{"id":68,"date":"2013-09-18T07:54:23","date_gmt":"2013-09-18T07:54:23","guid":{"rendered":"http:\/\/research.hip.fi\/hwp\/nucmat\/?page_id=68"},"modified":"2013-09-18T07:54:23","modified_gmt":"2013-09-18T07:54:23","slug":"mats","status":"publish","type":"page","link":"https:\/\/www.hip.fi\/nuclear-matter-programme\/mats\/","title":{"rendered":"MATS"},"content":{"rendered":"<h4>MATS<\/h4>\n<p>The recently developed phase-sensitive ion-cyclotron-frequency measurement technique allows a resolving power of up to 10<sup>8<\/sup>, corresponding to a few 100 eV, with a relative mass uncertainty at the 10<sup>\u221210<\/sup> level for nuclides with half-lives of only a few 10 ms. The successful completion of a single-ion detection method such as FT-ICR, will allow mass measurements on longer-lived nuclides produced with minute rates of one particle per day. Along with LaSpec, the first Penning-traps prototype of the MATS setup is also installed at the research reactor TRIGA at Mainz University. In-trap and trap-assisted spectroscopy experiments with dedicated setups are also foreseen in later stages.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>MATS The recently developed phase-sensitive ion-cyclotron-frequency measurement technique allows a resolving power of up to 108, corresponding to a few 100 eV, with a relative mass uncertainty at the 10\u221210 level for nuclides with half-lives of only a few 10 ms. The successful completion of a single-ion detection method such as FT-ICR, will allow mass [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-68","page","type-page","status-publish","hentry","post"],"_links":{"self":[{"href":"https:\/\/www.hip.fi\/nuclear-matter-programme\/wp-json\/wp\/v2\/pages\/68","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.hip.fi\/nuclear-matter-programme\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.hip.fi\/nuclear-matter-programme\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.hip.fi\/nuclear-matter-programme\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.hip.fi\/nuclear-matter-programme\/wp-json\/wp\/v2\/comments?post=68"}],"version-history":[{"count":0,"href":"https:\/\/www.hip.fi\/nuclear-matter-programme\/wp-json\/wp\/v2\/pages\/68\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.hip.fi\/nuclear-matter-programme\/wp-json\/wp\/v2\/media?parent=68"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}