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Quantum random power method for ground state computation

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arxiv 2408.08556 v2 pith:MANAHGLW submitted 2024-08-16 quant-ph cs.NAmath.NA

classification quant-phcs.NAmath.NA
keywords quantummethodgroundstatehamiltonianpolynomialapproximationpart
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We present a quantum-classical hybrid random power method that approximates a ground state of a Hamiltonian. The quantum part of our method computes a fixed number of elements of a Hamiltonian-matrix polynomial via quantum polynomial filtering techniques with either Hamiltonian simulation or block encoding. The use of the techniques provides a computational advantage that may not be achieved classically in terms of the degree of the polynomial. The classical part of our method is a randomized iterative algorithm that takes as input the matrix elements computed from the quantum part and outputs an approximation of ground state of the Hamiltonian. We prove that with probability one, our method converges to an approximation of a ground state of the Hamiltonian, requiring a constant scaling of the per-iteration classical complexity. The required quantum circuit depth is independent of the initial overlap and has no or a square-root dependence on the spectral gap. The iteration complexity scales linearly as the dimension of the Hilbert space when the quantum polynomial filtering corresponds to a sparse matrix. We numerically validate this sparsity condition for well-known model Hamiltonians. We also present a lower bound of the fidelity, which depends on the magnitude of noise occurring from quantum computation regardless of its charateristics, if it is smaller than a critical value. Several numerical experiments demonstrate that our method provides a good approximation of ground state in the presence of systematic and/or sampling noise.

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Cited by 1 Pith paper

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  1. Classical optimization algorithms for diagonalizing quantum Hamiltonians

    quant-ph 2025-06 reject novelty 5.0 of 10

    The authors prove a benign optimization landscape for a Pauli-based diagonalization cost, but the claimed new family of efficiently diagonalizable Hamiltonians is invalid as stated because its 'diagonal' D includes Y ...

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