{"id":87,"date":"2018-05-04T09:22:22","date_gmt":"2018-05-04T09:22:22","guid":{"rendered":"https:\/\/neutronstar.camk.edu.pl\/?page_id=87"},"modified":"2019-08-28T19:51:36","modified_gmt":"2019-08-28T19:51:36","slug":"latest-work","status":"publish","type":"page","link":"https:\/\/neutronstar.camk.edu.pl\/?page_id=87","title":{"rendered":"Latest work"},"content":{"rendered":"<p>This page will list projects completed during my Polonez fellowship.<\/p>\n<p><strong>Magneto-plastic dynamics of a highly-stressed neutron-star crust<\/strong><\/p>\n<p>X-ray bursts and gamma-ray flares from highly magnetised neutron stars rank among the most violent, energetic phenomena observed by astronomers.\u00a0 It is thought that the released energy from this activity was originally built up as stresses in the star&#8217;s crust as its magnetic field evolved.\u00a0 The neutron-star crust, like any elastic material, has a yield point &#8211; so, once the stresses get too high, the crust breaks.\u00a0 Or more accurately, it starts to deform plastically.<\/p>\n<figure id=\"attachment_106\" aria-describedby=\"caption-attachment-106\" style=\"width: 386px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-106 \" src=\"https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2019\/03\/R7_500_vx42.jpg\" alt=\"\" width=\"386\" height=\"289\" srcset=\"https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2019\/03\/R7_500_vx42.jpg 960w, https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2019\/03\/R7_500_vx42-300x224.jpg 300w, https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2019\/03\/R7_500_vx42-768x574.jpg 768w\" sizes=\"auto, (max-width: 386px) 100vw, 386px\" \/><figcaption id=\"caption-attachment-106\" class=\"wp-caption-text\">After 500 years, the segment of crust we simulate has built up enough stresses (through its magnetic-field evolution) to reach the elastic yield limit. It starts to flow plastically in the azimuthal direction, at a rate of some tens of centimetres per year. This would generate an exterior twist in the magnetosphere, as is thought to be necessary to explain magnetar bursts.<\/figcaption><\/figure>\n<p>For the first time in a quantitative model of the crust&#8217;s magnetic-field evolution, we were able to track the build-up of stresses, and the point at which the crust reached its yield point.\u00a0 After that, we solved for the way in which the magnetic field and the plastic flow evolve together.\u00a0 We found that the plastic motions at the surface are relatively fast &#8211; tens or hundreds of centimetres per year &#8211; and these would indeed be likely to induce flares and bursts outside the star.<\/p>\n<p>The final paper may be found <a href=\"https:\/\/academic.oup.com\/mnras\/article-abstract\/486\/3\/4130\/5449031?redirectedFrom=fulltext\">here<\/a>, or in preprint form <a href=\"https:\/\/arxiv.org\/abs\/1902.02121\">here.<\/a><\/p>\n<p><strong>Evolution of a neutron star&#8217;s inclination angle<\/strong><\/p>\n<figure id=\"attachment_94\" aria-describedby=\"caption-attachment-94\" style=\"width: 372px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-94\" src=\"https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2018\/08\/Screen-Shot-2018-08-05-at-16.17.46-300x243.png\" alt=\"\" width=\"372\" height=\"301\" srcset=\"https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2018\/08\/Screen-Shot-2018-08-05-at-16.17.46-300x243.png 300w, https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2018\/08\/Screen-Shot-2018-08-05-at-16.17.46-768x621.png 768w, https:\/\/neutronstar.camk.edu.pl\/wp-content\/uploads\/2018\/08\/Screen-Shot-2018-08-05-at-16.17.46.png 1068w\" sizes=\"auto, (max-width: 372px) 100vw, 372px\" \/><figcaption id=\"caption-attachment-94\" class=\"wp-caption-text\">A population of neutron stars, all with a birth inclination angle of 45 degrees, but with magnetic fields ranging from 10^12 to 10^16 gauss and initial spin frequencies from 0.1 to 1000 Hz.\u00a0 After a hundred years, a large portion of them have evolved so that their axes are orthogonal (O), with a region of highly-magnetised stars where the axes are aligned (A); the latter could not be seen as pulsars.\u00a0 On the colourscale are models where the angle has not finished evolving yet.