{"title":"局部量子自旋链淬火的有限时间路径场论微扰方法","authors":"Domagoj Kuić, Alemka Knapp, Diana Šaponja-Milutinović","doi":"arxiv-2409.03832","DOIUrl":null,"url":null,"abstract":"We discuss local magnetic field quenches using perturbative methods of finite\ntime path field theory in the following spin chains: Ising and XY in a\ntransverse magnetic field. Their common characteristics are: i) they are\nintegrable via mapping to second quantized noninteracting fermion problem; ii)\nwhen the ground state is nondegenerate (true for finite chains except in\nspecial cases) it can be represented as a vacuum of Bogoliubov fermions. By\nswitching on a local magnetic field perturbation at finite time, the problem\nbecomes nonintegrable and must be approached via numeric or perturbative\nmethods. Using the formalism of finite time path field theory based on Wigner\ntransforms of projected functions, we show how to: i) calculate the basic\n\"bubble\" diagram in the Loschmidt echo of a quenched chain to any order in the\nperturbation; ii) resum the generalized Schwinger-Dyson equation for the\nfermion two point retarded functions in the \"bubble\" diagram, hence achieving\nthe resummation of perturbative expansion of Loschmidt echo for a wide range of\nperturbation strengths under certain analiticity assumptions. Limitations of\nthe assumptions and possible generalizations beyond it and also for other spin\nchains are further discussed.","PeriodicalId":501520,"journal":{"name":"arXiv - PHYS - Statistical Mechanics","volume":"66 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Finite time path field theory perturbative methods for local quantum spin chain quenches\",\"authors\":\"Domagoj Kuić, Alemka Knapp, Diana Šaponja-Milutinović\",\"doi\":\"arxiv-2409.03832\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We discuss local magnetic field quenches using perturbative methods of finite\\ntime path field theory in the following spin chains: Ising and XY in a\\ntransverse magnetic field. Their common characteristics are: i) they are\\nintegrable via mapping to second quantized noninteracting fermion problem; ii)\\nwhen the ground state is nondegenerate (true for finite chains except in\\nspecial cases) it can be represented as a vacuum of Bogoliubov fermions. By\\nswitching on a local magnetic field perturbation at finite time, the problem\\nbecomes nonintegrable and must be approached via numeric or perturbative\\nmethods. Using the formalism of finite time path field theory based on Wigner\\ntransforms of projected functions, we show how to: i) calculate the basic\\n\\\"bubble\\\" diagram in the Loschmidt echo of a quenched chain to any order in the\\nperturbation; ii) resum the generalized Schwinger-Dyson equation for the\\nfermion two point retarded functions in the \\\"bubble\\\" diagram, hence achieving\\nthe resummation of perturbative expansion of Loschmidt echo for a wide range of\\nperturbation strengths under certain analiticity assumptions. Limitations of\\nthe assumptions and possible generalizations beyond it and also for other spin\\nchains are further discussed.\",\"PeriodicalId\":501520,\"journal\":{\"name\":\"arXiv - PHYS - Statistical Mechanics\",\"volume\":\"66 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-05\",\"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-2409.03832\",\"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 - Statistical Mechanics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.03832","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Finite time path field theory perturbative methods for local quantum spin chain quenches
We discuss local magnetic field quenches using perturbative methods of finite
time path field theory in the following spin chains: Ising and XY in a
transverse magnetic field. Their common characteristics are: i) they are
integrable via mapping to second quantized noninteracting fermion problem; ii)
when the ground state is nondegenerate (true for finite chains except in
special cases) it can be represented as a vacuum of Bogoliubov fermions. By
switching on a local magnetic field perturbation at finite time, the problem
becomes nonintegrable and must be approached via numeric or perturbative
methods. Using the formalism of finite time path field theory based on Wigner
transforms of projected functions, we show how to: i) calculate the basic
"bubble" diagram in the Loschmidt echo of a quenched chain to any order in the
perturbation; ii) resum the generalized Schwinger-Dyson equation for the
fermion two point retarded functions in the "bubble" diagram, hence achieving
the resummation of perturbative expansion of Loschmidt echo for a wide range of
perturbation strengths under certain analiticity assumptions. Limitations of
the assumptions and possible generalizations beyond it and also for other spin
chains are further discussed.