Xun Cai, Zhaoyu Han, Zi-Xiang Li, Steven A. Kivelson, Hong Yao
{"title":"来自电子-声子耦合的量子自旋液体","authors":"Xun Cai, Zhaoyu Han, Zi-Xiang Li, Steven A. Kivelson, Hong Yao","doi":"arxiv-2408.04002","DOIUrl":null,"url":null,"abstract":"A quantum spin liquid (QSL) is an exotic insulating phase with emergent gauge\nfields and fractionalized excitations. However, the unambiguous demonstration\nof the existence of a QSL in a \"non-engineered\" microscopic model (or in any\nmaterial) remains challenging. Here, using numerically-exact sign-problem-free\nquantum Monte Carlo simulations, we show that a QSL arises in a non-engineered\nelectron-phonon model. Specifically, we investigate the ground-state phase\ndiagram of the bond Su-Schrieffer-Heeger (SSH) model on a 2D triangular lattice\nat half filling (one electron per site) which we show includes a QSL phase\nwhich is fully gapped, exhibits no symmetry-breaking order, and supports\ndeconfined fractionalized holon excitations. This suggests new routes for\nfinding QSLs in realistic materials and high-$T_c$ superconductivity by lightly\ndoping them.","PeriodicalId":501069,"journal":{"name":"arXiv - PHYS - Superconductivity","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-08-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Quantum spin liquid from electron-phonon coupling\",\"authors\":\"Xun Cai, Zhaoyu Han, Zi-Xiang Li, Steven A. Kivelson, Hong Yao\",\"doi\":\"arxiv-2408.04002\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A quantum spin liquid (QSL) is an exotic insulating phase with emergent gauge\\nfields and fractionalized excitations. However, the unambiguous demonstration\\nof the existence of a QSL in a \\\"non-engineered\\\" microscopic model (or in any\\nmaterial) remains challenging. Here, using numerically-exact sign-problem-free\\nquantum Monte Carlo simulations, we show that a QSL arises in a non-engineered\\nelectron-phonon model. Specifically, we investigate the ground-state phase\\ndiagram of the bond Su-Schrieffer-Heeger (SSH) model on a 2D triangular lattice\\nat half filling (one electron per site) which we show includes a QSL phase\\nwhich is fully gapped, exhibits no symmetry-breaking order, and supports\\ndeconfined fractionalized holon excitations. This suggests new routes for\\nfinding QSLs in realistic materials and high-$T_c$ superconductivity by lightly\\ndoping them.\",\"PeriodicalId\":501069,\"journal\":{\"name\":\"arXiv - PHYS - Superconductivity\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-08-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Superconductivity\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2408.04002\",\"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 - Superconductivity","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.04002","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A quantum spin liquid (QSL) is an exotic insulating phase with emergent gauge
fields and fractionalized excitations. However, the unambiguous demonstration
of the existence of a QSL in a "non-engineered" microscopic model (or in any
material) remains challenging. Here, using numerically-exact sign-problem-free
quantum Monte Carlo simulations, we show that a QSL arises in a non-engineered
electron-phonon model. Specifically, we investigate the ground-state phase
diagram of the bond Su-Schrieffer-Heeger (SSH) model on a 2D triangular lattice
at half filling (one electron per site) which we show includes a QSL phase
which is fully gapped, exhibits no symmetry-breaking order, and supports
deconfined fractionalized holon excitations. This suggests new routes for
finding QSLs in realistic materials and high-$T_c$ superconductivity by lightly
doping them.