{"id":228,"date":"2026-08-20T15:17:11","date_gmt":"2026-08-20T15:17:11","guid":{"rendered":"http:\/\/www.pulsars.info\/wordpress\/?p=228"},"modified":"2026-08-20T15:21:19","modified_gmt":"2026-08-20T15:21:19","slug":"a-connection-between-proto-neutron-star-tayler-spruit-dynamos-and-low-field-magnetars","status":"publish","type":"post","link":"http:\/\/www.pulsars.info\/wordpress\/uncategorized\/a-connection-between-proto-neutron-star-tayler-spruit-dynamos-and-low-field-magnetars\/","title":{"rendered":"A connection between proto-neutron-star Tayler-Spruit dynamos and low-field magnetars"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">Igoshev, Andrei, Barr\u00e8re, Paul, Raynaud, Rapha\u00ebl, Guilet, J\u00e9rome, Wood, Toby, Hollerbach, Rainer\u00a0<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><span style=\"font-size: 16px; white-space: normal; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">Low-field magnetars have dipolar magnetic fields of 10<\/span><span style=\"white-space: normal; box-sizing: border-box; font-size: 12px; line-height: 0; position: relative; vertical-align: baseline; top: -0.5em; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">12<\/span><span style=\"font-size: 16px; white-space: normal; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">-10<\/span><span style=\"white-space: normal; box-sizing: border-box; font-size: 12px; line-height: 0; position: relative; vertical-align: baseline; top: -0.5em; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">13<\/span><span style=\"font-size: 16px; white-space: normal; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">\u00a0G, 10-100 times weaker than the values of magnetic-field strength B \u2248 10<\/span><span style=\"white-space: normal; box-sizing: border-box; font-size: 12px; line-height: 0; position: relative; vertical-align: baseline; top: -0.5em; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">14<\/span><span style=\"font-size: 16px; white-space: normal; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">-10<\/span><span style=\"white-space: normal; box-sizing: border-box; font-size: 12px; line-height: 0; position: relative; vertical-align: baseline; top: -0.5em; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">15<\/span><span style=\"font-size: 16px; white-space: normal; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">\u00a0G used to define classical magnetars, yet they produce similar X-ray bursts and outbursts. Using direct numerical simulations of magnetothermal evolution starting from a dynamo-generated magnetic field, we show that the low-field magnetars can be produced as a result of a Tayler-Spruit dynamo inside a proto-neutron star. We find that these simulations naturally explain key characteristics of low-field magnetars: weak (\u227210<\/span><span style=\"white-space: normal; box-sizing: border-box; font-size: 12px; line-height: 0; position: relative; vertical-align: baseline; top: -0.5em; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">13<\/span><span style=\"font-size: 16px; white-space: normal; caret-color: rgb(93, 93, 93); color: rgb(93, 93, 93); font-family: &quot;Helvetica Neue&quot;, Helvetica, Arial, sans-serif;\">\u00a0G) dipolar magnetic fields, strong small-scale fields and magnetically induced crustal failures producing X-ray bursts. These findings suggest that the formation channel of low-B magnetars is distinct from that for classical magnetars, reflecting potential differences in proto-neutron-star dynamos.<\/span><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><a href=\"https:\/\/ui.adsabs.harvard.edu\/link_gateway\/2025NatAs...9..541I\/doi:10.1038\/s41550-025-02477-y\">NA article<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Igoshev, Andrei, Barr\u00e8re, Paul, Raynaud, Rapha\u00ebl, Guilet, J\u00e9rome, Wood, Toby, Hollerbach, Rainer\u00a0 Low-field magnetars have dipolar magnetic fields of 1012-1013\u00a0G, 10-100 times weaker than the values of magnetic-field strength B \u2248 1014-1015\u00a0G used to define classical magnetars, yet they produce similar X-ray bursts and outbursts. Using direct numerical simulations of magnetothermal evolution starting from a &#8230; <a title=\"A connection between proto-neutron-star Tayler-Spruit dynamos and low-field magnetars\" class=\"read-more\" href=\"http:\/\/www.pulsars.info\/wordpress\/uncategorized\/a-connection-between-proto-neutron-star-tayler-spruit-dynamos-and-low-field-magnetars\/\" aria-label=\"Read more about A connection between proto-neutron-star Tayler-Spruit dynamos and low-field magnetars\">Read more<\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-228","post","type-post","status-publish","format-standard","hentry","category-uncategorized"],"_links":{"self":[{"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/posts\/228","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/comments?post=228"}],"version-history":[{"count":1,"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/posts\/228\/revisions"}],"predecessor-version":[{"id":229,"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/posts\/228\/revisions\/229"}],"wp:attachment":[{"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/media?parent=228"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/categories?post=228"},{"taxonomy":"post_tag","embeddable":true,"href":"http:\/\/www.pulsars.info\/wordpress\/wp-json\/wp\/v2\/tags?post=228"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}