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Add nice hhl example #1445
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| Original file line number | Diff line number | Diff line change |
|---|---|---|
| @@ -1,164 +1,110 @@ | ||
| qfunc load_b_expanded___0(amplitudes: real[], output memory: qbit[2]) { | ||
| prepare_amplitudes(amplitudes, 0.0, memory); | ||
| } | ||
| // Harrow–Hassidim–Lloyd (HHL) Algorithm for Solving Linear Systems | ||
|
|
||
| qfunc apply_to_all_expanded___0(target: qbit[4]) { | ||
| repeat (index: 4) { | ||
| H(target[index]); | ||
| } | ||
| } | ||
| // This example implements the HHL quantum linear-systems algorithm to solve | ||
| // A |x⟩ = |b⟩ | ||
| // where A is a Hermitian matrix and |b⟩ is the right-hand-side vector prepared | ||
| // as a quantum state. | ||
|
|
||
| qfunc hamiltonian_evolution_with_power_0_lambda___0_0_expanded___0(pw: int, target: qbit[2]) { | ||
| power (pw) { | ||
| unitary([ | ||
| [ | ||
| ((-0.09406240950199857) + 0.8149069223122054j), | ||
| (0.03521871946675126 - 0.029763534641642615j), | ||
| ((-0.018800717000078293) - 0.16142879795007106j), | ||
| (0.43769245930764733 + 0.32705554908759304j) | ||
| ], | ||
| [ | ||
| (0.03521871946675127 - 0.029763534641642633j), | ||
| ((-0.15347248298890326) - 0.17275282472948233j), | ||
| (0.23117644455908531 + 0.8872069971297389j), | ||
| (0.23971825754883572 + 0.21548267921288933j) | ||
| ], | ||
| [ | ||
| ((-0.01880071700007826) - 0.16142879795007103j), | ||
| (0.23117644455908523 + 0.8872069971297386j), | ||
| ((-0.1219131720516462) + 0.13200138126428373j), | ||
| (0.29584069101495575 + 0.11488938733473114j) | ||
| ], | ||
| [ | ||
| (0.43769245930764744 + 0.32705554908759327j), | ||
| (0.2397182575488357 + 0.21548267921288933j), | ||
| (0.29584069101495586 + 0.1148893873347311j), | ||
| ((-0.6563827949579104) + 0.25690988991104674j) | ||
| ] | ||
| ], target); | ||
| } | ||
| } | ||
|
|
||
| qfunc unitary_with_power_0_lambda___0_0_expanded___0(k: int, memory_captured__hhl__1: qbit[2]) { | ||
| hamiltonian_evolution_with_power_0_lambda___0_0_expanded___0(k, memory_captured__hhl__1); | ||
| } | ||
| // In this example, the matrix A is given as a sum of Pauli strings: | ||
| // A = 0.03*X(0)*X(1) + 0.05*Z(0)*Z(1) + 0.02*Y(0)*Y(1) + 0.08*I | ||
| // This Pauli decomposition corresponds to the matrix | ||
| // A = [[0.13, 0.00, 0.00, 0.01], | ||
| // [0.00, 0.03, 0.05, 0.00], | ||
| // [0.00, 0.05, 0.03, 0.00], | ||
| // [0.01, 0.00, 0.00, 0.13]] | ||
|
|
||
| qfunc qft_no_swap_expanded___0(qbv: qbit[4]) { | ||
| repeat (i: 4) { | ||
| H(qbv[i]); | ||
| repeat (j: (4 - i) - 1) { | ||
| CPHASE(pi / (2 ** (j + 1)), qbv[(i + j) + 1], qbv[i]); | ||
| } | ||
| } | ||
| } | ||
| hamiltonian: SparsePauliOp = SparsePauliOp { | ||
| terms=[ | ||
| SparsePauliTerm { | ||
| paulis=[ | ||
| IndexedPauli {pauli=1, index=0}, | ||
| IndexedPauli {pauli=1, index=1} | ||
| ], | ||
| coefficient=0.03 | ||
| }, | ||
| SparsePauliTerm { | ||
| paulis=[ | ||
| IndexedPauli {pauli=3, index=1}, | ||
| IndexedPauli {pauli=3, index=0} | ||
| ], | ||
| coefficient=0.05 | ||
| }, | ||
| SparsePauliTerm { | ||
| paulis=[ | ||
| IndexedPauli {pauli=2, index=0}, | ||
| IndexedPauli {pauli=2, index=1} | ||
| ], | ||
| coefficient=0.02 | ||
| }, | ||
| SparsePauliTerm { | ||
| paulis=[ | ||
| IndexedPauli {pauli=0, index=0} | ||
| ], | ||
| coefficient=0.08 | ||
| } | ||
| ], | ||
| num_qubits=2 | ||
| }; | ||
|
|
||
| qfunc qft_expanded___0(target: qbit[4]) { | ||
| repeat (index: 2.0) { | ||
| SWAP(target[index], target[3 - index]); | ||
| } | ||
| qft_no_swap_expanded___0(target); | ||
| } | ||
| // For the right-hand-side vector |b⟩, we use a normalized vector of size 4. | ||
| rhs_vector: real[] = [sqrt(1/6), sqrt(1/6), sqrt(1/6), sqrt(1/2)]; | ||
|
|
||
| qfunc qpe_flexible_expanded___0(phase: qbit[4], memory_captured__hhl__1: qbit[2]) { | ||
| apply_to_all_expanded___0(phase); | ||
| repeat (index: 4) { | ||
| control (phase[index]) { | ||
| unitary_with_power_0_lambda___0_0_expanded___0(2 ** index, memory_captured__hhl__1); | ||
| } | ||
| } | ||
| invert { | ||
| qft_expanded___0(phase); | ||
| } | ||
| // In our example the matrix A is a sum of commuting Pauli strings. | ||
| // We define how to take powers of the Hamiltonian evolution exp(2π A), which is applied | ||
| // within the Quantum Phase Estimation. We simply multiply the evolution time by the power value, | ||
| // keeping the number of Trotter repetition being 1, as suitable for commuting terms. | ||
| qfunc powered_suzuki_trotter_commuting_terms(k: int, hamiltonian: SparsePauliOp, qba: qbit[]) { | ||
