{"id":259,"date":"2016-08-05T19:22:35","date_gmt":"2016-08-05T19:22:35","guid":{"rendered":"http:\/\/girsh.rutgers.edu\/?p=259"},"modified":"2018-09-13T19:32:24","modified_gmt":"2018-09-13T19:32:24","slug":"bafe2as0-5p0-52","status":"publish","type":"post","link":"https:\/\/girsh.rutgers.edu\/index.php\/2016\/08\/05\/bafe2as0-5p0-52\/","title":{"rendered":"Collective excitations of dynamic Fermi surface deformations in BaFe2(As0.5P0.5)2"},"content":{"rendered":"<p style=\"text-align: left;\"><img fetchpriority=\"high\" decoding=\"async\" class=\"alignright size-medium wp-image-281\" src=\"http:\/\/girsh.rutgers.edu\/wp-content\/uploads\/2016\/08\/For-website-front-page-173x300.png\" alt=\"For website front page\" width=\"173\" height=\"300\" srcset=\"https:\/\/girsh.rutgers.edu\/wp-content\/uploads\/2016\/08\/For-website-front-page-173x300.png 173w, https:\/\/girsh.rutgers.edu\/wp-content\/uploads\/2016\/08\/For-website-front-page-768x1329.png 768w, https:\/\/girsh.rutgers.edu\/wp-content\/uploads\/2016\/08\/For-website-front-page-592x1024.png 592w, https:\/\/girsh.rutgers.edu\/wp-content\/uploads\/2016\/08\/For-website-front-page-960x1661.png 960w, https:\/\/girsh.rutgers.edu\/wp-content\/uploads\/2016\/08\/For-website-front-page.png 1904w\" sizes=\"(max-width: 173px) 100vw, 173px\" \/><strong>Authors:<\/strong> S.-F. Wu, W.-L. Zhang, D. Hu, H.-H. Kung, A. Lee, H.-C. Mao, P.-C. Dai, H. Ding, P. Richard and G. Blumberg<\/p>\n<p style=\"text-align: left;\"><strong>Abstract:<\/strong><\/p>\n<div data-canvas-width=\"233.529888\">We use electronic Raman scattering to study the low-energy excitations in BaFe<sub>2<\/sub>(As<sub>0.5<\/sub>P<sub>0.5<\/sub>)<sub>2<\/sub> (Tc\u224816 K) samples. In addition to a superconducting pair breaking peak (2\u0394=6.7 meV) in the A<sub>1g<\/sub> channel with a linear tail towards zero energy, suggesting a nodal gap structure, we detect spectral features associated to Pomeranchuk oscillations in the A<sub>1g<\/sub>, B<sub>1g<\/sub> and B<sub>2g<\/sub> channels. We argue that the small Fermi energy of the system is an essential condition for these Pomeranchuk oscillations to be underdamped. The Pomeranchuk oscillations have the same frequencies in the B<sub>1g<\/sub> and B<sub>2g<\/sub> channels, which we explain by the mixing of these symmetries resulting from the removal of the \u03c3<sub>v<\/sub> and \u03c3<sub>d<\/sub> symmetry planes due to a large As\/P disorder. Interestingly, we show that the temperature at which the peaks corresponding to the Pomeranchuk oscillations get underdamped is consistent with the non-Fermi liquid to Fermi liquid crossover determined by transport, suggesting that the Pomeranchuk instability plays an important role in the low-energy physics of the Fe-based superconductors.<\/div>\n<div data-canvas-width=\"233.529888\"><\/div>\n<ul>\n<li><em><a href=\"http:\/\/girsh.rutgers.edu\/wp-content\/uploads\/2016\/03\/1607.06575v1.pdf\" target=\"_blank\">Read preprint here (PDF)<\/a><\/em><\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>Authors: S.-F. Wu, W.-L. Zhang, D. Hu, H.-H. Kung, A. Lee, H.-C. Mao, P.-C. Dai, H. Ding, P. Richard and G. Blumberg Abstract: We use electronic Raman scattering to study the low-energy excitations in BaFe2(As0.5P0.5)2 (Tc\u224816 K) samples. In addition to a superconducting pair breaking peak (2\u0394=6.7 meV) in the A1g channel with a linear &hellip;<\/p>\n<p class=\"read-more\"> <a class=\"\" href=\"https:\/\/girsh.rutgers.edu\/index.php\/2016\/08\/05\/bafe2as0-5p0-52\/\"> <span class=\"screen-reader-text\">Collective excitations of dynamic Fermi surface deformations in BaFe2(As0.5P0.5)2<\/span> Read More &raquo;<\/a><\/p>\n","protected":false},"author":2,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"_links":{"self":[{"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/posts\/259"}],"collection":[{"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/comments?post=259"}],"version-history":[{"count":11,"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/posts\/259\/revisions"}],"predecessor-version":[{"id":799,"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/posts\/259\/revisions\/799"}],"wp:attachment":[{"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/media?parent=259"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/categories?post=259"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/girsh.rutgers.edu\/index.php\/wp-json\/wp\/v2\/tags?post=259"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}