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...
Main Authors: | , , , , , |
---|---|
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 |
id |
doaj-2c931efa1982454fade208a3210bd1ba |
---|---|
record_format |
Article |
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 |
work_keys_str_mv |
AT davideventurelli quantumoptimizationoffullyconnectedspinglasses AT salvatoremandra quantumoptimizationoffullyconnectedspinglasses AT sergeyknysh quantumoptimizationoffullyconnectedspinglasses AT bryanogorman quantumoptimizationoffullyconnectedspinglasses AT rupakbiswas quantumoptimizationoffullyconnectedspinglasses AT vadimsmelyanskiy quantumoptimizationoffullyconnectedspinglasses |
_version_ |
1716487091217498112 |