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Experimental investigation of performance differences between coherent Ising machines and a quantum annealer

Physical annealing systems provide heuristic approaches to solving combinatorial optimization problems. Here, we benchmark two types of annealing machines—a quantum annealer built by D-Wave Systems and measurement-feedback coherent Ising machines (CIMs) based on optical parametric oscillators—on two...

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Detalles Bibliográficos
Autores principales: Hamerly, Ryan, Inagaki, Takahiro, McMahon, Peter L., Venturelli, Davide, Marandi, Alireza, Onodera, Tatsuhiro, Ng, Edwin, Langrock, Carsten, Inaba, Kensuke, Honjo, Toshimori, Enbutsu, Koji, Umeki, Takeshi, Kasahara, Ryoichi, Utsunomiya, Shoko, Kako, Satoshi, Kawarabayashi, Ken-ichi, Byer, Robert L., Fejer, Martin M., Mabuchi, Hideo, Englund, Dirk, Rieffel, Eleanor, Takesue, Hiroki, Yamamoto, Yoshihisa
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Association for the Advancement of Science 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6534389/
https://www.ncbi.nlm.nih.gov/pubmed/31139743
http://dx.doi.org/10.1126/sciadv.aau0823
Descripción
Sumario:Physical annealing systems provide heuristic approaches to solving combinatorial optimization problems. Here, we benchmark two types of annealing machines—a quantum annealer built by D-Wave Systems and measurement-feedback coherent Ising machines (CIMs) based on optical parametric oscillators—on two problem classes, the Sherrington-Kirkpatrick (SK) model and MAX-CUT. The D-Wave quantum annealer outperforms the CIMs on MAX-CUT on cubic graphs. On denser problems, however, we observe an exponential penalty for the quantum annealer [exp(–α(DW)N(2))] relative to CIMs [exp(–α(CIM)N)] for fixed anneal times, both on the SK model and on 50% edge density MAX-CUT. This leads to a several orders of magnitude time-to-solution difference for instances with over 50 vertices. An optimal–annealing time analysis is also consistent with a substantial projected performance difference. The difference in performance between the sparsely connected D-Wave machine and the fully-connected CIMs provides strong experimental support for efforts to increase the connectivity of quantum annealers.