Paper
Monte Carlo sampling from a projected entangled-pair state in simulations of quantum annealing in the three dimensional random Ising model
Authors
Jacek Dziarmaga
Abstract
Quantum annealing with the D-Wave Advantage system in the random Ising model on a cubic lattice is simulated using a three-dimensional (3D) tensor network. The Hamiltonian is driven across a quantum phase transition from a paramagnetic phase to a spin-glass phase. The network is represented as a tensor product state, also known-particularly in two dimensions-as a projected entangled-pair state (PEPS). The annealing procedure is repeated for a range of annealing times in order to test the Kibble-Zurek (KZ) power law governing the residual energy at the end of the annealing ramp. For an infinite lattice with periodic nearest-neighbor random Ising couplings, the final energy is evaluated using a deterministic method. For a finite lattice with open boundaries, we introduce a more efficient Monte Carlo sampling approach. In both cases, the residual energy as a function of annealing time approaches the KZ power law as the annealing time increases.
Metadata
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Raw Data (Debug)
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"raw_xml": "<entry>\n <id>http://arxiv.org/abs/2603.16509v1</id>\n <title>Monte Carlo sampling from a projected entangled-pair state in simulations of quantum annealing in the three dimensional random Ising model</title>\n <updated>2026-03-17T13:37:59Z</updated>\n <link href='https://arxiv.org/abs/2603.16509v1' rel='alternate' type='text/html'/>\n <link href='https://arxiv.org/pdf/2603.16509v1' rel='related' title='pdf' type='application/pdf'/>\n <summary>Quantum annealing with the D-Wave Advantage system in the random Ising model on a cubic lattice is simulated using a three-dimensional (3D) tensor network. The Hamiltonian is driven across a quantum phase transition from a paramagnetic phase to a spin-glass phase. The network is represented as a tensor product state, also known-particularly in two dimensions-as a projected entangled-pair state (PEPS). The annealing procedure is repeated for a range of annealing times in order to test the Kibble-Zurek (KZ) power law governing the residual energy at the end of the annealing ramp. For an infinite lattice with periodic nearest-neighbor random Ising couplings, the final energy is evaluated using a deterministic method. For a finite lattice with open boundaries, we introduce a more efficient Monte Carlo sampling approach. In both cases, the residual energy as a function of annealing time approaches the KZ power law as the annealing time increases.</summary>\n <category scheme='http://arxiv.org/schemas/atom' term='quant-ph'/>\n <category scheme='http://arxiv.org/schemas/atom' term='cond-mat.dis-nn'/>\n <category scheme='http://arxiv.org/schemas/atom' term='cond-mat.str-el'/>\n <published>2026-03-17T13:37:59Z</published>\n <arxiv:comment>9 pages, 8 figures</arxiv:comment>\n <arxiv:primary_category term='quant-ph'/>\n <author>\n <name>Jacek Dziarmaga</name>\n </author>\n </entry>"
}