<\/figcaption><\/figure>\n<p>Two of the most fundamental attributes of a neutron star &#8211; indeed, any star &#8211; are its rotation and its magnetic field.\u00a0 The axis about which a neutron star rotates is generally not the same as the symmetry axis for its magnetic field though; they are misaligned by some angle\u00a0\u03c7.\u00a0 Observationally, there are suggestions that: this angle decreases over million-year timescales, that the distribution is bimodal (with\u00a0\u03c7 close to either zero or ninety degrees), and that the value of\u00a0\u03c7 for the famous Crab pulsar may have increased by an observable amount since we first started observing it a few decades ago.\u00a0 Can all these observations be reconciled with one model?\u00a0 Do they make sense on theory grounds?<\/p>\n<p>It has been known since the 1970s that there are two competing physical mechanisms for the evolution of \u03c7 in a star; one acts to bring the two axes into alignment, and the other acts to orthogonalise them.\u00a0 We recently managed to assemble all the physical ingredients needed to study this problem quantitatively for the first time and showed how the final value of\u00a0\u03c7 for a highly-magnetised neutron star is probably fixed shortly after its birth, since the evolution of the angle is very quick.\u00a0 Many such stars will end up with almost-aligned rotation and magnetic axes.<\/p>\n<p>The final paper may be found <a href=\"https:\/\/academic.oup.com\/mnras\/article\/481\/3\/4169\/5104392\">here<\/a>, or in preprint form\u00a0<a href=\"https:\/\/arxiv.org\/abs\/1807.01289\">here<\/a>.<\/p>\n<p><span class=\"s1\"><b>Heat conduction in rotating relativistic stars<\/b><\/span><\/p>\n<p class=\"p2\">A quantitative understanding of the cooling of a young neutron star needs to allow for general relativity, and the star&#8217;s rotation.\u00a0 The equation which governs heat conduction for a star in general relativity looks virtually the same as its Newtonian equivalent, but both are parabolic: they predict that if the local temperature changes, that information is known immediately everywhere else.\u00a0 This would violate a basic principle of relativity, called causality: that nothing travels faster than light.<\/p>\n<p>Fortunately, we were able to show that by starting from a more general theory &#8211; which does satisfy causality &#8211; one can indeed derive the heat equation in its familiar form.\u00a0 The equation would have causal terms, but one can often assume that they act over such short timescales that their contribution is negligible.\u00a0 Rotation terms are also absent from the equation, unless the star rotates very fast.\u00a0 So, we got back to the expected form of the heat equation, but with an understanding of how and when this equation will cease to be valid (in more dynamical processes like the inspiral of two neutron stars, for example).<\/p>\n<p>The final paper may be found\u00a0<a href=\"https:\/\/academic.oup.com\/mnras\/article-abstract\/479\/3\/4207\/5046729\">here<\/a>, or in preprint form <a href=\"https:\/\/arxiv.org\/abs\/1804.01520\">here<\/a>.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>This page will list projects completed during my Polonez fellowship. Magneto-plastic dynamics of a highly-stressed neutron-star crust X-ray bursts and gamma-ray flares from highly magnetised neutron stars rank among the most violent, energetic phenomena observed by astronomers.\u00a0 It is thought that the released energy from this activity was originally built up as stresses in the &hellip; <\/p>\n<p class=\"link-more\"><a href=\"https:\/\/neutronstar.camk.edu.pl\/?page_id=87\" class=\"more-link\">Continue reading<span class=\"screen-reader-text\"> &#8220;Latest work&#8221;<\/span><\/a><\/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-87","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=\/wp\/v2\/pages\/87","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=87"}],"version-history":[{"count":10,"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=\/wp\/v2\/pages\/87\/revisions"}],"predecessor-version":[{"id":114,"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=\/wp\/v2\/pages\/87\/revisions\/114"}],"wp:attachment":[{"href":"https:\/\/neutronstar.camk.edu.pl\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=87"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}