{"title":"广义量子拉比模型的分析近似值","authors":"Chon-Fai Kam, Yang Chen","doi":"arxiv-2401.05615","DOIUrl":null,"url":null,"abstract":"The quantum Rabi model is essential for understanding interacting quantum\nsystems. It serves as the simplest non-integrable yet solvable model describing\nthe interaction between a two-level system and a single mode of a bosonic\nfield. In this study, we delve into the exploration of the generalized quantum\nRabi model, wherein the bosonic mode of the field undergoes squeezing.\nUtilizing the Segal-Bargmann representation of the infinite-dimensional Hilbert\nspace, we demonstrate that the energy spectrum of the generalized quantum Rabi\nmodel, when both the Rabi coupling strength and the squeezing strength are not\nsignificantly large compared to the field mode frequency, can be analytically\ndetermined by a bi-confluent Fuchsian equation with two regular singularities\nat 0 and 1 and an irregular singularity of rank two at infinity.","PeriodicalId":501275,"journal":{"name":"arXiv - PHYS - Mathematical Physics","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-01-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Analytical approximations for generalized quantum Rabi models\",\"authors\":\"Chon-Fai Kam, Yang Chen\",\"doi\":\"arxiv-2401.05615\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The quantum Rabi model is essential for understanding interacting quantum\\nsystems. It serves as the simplest non-integrable yet solvable model describing\\nthe interaction between a two-level system and a single mode of a bosonic\\nfield. In this study, we delve into the exploration of the generalized quantum\\nRabi model, wherein the bosonic mode of the field undergoes squeezing.\\nUtilizing the Segal-Bargmann representation of the infinite-dimensional Hilbert\\nspace, we demonstrate that the energy spectrum of the generalized quantum Rabi\\nmodel, when both the Rabi coupling strength and the squeezing strength are not\\nsignificantly large compared to the field mode frequency, can be analytically\\ndetermined by a bi-confluent Fuchsian equation with two regular singularities\\nat 0 and 1 and an irregular singularity of rank two at infinity.\",\"PeriodicalId\":501275,\"journal\":{\"name\":\"arXiv - PHYS - Mathematical Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-01-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Mathematical Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2401.05615\",\"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 - Mathematical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2401.05615","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Analytical approximations for generalized quantum Rabi models
The quantum Rabi model is essential for understanding interacting quantum
systems. It serves as the simplest non-integrable yet solvable model describing
the interaction between a two-level system and a single mode of a bosonic
field. In this study, we delve into the exploration of the generalized quantum
Rabi model, wherein the bosonic mode of the field undergoes squeezing.
Utilizing the Segal-Bargmann representation of the infinite-dimensional Hilbert
space, we demonstrate that the energy spectrum of the generalized quantum Rabi
model, when both the Rabi coupling strength and the squeezing strength are not
significantly large compared to the field mode frequency, can be analytically
determined by a bi-confluent Fuchsian equation with two regular singularities
at 0 and 1 and an irregular singularity of rank two at infinity.