{"id":3835,"date":"2016-11-25T08:12:16","date_gmt":"2016-11-25T07:12:16","guid":{"rendered":"http:\/\/physics.uwb.edu.pl\/wf\/?page_id=3835"},"modified":"2016-11-25T08:13:29","modified_gmt":"2016-11-25T07:13:29","slug":"thermal-solitons-as-revealed-by-static-structure-factor","status":"publish","type":"page","link":"https:\/\/physics.uwb.edu.pl\/wf\/?page_id=3835","title":{"rendered":"Thermal solitons as revealed by static structure factor"},"content":{"rendered":"<p>Dnia <b>2016-11-29<\/b> o godzinie <b>12:15<\/b> w sali 2<b>011<\/b> odb\u0119dzie si\u0119 seminarium, na kt\u00f3rym dr Krzysztof Gawryluk wyg\u0142osi referat pt:<\/p>\n<p style=\"text-align: center;\"><b><strong>Thermal solitons as revealed by static structure factor<\/strong><\/b><\/p>\n<p lang=\"en-GB\" align=\"JUSTIFY\">We study, within a framework of the classical fields approximation, the static structure factor of a weakly interacting Bose gas at thermal equilibrium. As in a recent experiment (R. Schley et al., Phys. Rev. Lett. 111, 055301 (2013)), we find that the thermal distribution of phonons in a three-dimensional Bose gas follows the Planck distribution. We find as well a disagreement between the Planck and phonon distributions in the case of elongated quasi-one-dimensional systems. We attribute this discrepancy to the existence of spontaneous dark solitons (i.e., thermal solitons as reported in T. Karpiuk et al., Phys. Rev. Lett. 109, 205302 (2012)) in an elongated Bose gas at thermal equilibrium.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Dnia 2016-11-29 o godzinie 12:15 w sali 2011 odb\u0119dzie si\u0119 seminarium, na kt\u00f3rym dr Krzysztof Gawryluk wyg\u0142osi referat pt: Thermal solitons as revealed by static structure factor We study, within <a href=\"https:\/\/physics.uwb.edu.pl\/wf\/?page_id=3835\" class=\"more-link\">[&hellip;]<\/a><\/p>\n","protected":false},"author":9,"featured_media":3366,"parent":822,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"ngg_post_thumbnail":0,"Layout":"","footnotes":""},"categories":[69],"tags":[],"class_list":["entry","author-","post-3835","page","type-page","status-publish","has-post-thumbnail","category-seminarium_pl"],"jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/P7nvcn-ZR","_links":{"self":[{"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/pages\/3835","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/users\/9"}],"replies":[{"embeddable":true,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=3835"}],"version-history":[{"count":3,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/pages\/3835\/revisions"}],"predecessor-version":[{"id":3838,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/pages\/3835\/revisions\/3838"}],"up":[{"embeddable":true,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/pages\/822"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=\/wp\/v2\/media\/3366"}],"wp:attachment":[{"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=3835"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=3835"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/physics.uwb.edu.pl\/wf\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=3835"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}