrelation condition forces P_{AX} P_{XB} = P_{XB} P_{AX} = P_{AXB}
  • Commutativity of projectors ⟹ commuting Hamiltonian (set Q = 1 - P)
  • Converse: commuting projectors ⟹ P_{AX} P_{XB} = P_{AXB} ⟹ decorrelation

Reading

  • [CPGSV17] Papers/1606.00608/MPDO-22-12-17-2.tex §3.3 (lines 507–528), Appendix B last paragraph (lines 1305–1307), Appendix D.2 (lines 2181–2290)
  • [Beigi] Beigi, Shor, Whalen, Commun. Math. Phys. 2012 — ground space characterization for commuting Hamiltonians

Dependencies

Estimated ~470 LOC. Decorrelation theorem (~350) is independent of everything else.

Part of #232.

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    1606.00608arXiv:1606.00608 (MPDO RFP)formalizationLean 4 formalization taskparent-hamiltonianParent Hamiltonian theory for MPS (RMP §IV.C)rfp-mpdoRenormalization fixed points and MPDO theory

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