{"id":778650,"date":"2024-03-11T08:51:54","date_gmt":"2024-03-11T13:51:54","guid":{"rendered":"http:\/\/spaceweekly.com\/?p=778650"},"modified":"2024-03-11T08:51:54","modified_gmt":"2024-03-11T13:51:54","slug":"maximum-mass-of-non-rotating-neutron-star-precisely-inferred-to-be-2-25-solar-masses","status":"publish","type":"post","link":"https:\/\/spaceweekly.com\/?p=778650","title":{"rendered":"Maximum mass of non-rotating neutron star precisely inferred to be 2.25 solar masses"},"content":{"rendered":"<p> <br \/>\n<\/p>\n<div>\n<div class=\"article-gallery lightGallery\">\n<div data-thumb=\"https:\/\/scx1.b-cdn.net\/csz\/news\/tmb\/2024\/maximum-mass-of-non-ro.jpg\" data-src=\"https:\/\/scx2.b-cdn.net\/gfx\/news\/2024\/maximum-mass-of-non-ro.jpg\" data-sub-html=\"The red line represents the best-fit mass distribution, i.e., a two-component Gaussian mixture with a sharp cutoff of M&lt;sub&gt;max&lt;\/sub&gt;=2.28M\u2299, of the 136 neutron stars with gravitational mass measurements. Here we take 1,000 independent posterior samples (the gray lines) to give a visual guide for the uncertainties. The inset shows P(M&lt;sub&gt;max&lt;\/sub&gt;), the posterior distribution of M&lt;sub&gt;max&lt;\/sub&gt;. Credit: &lt;i&gt;Physical Review D&lt;\/i&gt; (2024). DOI: 10.1103\/PhysRevD.109.043052\">\n<figure class=\"article-img\">\n            <figcaption class=\"text-darken text-low-up text-truncate-js text-truncate mt-3\">\n                The red line represents the best-fit mass distribution, i.e., a two-component Gaussian mixture with a sharp cutoff of M<sub>max<\/sub>=2.28M\u2299, of the 136 neutron stars with gravitational mass measurements. Here we take 1,000 independent posterior samples (the gray lines) to give a visual guide for the uncertainties. The inset shows P(M<sub>max<\/sub>), the posterior distribution of M<sub>max<\/sub>. Credit: <i>Physical Review D<\/i> (2024). DOI: 10.1103\/PhysRevD.109.043052<br \/>\n            <\/figcaption><\/figure>\n<\/p><\/div>\n<\/div>\n<p>A study led by Prof. Fan Yizhong from the Purple Mountain Observatory of the Chinese Academy of Sciences has achieved significant precision in determining the upper mass limit for non-rotating neutron stars, a pivotal aspect in the study of nuclear physics and astrophysics.<\/p>\n<section class=\"article-banner first-banner ads-336x280\">\n         <!-- \/4988204\/Phys_Story_InText_Box --><\/p>\n<\/section>\n<p>The researchers showed that the maximum gravitational mass of a non-rotating neutron star is approximately 2.25 solar masses with an uncertainty of just 0.07 solar mass. Their study is published in <i>Physical Review D<\/i>.<\/p>\n<p>The ultimate fate of a massive star is intricately linked to its mass. Stars lighter than eight solar masses end their life cycle as white dwarfs, supported by electron degeneracy pressure with a well-known upper mass limit, the Chandrasekhar limit, near 1.4 solar masses.<\/p>\n<p>For stars heavier than eight but lighter than 25 solar masses, neutron stars will be produced, which instead, are mainly upheld by neutron degeneracy pressure. For non-rotating neutron stars, there is also a critical gravitational mass (i.e., M<sub>TOV<\/sub>) known as the Oppenheimer limit, above which the neutron star will collapse into a black hole.<\/p>\n<p>Establishing a precise Oppenheimer limit is quite challenging. Only loose bounds can be set based on the first principle. Many specific evaluations are strongly model-dependent. The resulting M<sub>TOV<\/sub> are diverse and the uncertainties are large.<\/p>\n<p>Prof. Fan&#8217;s team has refined the inference of M<sub>TOV<\/sub> by incorporating robust multi-messenger observations and reliable nuclear physics data, circumventing the uncertainties present in earlier models. This includes leveraging recent advancements in mass\/radius measurements from LIGO\/Virgo gravitational-wave detectors and the Neutron star Interior Composition Explorer (NICER).