{"id":2530,"date":"2024-02-17T09:44:59","date_gmt":"2024-02-17T08:44:59","guid":{"rendered":"https:\/\/www.mr-physik.med.fau.de\/?p=2530"},"modified":"2024-02-19T09:46:49","modified_gmt":"2024-02-19T08:46:49","slug":"neues-paper-fast-online-spectral-spatial-pulse-design-for-subject-specific-fat-saturation-in-cervical-spine-and-foot-imaging-at-1-5-t","status":"publish","type":"post","link":"https:\/\/www.mr-physik.med.fau.de\/en\/2024\/02\/17\/neues-paper-fast-online-spectral-spatial-pulse-design-for-subject-specific-fat-saturation-in-cervical-spine-and-foot-imaging-at-1-5-t\/","title":{"rendered":"New Paper: Fast online spectral-spatial pulse design for subject-specific fat saturation in cervical spine and foot imaging at 1.5 T"},"content":{"rendered":"<p>Congratulations to <a href=\"https:\/\/www.mr-physik.med.fau.de\/en\/team\/christian-eisen\/\">Christian Eisen<\/a> (and colleagues) on the recently published paper &#8220;Fast online spectral-spatial pulse design for subject-specific fat saturation in cervical spine and foot imaging at 1.5 T&#8221;!<\/p>\n<p>A new fat saturation method for MRI is presented, which aims to ensure a more reliable and uniform suppression of the fat signal. Essentially, the method consists of calculating a dynamic 1-channel pulse based on the actual magnetic field distribution, which is simultaneously applied with pre-optimized gradients. Read more here:<br \/>\n<a href=\"https:\/\/www.springermedizin.de\/fast-online-spectral-spatial-pulse-design-for-subject-specific-f\/26745740\">https:\/\/www.springermedizin.de\/fast-online-spectral-spatial-pulse-design-for-subject-specific-f\/26745740<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Congratulations to Christian Eisen (and colleagues) on the recently published paper &#8220;Fast online spectral-spatial pulse design for subject-specific fat saturation in cervical spine and foot imaging at 1.5 T&#8221;! A new fat saturation method for MRI is presented, which aims to ensure a more reliable and uniform suppression of the fat signal. Essentially, the method [&hellip;]<\/p>\n","protected":false},"author":3987,"featured_media":2528,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_rrze_cache":"enabled","_rrze_multilang_single_locale":"en_US","_rrze_multilang_single_source":"https:\/\/www.mr-physik.med.fau.de\/?p=2525","_faue_teaser_image_id":0,"footnotes":""},"categories":[20,1,21],"tags":[],"class_list":["post-2530","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-ag-nagel","category-allgemein","category-startseite","en-US"],"faue_teaser_image_url":"","_links":{"self":[{"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/posts\/2530","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/users\/3987"}],"replies":[{"embeddable":true,"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/comments?post=2530"}],"version-history":[{"count":2,"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/posts\/2530\/revisions"}],"predecessor-version":[{"id":2948,"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/posts\/2530\/revisions\/2948"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/media\/2528"}],"wp:attachment":[{"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/media?parent=2530"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/categories?post=2530"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.mr-physik.med.fau.de\/wp-json\/wp\/v2\/tags?post=2530"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}