{"id":7348,"date":"2022-06-17T19:25:13","date_gmt":"2022-06-17T17:25:13","guid":{"rendered":"https:\/\/www.lapth.cnrs.fr\/?page_id=7348"},"modified":"2026-03-20T11:16:31","modified_gmt":"2026-03-20T10:16:31","slug":"theoretical-physics","status":"publish","type":"page","link":"https:\/\/www.lapth.cnrs.fr\/en\/research-areas\/theoretical-physics\/","title":{"rendered":"Mathematical physics"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"7348\" class=\"elementor elementor-7348\" data-elementor-post-type=\"page\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-61d6a9c elementor-section-full_width elementor-section-height-min-height elementor-section-height-default elementor-section-items-middle\" data-id=\"61d6a9c\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-d107d27 elementor-hidden-tablet elementor-hidden-phone\" data-id=\"d107d27\" data-element_type=\"column\" data-e-type=\"column\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-a23d9c2 elementor-widget elementor-widget-spacer\" data-id=\"a23d9c2\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-98f481d\" data-id=\"98f481d\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-inner-section elementor-element elementor-element-99d9754 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"99d9754\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-inner-column elementor-element elementor-element-836a110\" data-id=\"836a110\" data-element_type=\"column\" data-e-type=\"column\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-5819e6c7 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"5819e6c7\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-31125670\" data-id=\"31125670\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-inner-section elementor-element elementor-element-20b9d0a7 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"20b9d0a7\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-inner-column elementor-element elementor-element-254e10ad\" data-id=\"254e10ad\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-7aea7393 elementor-widget elementor-widget-image\" data-id=\"7aea7393\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"775\" height=\"366\" src=\"https:\/\/www.lapth.cnrs.fr\/wp-content\/uploads\/2022\/04\/physmat.jpg\" class=\"attachment-full size-full wp-image-5924\" alt=\"\" srcset=\"https:\/\/www.lapth.cnrs.fr\/wp-content\/uploads\/2022\/04\/physmat.jpg 775w, https:\/\/www.lapth.cnrs.fr\/wp-content\/uploads\/2022\/04\/physmat-300x142.jpg 300w, https:\/\/www.lapth.cnrs.fr\/wp-content\/uploads\/2022\/04\/physmat-768x363.jpg 768w\" sizes=\"(max-width: 775px) 100vw, 775px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-1e7b1ca0\" data-id=\"1e7b1ca0\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-4864017a elementor-widget elementor-widget-text-editor\" data-id=\"4864017a\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t\t\t\t\t\t<p>Staff members : D. Andriot, D. Chicherin, L. Gallot, G. Parez, E. Ragoucy, F. Thuillier and P. Tourkine.<\/p><p>Postdoc: M. G\u00fcmus<\/p><p>Temporary Researcher: S. Pakuliak.<\/p><p>PhD students: M. Dabrowski, D. Leflot, H. Quillet, M. Tagaris et A. Villey.<\/p><p>Emeritus : L. Frappat, E. Sokatchev et P. Sorba.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-6a56afab elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"6a56afab\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-3857164b\" data-id=\"3857164b\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-2d2a03df elementor-widget elementor-widget-heading\" data-id=\"2d2a03df\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Mathematical physics - Symmetries- Integrable systems and their applications- Field theory and string theory<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-5a0854df elementor-widget elementor-widget-text-editor\" data-id=\"5a0854df\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t\t\t\t\t\t<p>The mathematical physics team has gained international recognition in three major areas: gauge theories (particularly supersymmetric Yang-Mills gauge theories), string theories, and integrable systems.<\/p><p>Supersymmetric gauge theories are field theories that have a local symmetry group (dependent on position in space) as well as supersymmetry (which connects bosons and fermions). Physical quantities are calculated from diffusion amplitudes. String theories are very strong candidates for unifying gravitation with particle physics. Finally, integrable systems have a very rigid mathematical structure which makes it possible to calculate exactly (non-perturbatively) the physical quantities (here called correlation functions) of the model that we are studying. Over the past years, the team has achieved excellent results in each of these fields. It should be noted that these three areas are closely related. On one hand, gauge theories and string theories are dual, meaning that it is possible to switch between them by exchanging regimes of weak or strong coupling. On the other hand, some of these theories possess integrable parts and are sometimes assumed to be completely integrable.<\/p><p>Regarding supersymmetric gauge theories, the team is recognized as a leader in the calculation of scattering amplitudes, in relation to particle physics. They work on perturbative and non-perturbative aspects (including via the bootstrap) of scattering amplitudes and S-matrices in field theory and quantum gravity.<\/p><p>The group has also expanded into the field of string theory, which offers a perspective to include gravity in particle physics. The researchers seek to establish connections between string theory and phenomenology, especially with cosmology, in relation to the Swampland program. Their goal is to obtain de Sitter solutions, as well as other cosmological models, from string theory in order to explain dark energy responsible for the accelerated expansion of our universe.<\/p><p>In the field of integrable systems, the team is leader in the calculation of correlation functions of spin chains, within the framework of the algebraic Bethe ansatz. They have a strong expertise in the theory of Lie algebras and integrable field theory. They also develop the study of integrability in statistical physics of non-equilibrium systems, a generalization of usual thermodynamics.More mathematical aspects are also covered, such as the construction of orthogonal polynomials with several variables, or the study of Hopf algebras.<\/p><p>Finally, the team also conducts research in the fields of topological field theories, addressing more formal aspects of field theory with developments in both mathematics and physics, as well as classical gravitational field theories, including the construction of stationary solutions describing black holes in general relativity.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Staff members : D. Andriot, D. Chicherin, L. Gallot, G. Parez, E. Ragoucy, F. Thuillier and P. Tourkine. Postdoc: M. G\u00fcmus Temporary Researcher: S. Pakuliak. PhD students: M. Dabrowski, D. [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":6782,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"footnotes":""},"class_list":["post-7348","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/7348","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/comments?post=7348"}],"version-history":[{"count":12,"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/7348\/revisions"}],"predecessor-version":[{"id":17532,"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/7348\/revisions\/17532"}],"up":[{"embeddable":true,"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/6782"}],"wp:attachment":[{"href":"https:\/\/www.lapth.cnrs.fr\/en\/wp-json\/wp\/v2\/media?parent=7348"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}