{"id":303,"date":"2018-06-10T21:26:20","date_gmt":"2018-06-10T18:26:20","guid":{"rendered":"https:\/\/magneticmoments.info\/wp\/?p=303"},"modified":"2018-06-10T21:26:20","modified_gmt":"2018-06-10T18:26:20","slug":"probing-sizes-and-shapes-of-nobelium-isotopes-by-laser-spectroscopy","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=303","title":{"rendered":"Probing Sizes and Shapes of Nobelium Isotopes by Laser Spectroscopy"},"content":{"rendered":"<p><span style=\"caret-color: #222222; color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\">Until recently, ground-state nuclear moments of the heaviest nuclei could only be inferred from nuclear spectroscopy, where model assumptions are required. Laser spectroscopy in combination with modern atomic structure calculations is now able to probe these moments directly, in a comprehensive and nuclear-model-independent way. Here we report on unique access to the differential mean-square charge radii of\u00a0<\/span><span id=\"MathJax-Element-1-Frame\" class=\"mjx-chtml MathJax_CHTML\" style=\"box-sizing: border-box; display: inline-block; line-height: 0; font-size: 14.84000015258789px; word-wrap: normal; white-space: nowrap; float: none; direction: ltr; max-width: none; max-height: none; min-width: 0px; min-height: 0px; border: 0px; margin: 0px; padding: 1px 0px; caret-color: #222222; color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\" tabindex=\"0\"><span id=\"MJXc-Node-1\" class=\"mjx-math\" style=\"box-sizing: border-box; display: inline-block; border-collapse: separate; border-spacing: 0px;\"><span id=\"MJXc-Node-2\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-3\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-4\" class=\"mjx-mmultiscripts\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-presup\" style=\"display: inline-block; vertical-align: 0.435em; padding-left: 0.05em; padding-right: 0px; box-sizing: content-box !important;\"><span id=\"MJXc-Node-7\" class=\"mjx-mrow\" style=\"display: inline-block; font-size: 10.4918794631958px; box-sizing: content-box !important;\"><span id=\"MJXc-Node-8\" class=\"mjx-mn\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">252<\/span><\/span><span id=\"MJXc-Node-9\" class=\"mjx-mo\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; margin-top: -0.131em; padding-bottom: 0.542em; box-sizing: content-box !important;\">,<\/span><\/span><span id=\"MJXc-Node-10\" class=\"mjx-mn\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">253<\/span><\/span><span id=\"MJXc-Node-11\" class=\"mjx-mo\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; margin-top: -0.131em; padding-bottom: 0.542em; box-sizing: content-box !important;\">,<\/span><\/span><span id=\"MJXc-Node-12\" class=\"mjx-mn\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">254<\/span><\/span><\/span><\/span><span id=\"MJXc-Node-5\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-6\" class=\"mjx-mi\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">No<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/span><span style=\"caret-color: #222222; color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\">, and therefore to changes in nuclear size and shape. State-of-the-art nuclear density functional calculations describe well the changes in nuclear charge radii in the region of the heavy actinides, indicating an appreciable central depression in the deformed proton density distribution in\u00a0<\/span><span id=\"MathJax-Element-2-Frame\" class=\"mjx-chtml MathJax_CHTML\" style=\"box-sizing: border-box; display: inline-block; line-height: 0; font-size: 14.84000015258789px; word-wrap: normal; white-space: nowrap; float: none; direction: ltr; max-width: none; max-height: none; min-width: 0px; min-height: 0px; border: 0px; margin: 0px; padding: 1px 0px; caret-color: #222222; color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\" tabindex=\"0\"><span id=\"MJXc-Node-13\" class=\"mjx-math\" style=\"box-sizing: border-box; display: inline-block; border-collapse: separate; border-spacing: 0px;\"><span id=\"MJXc-Node-14\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-15\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-16\" class=\"mjx-mmultiscripts\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-presup\" style=\"display: inline-block; vertical-align: 0.435em; padding-left: 0.05em; padding-right: 0px; box-sizing: content-box !important;\"><span