C. Marin, A. Fontana, V. Bellani, F. Pederiva, A. Quaranta, F. Rossella, A. Salamon, G. Salina
{"title":"用 D-Wave 量子退火器模拟受挫伊辛方阵","authors":"C. Marin, A. Fontana, V. Bellani, F. Pederiva, A. Quaranta, F. Rossella, A. Salamon, G. Salina","doi":"arxiv-2409.11259","DOIUrl":null,"url":null,"abstract":"The Ising model with nearest-neighbor interactions on a two-dimensional (2D)\nsquare lattice is one of the simplest models for studying ferro-magnetic to\npara-magnetic transitions. Extensive results are available in the literature\nfor this model, which has become a paradigm for the study of magnetic phase\ntransitions in materials, both theoretically and numerically. After a brief\nreview of the main results obtained with a classical computer, we show how to\nimplement on the D- Wave quantum annealer a more complex Ising model with the\naddition of competing antiferromagnetic interactions between the diagonal\nnext-to-nearest neighbors with two coupling constants J1 and J2. The dynamics\nof this system, owing to frustration, are richer than those of the simple Ising\nmodel and exhibit a third striped (or antiferromagnetic) phase in addition to\nthe ferro- and para-magnetic phases. In this work, we observed all three phases\non the D-Wave hardware, studied the behavior of the solution with different\nannealing parameters, such as the chain strength and annealing time, and showed\nhow to identify the phase transition by varying the ratio between the\nferromagnetic and antiferromagnetic couplings. The same system is studied on a\nclassical computer, with the possibility of taking into account the temperature\n(fixed on D-Wave) as a free parameter and to explore the full phase diagram:\nsome comparative conclusions with D-Wave are drawn.","PeriodicalId":501226,"journal":{"name":"arXiv - PHYS - Quantum Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Modeling a frustrated Ising square lattice with the D-Wave Quantum Annealer\",\"authors\":\"C. Marin, A. Fontana, V. Bellani, F. Pederiva, A. Quaranta, F. Rossella, A. Salamon, G. Salina\",\"doi\":\"arxiv-2409.11259\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The Ising model with nearest-neighbor interactions on a two-dimensional (2D)\\nsquare lattice is one of the simplest models for studying ferro-magnetic to\\npara-magnetic transitions. Extensive results are available in the literature\\nfor this model, which has become a paradigm for the study of magnetic phase\\ntransitions in materials, both theoretically and numerically. After a brief\\nreview of the main results obtained with a classical computer, we show how to\\nimplement on the D- Wave quantum annealer a more complex Ising model with the\\naddition of competing antiferromagnetic interactions between the diagonal\\nnext-to-nearest neighbors with two coupling constants J1 and J2. The dynamics\\nof this system, owing to frustration, are richer than those of the simple Ising\\nmodel and exhibit a third striped (or antiferromagnetic) phase in addition to\\nthe ferro- and para-magnetic phases. In this work, we observed all three phases\\non the D-Wave hardware, studied the behavior of the solution with different\\nannealing parameters, such as the chain strength and annealing time, and showed\\nhow to identify the phase transition by varying the ratio between the\\nferromagnetic and antiferromagnetic couplings. The same system is studied on a\\nclassical computer, with the possibility of taking into account the temperature\\n(fixed on D-Wave) as a free parameter and to explore the full phase diagram:\\nsome comparative conclusions with D-Wave are drawn.\",\"PeriodicalId\":501226,\"journal\":{\"name\":\"arXiv - PHYS - Quantum Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Quantum Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.11259\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Quantum Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.11259","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Modeling a frustrated Ising square lattice with the D-Wave Quantum Annealer
The Ising model with nearest-neighbor interactions on a two-dimensional (2D)
square lattice is one of the simplest models for studying ferro-magnetic to
para-magnetic transitions. Extensive results are available in the literature
for this model, which has become a paradigm for the study of magnetic phase
transitions in materials, both theoretically and numerically. After a brief
review of the main results obtained with a classical computer, we show how to
implement on the D- Wave quantum annealer a more complex Ising model with the
addition of competing antiferromagnetic interactions between the diagonal
next-to-nearest neighbors with two coupling constants J1 and J2. The dynamics
of this system, owing to frustration, are richer than those of the simple Ising
model and exhibit a third striped (or antiferromagnetic) phase in addition to
the ferro- and para-magnetic phases. In this work, we observed all three phases
on the D-Wave hardware, studied the behavior of the solution with different
annealing parameters, such as the chain strength and annealing time, and showed
how to identify the phase transition by varying the ratio between the
ferromagnetic and antiferromagnetic couplings. The same system is studied on a
classical computer, with the possibility of taking into account the temperature
(fixed on D-Wave) as a free parameter and to explore the full phase diagram:
some comparative conclusions with D-Wave are drawn.