Quantum Optimization of Fully Connected Spin Glasses

Many NP-hard problems can be seen as the task of finding a ground state of a disordered highly connected Ising spin glass. If solutions are sought by means of quantum annealing, it is often necessary to represent those graphs in the annealer’s hardware by means of the graph-minor embedding technique...

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Main Authors: Davide Venturelli, Salvatore Mandrà, Sergey Knysh, Bryan O’Gorman, Rupak Biswas, Vadim Smelyanskiy
Format: Article
Language:English
Published: American Physical Society 2015-09-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.5.031040
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spelling doaj-2c931efa1982454fade208a3210bd1ba2020-11-24T22:39:32ZengAmerican Physical SocietyPhysical Review X2160-33082015-09-015303104010.1103/PhysRevX.5.031040Quantum Optimization of Fully Connected Spin GlassesDavide VenturelliSalvatore MandràSergey KnyshBryan O’GormanRupak BiswasVadim SmelyanskiyMany NP-hard problems can be seen as the task of finding a ground state of a disordered highly connected Ising spin glass. If solutions are sought by means of quantum annealing, it is often necessary to represent those graphs in the annealer’s hardware by means of the graph-minor embedding technique, generating a final Hamiltonian consisting of coupled chains of ferromagnetically bound spins, whose binding energy is a free parameter. In order to investigate the effect of embedding on problems of interest, the fully connected Sherrington-Kirkpatrick model with random ±1 couplings is programmed on the D-Wave Two^{TM} annealer using up to 270 qubits interacting on a Chimera-type graph. We present the best embedding prescriptions for encoding the Sherrington-Kirkpatrick problem in the Chimera graph. The results indicate that the optimal choice of embedding parameters could be associated with the emergence of the spin-glass phase of the embedded problem, whose presence was previously uncertain. This optimal parameter setting allows the performance of the quantum annealer to compete with (and potentially outperform, in the absence of analog control errors) optimized simulated annealing algorithms.http://doi.org/10.1103/PhysRevX.5.031040
collection DOAJ
language English
format Article
sources DOAJ
author Davide Venturelli
Salvatore Mandrà
Sergey Knysh
Bryan O’Gorman
Rupak Biswas
Vadim Smelyanskiy
spellingShingle Davide Venturelli
Salvatore Mandrà
Sergey Knysh
Bryan O’Gorman
Rupak Biswas
Vadim Smelyanskiy
Quantum Optimization of Fully Connected Spin Glasses
Physical Review X
author_facet Davide Venturelli
Salvatore Mandrà
Sergey Knysh
Bryan O’Gorman
Rupak Biswas
Vadim Smelyanskiy
author_sort Davide Venturelli
title Quantum Optimization of Fully Connected Spin Glasses
title_short Quantum Optimization of Fully Connected Spin Glasses
title_full Quantum Optimization of Fully Connected Spin Glasses
title_fullStr Quantum Optimization of Fully Connected Spin Glasses
title_full_unstemmed Quantum Optimization of Fully Connected Spin Glasses
title_sort quantum optimization of fully connected spin glasses
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2015-09-01
description Many NP-hard problems can be seen as the task of finding a ground state of a disordered highly connected Ising spin glass. If solutions are sought by means of quantum annealing, it is often necessary to represent those graphs in the annealer’s hardware by means of the graph-minor embedding technique, generating a final Hamiltonian consisting of coupled chains of ferromagnetically bound spins, whose binding energy is a free parameter. In order to investigate the effect of embedding on problems of interest, the fully connected Sherrington-Kirkpatrick model with random ±1 couplings is programmed on the D-Wave Two^{TM} annealer using up to 270 qubits interacting on a Chimera-type graph. We present the best embedding prescriptions for encoding the Sherrington-Kirkpatrick problem in the Chimera graph. The results indicate that the optimal choice of embedding parameters could be associated with the emergence of the spin-glass phase of the embedded problem, whose presence was previously uncertain. This optimal parameter setting allows the performance of the quantum annealer to compete with (and potentially outperform, in the absence of analog control errors) optimized simulated annealing algorithms.
url http://doi.org/10.1103/PhysRevX.5.031040
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