<\/p>\n<p>In particular, they incorporated the information of the maximum mass cutoff inferred from the neutron star mass distribution and significantly narrowed the parameter space, leading to an unprecedented precision in the inferred M<sub>TOV<\/sub>. Three diverse equation of state (EoS) reconstruction models were employed to mitigate potential systematic errors, yielding almost identical results for M<sub>TOV<\/sub> and the corresponding radius, which is 11.9 km with an uncertainty of 0.6 km in three independent EoS reconstruction approaches.<\/p>\n<p>The precise evaluation of M<sub>TOV<\/sub> carries profound implications for both nuclear physics and astrophysics. It indicates a moderately stiff EoS for neutron star matter and suggests that the compact objects with masses in the range of approximately 2.5 to 3.0 solar masses, detected by LIGO\/Virgo, are more likely to be the lightest black holes. Furthermore, the merger remnants of binary neutron star systems exceeding a total mass of roughly 2.76 solar masses would collapse into black holes, while lighter systems would result in the formation of (supramassive) neutron stars.<\/p>\n<div class=\"article-main__more p-4\">\n<p><strong>More information:<\/strong><br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tYi-Zhong Fan et al, Maximum gravitational mass MTOV=2.25\u22120.07+0.08M\u2299 inferred at about 3% precision with multimessenger data of neutron stars, <i>Physical Review D<\/i> (2024). DOI: 10.1103\/PhysRevD.109.043052. On <i>arXiv<\/i>: DOI: 10.48550\/arxiv.2309.12644<\/p>\n<\/p><\/div>\n<div class=\"d-inline-block text-medium mt-4\">\n<p>\n\t\t\t\t\t\t\t\t\t\t\t\t\tProvided by<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\tChinese Academy of Sciences<\/p>\n<p>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<svg>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<use href=\"https:\/\/phys.b-cdn.net\/tmpl\/v6\/img\/svg\/sprite.svg#icon_open\" x=\"0\" y=\"0\"\/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/svg><\/p>\n<\/p><\/div>\n<p>\t\t\t\t\t\t\t\t\t\t<!-- print only --><\/p>\n<div class=\"d-none d-print-block\">\n<p>\n\t\t\t\t\t\t\t\t\t\t\t\t<strong>Citation<\/strong>:<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tMaximum mass of non-rotating neutron star precisely inferred to be 2.25 solar masses (2024, March 11)<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tretrieved 11 March 2024<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tfrom\n\t\t\t\t\t\t\t\t\t\t\t <\/p>\n<p>\n\t\t\t\t\t\t\t\t\t\t\t This document is subject to copyright. Apart from any fair dealing for the purpose of private study or research, no<br \/>\n\t\t\t\t\t\t\t\t\t\t\t part may be reproduced without the written permission. The content is provided for information purposes only.\n\t\t\t\t\t\t\t\t\t\t\t <\/p>\n<\/p><\/div>\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"https:\/\/phys.org\/news\/2024-03-maximum-mass-rotating-neutron-star.html\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>The red line represents the best-fit mass distribution, i.e., a two-component Gaussian mixture with a sharp cutoff of Mmax=2.28M\u2299, of the 136 neutron stars with gravitational mass measurements. Here we&hellip; <\/p>\n","protected":false},"author":1,"featured_media":778651,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[41],"tags":[],"class_list":["post-778650","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-phys-org"],"_links":{"self":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/778650","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=778650"}],"version-history":[{"count":0,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/posts\/778650\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=\/wp\/v2\/media\/778651"}],"wp:attachment":[{"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=778650"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=778650"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/spaceweekly.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=778650"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}