{"id":304202,"date":"2016-10-17T17:00:00","date_gmt":"2016-10-17T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=0e7497893b30c4aa2d11684e5c7ff6bf"},"modified":"2016-10-17T17:00:00","modified_gmt":"2016-10-17T14:00:00","slug":"first-measurement-of-collectivity-of-coexisting-shapes-based-on-type-ii-shell-evolution-the-case-of-96-zr","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=304202","title":{"rendered":"First Measurement of Collectivity of Coexisting Shapes Based on Type II Shell Evolution: The Case of ^{96} Zr"},"content":{"rendered":"<p>Author(s): C. Kremer, S. Aslanidou, S. Bassauer, M. Hilcker, A. Krugmann, P. von Neumann-Cosel, T. Otsuka, N. Pietralla, V. Yu. Ponomarev, N. Shimizu, M. Singer, G. Steinhilber, T. Togashi, Y. Tsunoda, V. Werner, and M. Zweidinger<\/p>\n<p>High-resolution inelastic electron scattering on <math xmlns=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><msup><mrow><\/mrow><mn>96<\/mn><\/msup><\/math>Zr establishes shape coexistence\u2014where two nearby states possess distinct shapes\u2014for this nucleus. Monte Carlo shell-model calculations indicate that the shape change in Zr isotopes is a quantum phase transition.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.117.172503.png\" width=\"200\" height=\"100\"><\/p>\n<p>[Phys. Rev. Lett. 117, 172503] Published Mon Oct 17, 2016<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): C. Kremer, S. Aslanidou, S. Bassauer, M. Hilcker, A. Krugmann, P. von Neumann-Cosel, T. Otsuka, N. Pietralla, V. Yu. Ponomarev, N. Shimizu, M. Singer, G. Steinhilber, T. Togashi, Y. Tsunoda, V. Werner, and M. Zweidinger<\/p>\n<p>High-resolution inelastic electron scattering on 96Zr establishes shape coexistence&mdash;where two nearby states possess distinct shapes&mdash;for this nucleus. Monte Carlo shell-model calculations indicate that the shape change in Zr isotopes is a quantum phase transition.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.117.172503.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 117, 172503] Published Mon Oct 17, 2016<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"categories":[182],"tags":[],"class_list":{"0":"post-304202","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-rss-teadus","7":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/304202","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=304202"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/304202\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=304202"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=304202"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=304202"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}