| suzuki_trotter(hamiltonian, -2*pi* k, 1, 1, qba); | ||
| } | ||
|
|
||
| qfunc assign_amplitude_table_expanded___0(const index: qbit[4], indicator: qbit) { | ||
| RY(0.49069646327199606, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(-0.159660988575539, indicator); | ||
| skip_control { | ||
| CX(index[1], indicator); | ||
| } | ||
| RY(-0.215103068840025, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(0.114786680603947, indicator); | ||
| skip_control { | ||
| CX(index[2], indicator); | ||
| } | ||
| RY(0.0734201414091853, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(-0.222322935969005, indicator); | ||
| skip_control { | ||
| CX(index[1], indicator); | ||
| } | ||
| RY(-0.181317761599329, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(0.22482930086683403, indicator); | ||
| skip_control { | ||
| CX(index[3], indicator); | ||
| } | ||
| RY(0.192520246080629, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(-0.184296564729869, indicator); | ||
| skip_control { | ||
| CX(index[1], indicator); | ||
| } | ||
| RY(-0.22312206827512002, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(0.0676093870745949, indicator); | ||
| skip_control { | ||
| CX(index[2], indicator); | ||
| } | ||
| RY(0.0978641117835104, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(-0.216731023385388, indicator); | ||
| skip_control { | ||
| CX(index[1], indicator); | ||
| } | ||
| RY(-0.168241915420623, indicator); | ||
| skip_control { | ||
| CX(index[0], indicator); | ||
| } | ||
| RY(0.309069995704199, indicator); | ||
| skip_control { | ||
| CX(index[3], indicator); | ||
| } | ||
| // We define a quantum function that assigns eigenvalue inversion to the amplitudes for a signed qnum of | ||
| // size 4 with 4 fraction places index. The desired amplitudes are conditioned by an additional | ||
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|
||
| // indicator qubit being at state 1, and are normalized by the smallest possible value of 1/2^index.size. | ||
| qfunc assign_inversion_size4(const index: qbit[4], indicator: qbit) { | ||
| RY(-0.0157, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(-0.0157, indicator); | ||
| skip_control { CX(index[1], indicator); } | ||
| RY(-0.3379, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(0.3066, indicator); | ||
| skip_control { CX(index[2], indicator); } | ||
| RY(-0.1047, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(-0.1047, indicator); | ||
| skip_control { CX(index[1], indicator); } | ||
| RY(-0.3181, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(0.4649, indicator); | ||
| skip_control { CX(index[3], indicator); } | ||
| RY(-0.0475, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(-0.0475, indicator); | ||
| skip_control { CX(index[1], indicator); } | ||
| RY(-0.3407, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(0.2457, indicator); | ||
| skip_control { CX(index[2], indicator); } | ||
| RY(-0.0939, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(-0.0939, indicator); | ||
| skip_control { CX(index[1], indicator); } | ||
| RY(-0.3122, indicator); | ||
| skip_control { CX(index[0], indicator); } | ||
| RY(0.8154, indicator); | ||
| skip_control { CX(index[3], indicator); } | ||
| } | ||
|
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||
| qfunc hhl_expanded___0(rhs_vector: real[], output memory: qbit[2], output estimator: qnum<4, False, 4>, output indicator: qbit) { | ||
| allocate(4, False, 4, estimator); | ||
| load_b_expanded___0([ | ||
| 0.18257418583505536, | ||
| 0.3651483716701107, | ||
| 0.7302967433402214, | ||
| 0.5477225575051661 | ||
| ], memory); | ||
| allocate(1, indicator); | ||
| qfunc main(output solution: qnum<2, False, 0>, output phase_var: qnum<4, True, 4>, output indicator: qbit) { | ||
| allocate(phase_var); | ||
| allocate(indicator); | ||
| prepare_amplitudes(rhs_vector, 0.0, solution); | ||
| within { | ||
| qpe_flexible_expanded___0(estimator, memory); | ||
| qpe_flexible(lambda(k) { | ||
| powered_suzuki_trotter_commuting_terms(k, hamiltonian, solution); | ||
| }, phase_var); | ||
| } apply { | ||
| assign_amplitude_table_expanded___0(estimator, indicator); | ||
| assign_inversion_size4(phase_var, indicator); | ||
| } | ||
| } | ||
|
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||
| qfunc main(output res: qnum<2, False, 0>, output estimator_var: qnum<4, False, 4>, output indicator: qbit) { | ||
| hhl_expanded___0([ | ||
| 0.18257418583505536, | ||
| 0.3651483716701107, | ||
| 0.7302967433402214, | ||
| 0.5477225575051661 | ||
| ], res, estimator_var, indicator); | ||
| } | ||
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