{"title":"Nonequilibrium thermodynamics as a symplecto-contact reduction and relative information entropy","authors":"Jin-wook Lim, Yong-Geun Oh","doi":"10.1016/s0034-4877(23)00084-8","DOIUrl":null,"url":null,"abstract":"<p>Both statistical phase space (SPS), which is Γ = <em>T</em>* <span><math><mrow is=\"true\"><mi is=\"true\" mathvariant=\"double-struck\">R</mi></mrow></math></span><sup>3<em>N</em></sup> of <em>N</em><span><span>-body particle system, and kinetic theory phase space (KTPS), which is the </span>cotangent bundle </span><em>T</em>* <span><math><mrow is=\"true\"><mi is=\"true\" mathvariant=\"double-struck\">P</mi></mrow></math></span>(Γ) of the probability space <span><math><mrow is=\"true\"><mi is=\"true\" mathvariant=\"double-struck\">P</mi></mrow></math></span><span><span><span>(Γ) thereon, carry canonical symplectic structures. Starting from this first principle<span>, we provide a canonical derivation of thermodynamic phase space (TPS) of nonequilibrium thermodynamics as a </span></span>contact manifold<span><span> in two steps. First, regarding the collective observation of observables in SPS as a moment map defined on KTPS, we apply the Marsden–Weinstein reduction and obtain a mesoscopic phase space in between KTPS and TPS as a (infinite-dimensional) symplectic fibration. Then we show that the reduced relative information entropy defines a generating function that provides a covariant construction of a </span>thermodynamic equilibrium as a Legen-drian </span></span>submanifold<span><span>. This Legendrian submanifold is not necessarily graph-like. We interpret the </span>Maxwell construction of </span></span><em>equal-area law</em><span> as the procedure of finding a continuous, not necessarily differentiable, thermodynamic potential<span> and explain the associated phase transition by identifying the procedure with that of finding a graph selector in symplecto-contact geometry and in the Aubry-Mather theory of dynamical system.</span></span></p>","PeriodicalId":49630,"journal":{"name":"Reports on Mathematical Physics","volume":"43 2 1","pages":""},"PeriodicalIF":1.0000,"publicationDate":"2023-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Reports on Mathematical Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1016/s0034-4877(23)00084-8","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
引用次数: 0
Abstract
Both statistical phase space (SPS), which is Γ = T* 3N of N-body particle system, and kinetic theory phase space (KTPS), which is the cotangent bundle T* (Γ) of the probability space (Γ) thereon, carry canonical symplectic structures. Starting from this first principle, we provide a canonical derivation of thermodynamic phase space (TPS) of nonequilibrium thermodynamics as a contact manifold in two steps. First, regarding the collective observation of observables in SPS as a moment map defined on KTPS, we apply the Marsden–Weinstein reduction and obtain a mesoscopic phase space in between KTPS and TPS as a (infinite-dimensional) symplectic fibration. Then we show that the reduced relative information entropy defines a generating function that provides a covariant construction of a thermodynamic equilibrium as a Legen-drian submanifold. This Legendrian submanifold is not necessarily graph-like. We interpret the Maxwell construction of equal-area law as the procedure of finding a continuous, not necessarily differentiable, thermodynamic potential and explain the associated phase transition by identifying the procedure with that of finding a graph selector in symplecto-contact geometry and in the Aubry-Mather theory of dynamical system.
期刊介绍:
Reports on Mathematical Physics publish papers in theoretical physics which present a rigorous mathematical approach to problems of quantum and classical mechanics and field theories, relativity and gravitation, statistical physics, thermodynamics, mathematical foundations of physical theories, etc. Preferred are papers using modern methods of functional analysis, probability theory, differential geometry, algebra and mathematical logic. Papers without direct connection with physics will not be accepted. Manuscripts should be concise, but possibly complete in presentation and discussion, to be comprehensible not only for mathematicians, but also for mathematically oriented theoretical physicists. All papers should describe original work and be written in English.