{"title":"临界三量级原子模型的混合排列对称量子相变","authors":"A. Mayorgas, J. Guerrero, Manuel Calixto","doi":"10.21468/scipostphysproc.14.036","DOIUrl":null,"url":null,"abstract":"We define the concept of Mixed Symmetry Quantum Phase Transition (MSQPT), considering each permutation symmetry sector \\muμ of an identical particles system, as singularities in the properties of the lowest-energy state into each \\muμ when shifting a Hamiltonian control parameter \\lambdaλ. A three-level Lipkin-Meshkov-Glick (LMG) model is chosen to typify our construction. Firstly, we analyze the finite number NN of particles case, proving the presence of MSQPT precursors. Then, in the thermodynamic limit N\\to∞N→∞, we calculate the lowest-energy density inside each sector \\muμ, augmenting the control parameter space by \\muμ, and showing a phase diagram with four different quantum phases.","PeriodicalId":355998,"journal":{"name":"SciPost Physics Proceedings","volume":"1 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Mixed permutation symmetry quantum phase transitions of critical three-level atom models\",\"authors\":\"A. Mayorgas, J. Guerrero, Manuel Calixto\",\"doi\":\"10.21468/scipostphysproc.14.036\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We define the concept of Mixed Symmetry Quantum Phase Transition (MSQPT), considering each permutation symmetry sector \\\\muμ of an identical particles system, as singularities in the properties of the lowest-energy state into each \\\\muμ when shifting a Hamiltonian control parameter \\\\lambdaλ. A three-level Lipkin-Meshkov-Glick (LMG) model is chosen to typify our construction. Firstly, we analyze the finite number NN of particles case, proving the presence of MSQPT precursors. Then, in the thermodynamic limit N\\\\to∞N→∞, we calculate the lowest-energy density inside each sector \\\\muμ, augmenting the control parameter space by \\\\muμ, and showing a phase diagram with four different quantum phases.\",\"PeriodicalId\":355998,\"journal\":{\"name\":\"SciPost Physics Proceedings\",\"volume\":\"1 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-11-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"SciPost Physics Proceedings\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.21468/scipostphysproc.14.036\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"SciPost Physics Proceedings","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.21468/scipostphysproc.14.036","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
我们定义了混合对称量子相变(Mixed Symmetry Quantum Phase Transition,MSQPT)的概念,将相同粒子系统的每个排列对称扇区(permutation symmetry sector \muμ)视为当移动哈密顿控制参数(Hamiltonian control parameter \lambdaλ)时,最低能量态进入每个扇区(\muμ)的奇异特性。我们选择了一个三层的利普金-梅什科夫-格里克(LMG)模型来说明我们的构造。首先,我们分析了粒子数 NN 有限的情况,证明了 MSQPT 前体的存在。然后,在热力学极限Nto∞N→∞中,我们计算了每个扇形内部的最低能量密度(\muμ),用\muμ增加了控制参数空间,并展示了具有四种不同量子相的相图。
Mixed permutation symmetry quantum phase transitions of critical three-level atom models
We define the concept of Mixed Symmetry Quantum Phase Transition (MSQPT), considering each permutation symmetry sector \muμ of an identical particles system, as singularities in the properties of the lowest-energy state into each \muμ when shifting a Hamiltonian control parameter \lambdaλ. A three-level Lipkin-Meshkov-Glick (LMG) model is chosen to typify our construction. Firstly, we analyze the finite number NN of particles case, proving the presence of MSQPT precursors. Then, in the thermodynamic limit N\to∞N→∞, we calculate the lowest-energy density inside each sector \muμ, augmenting the control parameter space by \muμ, and showing a phase diagram with four different quantum phases.