{"id":81611,"date":"2024-11-22T15:31:24","date_gmt":"2024-11-22T14:31:24","guid":{"rendered":"https:\/\/wfa.uwr.edu.pl\/?p=81611"},"modified":"2024-11-22T15:31:30","modified_gmt":"2024-11-22T14:31:30","slug":"classification-of-non-lorentzian-quantum-symmetries-in-21-dimensions","status":"publish","type":"post","link":"https:\/\/wfa.uwr.edu.pl\/en\/2024\/11\/22\/classification-of-non-lorentzian-quantum-symmetries-in-21-dimensions\/","title":{"rendered":"Classification of non-Lorentzian quantum symmetries in 2+1 dimensions"},"content":{"rendered":"<h2 class=\"wp-block-post-title\">Classification of non-Lorentzian quantum symmetries in 2+1 dimensions<\/h2>\n\n\n<p>Space-time symmetries constitute a key component of fundamental physical theories, such as classic and quantum electrodynamics, or the general relativity theory (classic gravitational field theory). The most basic of them are described by the Lorentz group (for a non-zero cosmological constant, it generalizes to the de Sitter or anti-de Sitter group), keeping the value of the speed of light c. On the other hand, if we consider the so-called Galilei limit, where c tends to infinity, we reduce the given theory to classic Newtonian physics where time is absolute. The opposite option is taking the limit of c going to zero, known as the Carroll limit, which leads to ultralocal physics without a causal link between different points in space. Those two extreme cases that can be collectively called non-lorentzian recently became the object of active interest of theorists because they turn out to play an essential role in many advanced issues.<\/p>\n\n\n\n<figure class=\"wp-block-image aligncenter size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"419\" src=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-1024x419.jpg\" alt=\"Trze\u015bniewski\" class=\"wp-image-75900\" srcset=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-1024x419.jpg 1024w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-300x123.jpg 300w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-768x314.jpg 768w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-1536x629.jpg 1536w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-24x10.jpg 24w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-36x15.jpg 36w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-48x20.jpg 48w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-1320x540.jpg 1320w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2.jpg 1551w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\">Quantum contraptions combining all classes of (anti)de Sitter, (anti)de Sitter-Carroll and Carroll symmetry deformations<\/figcaption><\/figure>\n\n\n\n<p>Meanwhile, in the context of seeking the quantum gravity theory spacetime symmetry deformations are being introduced, which is enabled to us by the formalism of quantum groups. The paper <em>Quantum symmetries in 2+1 dimensions: Carroll, (a)dS-Carroll, Galilei and (a)dS-Galilei<\/em> by Tomasz Trze\u015bniewski, published in the Journal of High Energy Physics, generalises the Galilei and Carroll limits (using the quantum contractions procedure and adequate isomorphisms) into all the quantum symmetries identifiable for the 2+1-dimensional space-time with a zero, positive, or negative cosmological constant. The case of three dimensions is not just a test arena for working in four, but it is also interesting in its own right due to the gravity theory reduced to it, in which quantum symmetries already emerge on the classic level. <\/p>\n\n\n<div class=\"bs__links\">\r\n    <div class=\"bs__links__section\">\r\n        <ul class=\"bs__links__list\">\r\n                            <li class=\"bs__links__list__item\">\r\n                    <a href=\"https:\/\/link.springer.com\/article\/10.1007\/JHEP02(2024)200\" class=\"bs__links__list__item__link\">\r\n                        Link to the paper \r\n                        <div class=\"bs__links__list__item__link__before__icon\">\r\n                            <div class=\"bs__links__list__item__link__icon\">\r\n                                <svg width=\"40px\" height=\"40px\" viewBox=\"0 0 22 16\" version=\"1.1\">\r\n                                <g stroke=\"none\" strokeWidth=\"1\" fill=\"black\" fillRule=\"evenodd\">\r\n                                    <g>\r\n                                    <polygon points=\"13.4875 0 12 1.6215 18.7875 8 12 14.3795 13.4875 16 21.9995 8\" \/>\r\n                                    <\/g>\r\n                                <\/g>\r\n                                <\/svg>\r\n                            <\/div>\r\n                        <\/div>\r\n                    <\/a>\r\n                <li>\r\n                    <\/ul>\r\n    <\/div>\r\n<\/div>","protected":false},"excerpt":{"rendered":"<p>Space-time symmetries constitute a key component of fundamental physical theories, such as classic and quantum electrodynamics, or the general relativity theory (classic gravitational field theory). The most basic of them are described by the Lorentz group (for a non-zero cosmological constant, it generalizes to the de Sitter or anti-de Sitter group), keeping the value of [&hellip;]<\/p>\n","protected":false},"author":7182,"featured_media":75900,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"inline_featured_image":false,"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","ast-disable-related-posts":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"set","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"footnotes":""},"categories":[389],"tags":[392],"class_list":["post-81611","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-publikacje-en","tag-publikacje-en"],"featured_image_urls_v2":{"full":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2.jpg",1551,635,false],"thumbnail":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-150x150.jpg",150,150,true],"medium":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-300x123.jpg",300,123,true],"medium_large":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-768x314.jpg",768,314,true],"large":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-1024x419.jpg",1024,419,true],"1536x1536":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-1536x629.jpg",1536,629,true],"2048x2048":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2.jpg",1551,635,false],"menu-24x24":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-24x10.jpg",24,10,true],"menu-36x36":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-36x15.jpg",36,15,true],"menu-48x48":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2024\/05\/g2-48x20.jpg",48,20,true]},"post_excerpt_stackable_v2":"<p>Classification of non-Lorentzian quantum symmetries in 2+1 dimensions Space-time symmetries constitute a key component of fundamental physical theories, such as classic and quantum electrodynamics, or the general relativity theory (classic gravitational field theory). The most basic of them are described by the Lorentz group (for a non-zero cosmological constant, it generalizes to the de Sitter or anti-de Sitter group), keeping the value of the speed of light c. On the other hand, if we consider the so-called Galilei limit, where c tends to infinity, we reduce the given theory to classic Newtonian physics where time is absolute. The opposite option&hellip;<\/p>\n","category_list_v2":"<a href=\"https:\/\/wfa.uwr.edu.pl\/en\/category\/publikacje-en\/\" rel=\"category tag\">Publications<\/a>","author_info_v2":{"name":"kswistak","url":"https:\/\/wfa.uwr.edu.pl\/en\/author\/kswistak\/"},"comments_num_v2":"0 comments","acf":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.1.1 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Classification of non-Lorentzian quantum symmetries in 2+1 dimensions - Faculty of Physics and Astronomy<\/title>\n<meta name=\"description\" content=\"Wydzia\u0142 Fizyki i Astronomii\" \/>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/wfa.uwr.edu.pl\/en\/2024\/11\/22\/classification-of-non-lorentzian-quantum-symmetries-in-21-dimensions\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Classification of non-Lorentzian quantum symmetries in 2+1 dimensions - 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