{"id":275,"date":"2026-01-28T08:57:04","date_gmt":"2026-01-28T07:57:04","guid":{"rendered":"https:\/\/www.idpoisson.fr\/barre\/?page_id=275"},"modified":"2026-01-28T09:28:34","modified_gmt":"2026-01-28T08:28:34","slug":"finite-size-fluctuations-in-complex-systems-a-large-deviation-approach","status":"publish","type":"page","link":"https:\/\/www.idpoisson.fr\/barre\/finite-size-fluctuations-in-complex-systems-a-large-deviation-approach\/","title":{"rendered":"Finite Size Fluctuations in Complex Systems : a Large Deviation Approach &#8211; CEFIPRA project"},"content":{"rendered":"<h1> Finite Size Fluctuations in Complex Systems : a Large Deviation Approach &#8211; CEFIPRA project <\/h1>\n\n<p><b>Co-PI: Shamik Gupta<\/b> TIFR Mumbai <\/p>\n<p> <b>Participants<\/b>: Rupak Majumder, Samir Sahoo, Anwar El Rhirhayi<br><br>Complex systems are usually modelled by a large number of coupled nonlinear Ordinary Differential Equations (ODEs) (or Stochastic Differential Equations -SDEs- if one takes ambient noise into account) involving the microscopic degrees of freedom. These equations, being nonlinear and coupled, are inevitably difficult to understand. <\/p>\n\n\n\n<p>It is then a well established strategy to describe the system in terms of one- particle, two-particle, &#8230; distribution functions, and to write down deterministic partial differential equations (PDEs) of kinetic or diffusive type for their evolution, which are valid in some large N limit. These distribution functions depend on all the microscopic degrees of freedom (e.g., position, velocity, some internal degree of freedom&#8230;), and hence are often still difficult to handle. The next step is to reduce the description further, taking advantage of small parameters at hand: it may be a small Knudsen number in classical kinetic theory, a small inertia yielding an overdamped approximation, or, a situation which will be of particular interest to us, a small bifurcation parameter near an instability, underpinning a center manifold reduction. In many application fields, among them spontaneous synchronization which will be a motivating example in the project, it is crucial to go beyond this infinite N, <em>deterministic<\/em> picture, and to account for finite-N fluctuations.<\/p>\n\n\nIllustration (joint work with Rupak Majumder and Shamik Gupta, 2025): combining center manifold expansion with Dean-Kawasaki equation to capture finite size fluctuations for a synchronization model. \n\n<figure class=\"wp-block-image size-medium\"><img decoding=\"async\" src=\"https:\/\/www.idpoisson.fr\/barre\/wp-content\/uploads\/sites\/20\/2026\/01\/Figure_Rupak.png\" alt=\"\" class=\"wp-image-158\" \/><\/figure>\n","protected":false},"excerpt":{"rendered":"<p>Finite Size Fluctuations in Complex Systems : a Large Deviation Approach &#8211; CEFIPRA project Co-PI: Shamik Gupta TIFR Mumbai Participants: &hellip; <a href=\"https:\/\/www.idpoisson.fr\/barre\/finite-size-fluctuations-in-complex-systems-a-large-deviation-approach\/\" class=\"more-link\">Plus <span class=\"screen-reader-text\">Finite Size Fluctuations in Complex Systems : a Large Deviation Approach &#8211; CEFIPRA project<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":7,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"folder":[],"class_list":["post-275","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/pages\/275","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/users\/7"}],"replies":[{"embeddable":true,"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/comments?post=275"}],"version-history":[{"count":13,"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/pages\/275\/revisions"}],"predecessor-version":[{"id":299,"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/pages\/275\/revisions\/299"}],"wp:attachment":[{"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/media?parent=275"}],"wp:term":[{"taxonomy":"folder","embeddable":true,"href":"https:\/\/www.idpoisson.fr\/barre\/wp-json\/wp\/v2\/folder?post=275"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}