Nick P. Proukakis, Gerasimos Rigopoulos, Alex Soto
{"title":"Self-Consistent Stochastic Finite-Temperature Modelling: Ultracold Bose Gases with Local (s-wave) and Long-Range (Dipolar) Interactions","authors":"Nick P. Proukakis, Gerasimos Rigopoulos, Alex Soto","doi":"arxiv-2407.20178","DOIUrl":null,"url":null,"abstract":"We formulate a generalized self-consistent quantum kinetic theory including\nthermal fluctuations and stochastic contributions for modelling ultracold Bose\ngases interacting via a generic long-range interaction. Our generalised\nequations take the usual form of an effective field theory, separating\ncoherent, low-lying, modes of the system from incoherent, higher-lying, thermal\nmodes. The low-lying modes are described by a stochastic Langevin equation with\ntwo explicitly time-dependent collisional terms (corresponding to a dissipative\nand an energy-correcting contribution) and their corresponding additive and\nmultiplicative stochastic noise terms. By coupling such an equation to an\nexplicitly non-equilibrium gas of incoherent (thermal) particles described by a\nquantum Boltzmann equation, we thus extend beyond both earlier stochastic\napproaches (including the full SPGPE) and generalised kinetic models inspired\nby a two-gas picture (the so-called ZNG formalism) commonly used in the context\nof short-range interactions, such as those relevant in ultracold alkali atoms.\nLong-range interactions are further included into our model by the\nself-consistent addition of a Poisson-like equation for the long-range\ninteraction potential. Our approach leads directly to a self-consistent model\nfor finite-temperature Bose-Einstein condensation in a long-range interacting\nsystem within the regime where thermal fluctuations dominate over quantum\nfluctuations. While such an approach could be of general use for a variety of\nexperimentally-accessible long-range interacting systems, we focus specifically\nhere on the well-studied case of dipolar atomic condensates. In this particular\ncontext, we additionally supplement our Keldysh non-equilibrium analysis for\nfluctuations of the fast (incoherent) modes by a somewhat ad hoc extension of\nthe slow (coherent) modes via the usual route of Bogoliubov-de Gennes\nequations.","PeriodicalId":501521,"journal":{"name":"arXiv - PHYS - Quantum Gases","volume":"51 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Quantum Gases","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2407.20178","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 formulate a generalized self-consistent quantum kinetic theory including
thermal fluctuations and stochastic contributions for modelling ultracold Bose
gases interacting via a generic long-range interaction. Our generalised
equations take the usual form of an effective field theory, separating
coherent, low-lying, modes of the system from incoherent, higher-lying, thermal
modes. The low-lying modes are described by a stochastic Langevin equation with
two explicitly time-dependent collisional terms (corresponding to a dissipative
and an energy-correcting contribution) and their corresponding additive and
multiplicative stochastic noise terms. By coupling such an equation to an
explicitly non-equilibrium gas of incoherent (thermal) particles described by a
quantum Boltzmann equation, we thus extend beyond both earlier stochastic
approaches (including the full SPGPE) and generalised kinetic models inspired
by a two-gas picture (the so-called ZNG formalism) commonly used in the context
of short-range interactions, such as those relevant in ultracold alkali atoms.
Long-range interactions are further included into our model by the
self-consistent addition of a Poisson-like equation for the long-range
interaction potential. Our approach leads directly to a self-consistent model
for finite-temperature Bose-Einstein condensation in a long-range interacting
system within the regime where thermal fluctuations dominate over quantum
fluctuations. While such an approach could be of general use for a variety of
experimentally-accessible long-range interacting systems, we focus specifically
here on the well-studied case of dipolar atomic condensates. In this particular
context, we additionally supplement our Keldysh non-equilibrium analysis for
fluctuations of the fast (incoherent) modes by a somewhat ad hoc extension of
the slow (coherent) modes via the usual route of Bogoliubov-de Gennes
equations.