id=\"MJXc-Node-19\" class=\"mjx-mrow\" style=\"display: inline-block; font-size: 10.4918794631958px; box-sizing: content-box !important;\"><span id=\"MJXc-Node-20\" class=\"mjx-mn\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">252<\/span><\/span><span id=\"MJXc-Node-21\" class=\"mjx-mo\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; margin-top: -0.131em; padding-bottom: 0.542em; box-sizing: content-box !important;\">,<\/span><\/span><span id=\"MJXc-Node-22\" class=\"mjx-mn\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">254<\/span><\/span><\/span><\/span><span id=\"MJXc-Node-17\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-18\" class=\"mjx-mi\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">No<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/span><span style=\"caret-color: #222222; color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\">\u00a0isotopes. Finally, the hyperfine splitting of\u00a0<\/span><span id=\"MathJax-Element-3-Frame\" class=\"mjx-chtml MathJax_CHTML\" style=\"box-sizing: border-box; display: inline-block; line-height: 0; font-size: 14.84000015258789px; word-wrap: normal; white-space: nowrap; float: none; direction: ltr; max-width: none; max-height: none; min-width: 0px; min-height: 0px; border: 0px; margin: 0px; padding: 1px 0px; caret-color: #222222; color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\" tabindex=\"0\"><span id=\"MJXc-Node-23\" class=\"mjx-math\" style=\"box-sizing: border-box; display: inline-block; border-collapse: separate; border-spacing: 0px;\"><span id=\"MJXc-Node-24\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-25\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-26\" class=\"mjx-mmultiscripts\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-presup\" style=\"display: inline-block; vertical-align: 0.435em; padding-left: 0.05em; padding-right: 0px; box-sizing: content-box !important;\"><span id=\"MJXc-Node-29\" class=\"mjx-mrow\" style=\"display: inline-block; font-size: 10.4918794631958px; box-sizing: content-box !important;\"><span id=\"MJXc-Node-30\" class=\"mjx-mn\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">253<\/span><\/span><\/span><\/span><span id=\"MJXc-Node-27\" class=\"mjx-mrow\" style=\"display: inline-block; box-sizing: content-box !important;\"><span id=\"MJXc-Node-28\" class=\"mjx-mi\" style=\"display: inline-block; box-sizing: content-box !important;\"><span class=\"mjx-char MJXc-TeX-main-R\" style=\"display: block; white-space: pre; font-family: MJXc-TeX-main-R, MJXc-TeX-main-Rw; padding-top: 0.408em; padding-bottom: 0.34em; box-sizing: content-box !important;\">No<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/span><span style=\"caret-color: #222222; color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\">\u00a0was evaluated, enabling a complementary measure of its (quadrupole) deformation, as well as an insight into the neutron single-particle wave function via the nuclear spin and magnetic moment.<\/span><\/p>\n<p>\u00a0<\/p>\n<p><img class=\"lazy\" style=\"font-family: -webkit-standard;\" src=\"https:\/\/journals.aps.org\/prl\/article\/10.1103\/PhysRevLett.120.232503\/figures\/3\/medium\" alt=\"Figure 3\" data-original=\"\/prl\/article\/10.1103\/PhysRevLett.120.232503\/figures\/3\/medium\" \/><\/p>\n<p>Read the full article on <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.120.232503\" target=\"_blank\">Phys. Rev. Lett<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Until recently, ground-state nuclear moments of the heaviest nuclei could only be inferred from nuclear spectroscopy, where model assumptions are required. Laser spectroscopy in combination with modern atomic structure calculations is now able to probe these moments directly, in a&#46;&#46;&#46;<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"jetpack_publicize_message":"","jetpack_is_tweetstorm":false,"jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","enabled":false}}},"categories":[1],"tags":[302,303,9,8],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-4T","jetpack-related-posts":[{"id":113,"url":"https:\/\/magneticmoments.info\/wp\/?p=113","url_meta":{"origin":303,"position":0},"title":"[Conference paper] Physics highlights from laser spectroscopy at the IGISOL","date":"Mar 30, 2012","format":false,"excerpt":"Physics highlights from laser spectroscopy at the IGISOL D.H. 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