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A Quantum-Quantum Metropolis Algorithm

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arxiv 1011.1468 v1 pith:OZ5HMW2L submitted 2010-11-05 quant-ph math-phmath.MP

A Quantum-Quantum Metropolis Algorithm

classification quant-ph math-phmath.MP
keywords quantumclassicalmetropolismarkovalgorithmhamiltoniansmethodspeedup
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Recently, the idea of classical Metropolis sampling through Markov chains has been generalized for quantum Hamiltonians. However, the underlying Markov chain of this algorithm is still classical in nature. Due to Szegedy's method, the Markov chains of classical Hamiltonians can achieve a quadratic quantum speedup in the eigenvalue gap of the corresponding transition matrix. A natural question to ask is whether Szegedy's quantum speedup is merely a consequence of employing classical Hamiltonians, where the eigenstates simply coincide with the computational basis, making cloning of the classical information possible. We solve this problem by introducing a quantum version of the method of Markov-chain quantization combined with the quantum simulated annealing (QSA) procedure, and describe explicitly a novel quantum Metropolis algorithm, which exhibits a quadratic quantum speedup in the eigenvalue gap of the corresponding Metropolis Markov chain for any quantum Hamiltonian. This result provides a complete generalization of the classical Metropolis method to the quantum domain.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Preparing thermal states of frustrated quantum spin systems using 139 qubits

    quant-ph 2026-05 unverdicted novelty 6.0

    Dissipative preparation of thermal states for kagome antiferromagnets demonstrated on IBM hardware up to 79 spins, with simulations showing scalable circuit depths.

  2. Preparing thermal states of frustrated quantum spin systems using 139 qubits

    quant-ph 2026-05 unverdicted novelty 5.0

    Dissipative protocols on quantum hardware prepare approximate thermal states for kagome AFIM up to 79 sites and AFHM via simulation, with circuit depth independent of size and linear in inverse temperature.