{"title":"Fully polarized Fermi systems at finite temperature","authors":"Krzysztof Myśliwy, Marek Napiórkowski","doi":"arxiv-2409.02568","DOIUrl":null,"url":null,"abstract":"We propose a simple model of an interacting, fully spin--polarized Fermi gas\nin dimensions $d=2$ and $d=3$, and derive the approximate expression for the\nenergy spectrum and the corresponding formula for the Helmholtz free energy. We\nanalyze the thermodynamics of the system and find the lines of first--order\nphase transitions between the low and high density phases terminating at\ncritical points. The properties of the corresponding phase diagrams are\nqualitatively different for $d=2$ and $3$, and sensitively depend on the\ninterparticle attraction, which marks a departure from the standard van der\nWaals theory. The differences originate from the Pauli exclusion principle and\nare embeded in the fermionic nature of the system under study.","PeriodicalId":501520,"journal":{"name":"arXiv - PHYS - Statistical Mechanics","volume":"13 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Statistical Mechanics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.02568","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
We propose a simple model of an interacting, fully spin--polarized Fermi gas
in dimensions $d=2$ and $d=3$, and derive the approximate expression for the
energy spectrum and the corresponding formula for the Helmholtz free energy. We
analyze the thermodynamics of the system and find the lines of first--order
phase transitions between the low and high density phases terminating at
critical points. The properties of the corresponding phase diagrams are
qualitatively different for $d=2$ and $3$, and sensitively depend on the
interparticle attraction, which marks a departure from the standard van der
Waals theory. The differences originate from the Pauli exclusion principle and
are embeded in the fermionic nature of the system under study.