{"id":11736,"date":"2021-04-14T07:04:45","date_gmt":"2021-04-14T06:04:45","guid":{"rendered":"https:\/\/www.einstein-online.info\/?post_type=spotlight&#038;p=11736"},"modified":"2021-04-14T07:33:17","modified_gmt":"2021-04-14T06:33:17","slug":"multi-messenger-astrophysics","status":"publish","type":"spotlight","link":"https:\/\/www.einstein-online.info\/en\/spotlight\/multi-messenger-astrophysics\/","title":{"rendered":"Multi-messenger astrophysics and numerical relativity"},"content":{"rendered":"<p>The first detection of <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/gravitational-waves\/\">gravitational waves<\/a> from a binary neutron star merger on <a href=\"https:\/\/www.einstein-online.info\/en\/spotlight\/GW170817\/\">August 17th, 2017<\/a>, marked the beginning of a new era in astrophysics. Not only had the <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/ligo-2\/\">LIGO<\/a> observatories recorded gravitational wave signals from such an event, but researchers around the world also observed its <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/electromagnetic-radiation\/\">electromagnetic<\/a> counterparts. This breakthrough announced the beginning of multi-messenger astrophysics.<\/p>\n<p>The merger of <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/neutron-star\/\">neutron star<\/a> binaries (neutron star and neutron star or <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/black-hole\/\">black hole<\/a> and neutron star) is one of the most interesting and important observational targets in multi-messenger astrophysics. They represent cases of very strong <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/gravity\/\">gravity<\/a>, which still aren\u2019t fully understood, and that makes them interesting enough already. On top of that, the study of neutron-star <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/merger\/\">mergers<\/a> could help scientists to solve long-standing issues in basic research in physics.<\/p>\n<h2>What neutron star mergers reveal about long-standing physics questions<\/h2>\n<p>One of the open questions is the nature of the high-density nuclear matter. Neutron stars are an ultra high-density object composed primarily of neutrons, as the name suggests. However, their exact composition is unknown. Gravitational-wave and electromagnetic signals from neutron star binaries can provide information on the radius of neutron stars, which is determined by their composition.<\/p>\n<p>Another long-standing issue in physics is the origin of heavy elements like gold and uranium. We believe that these heavy elements are synthesized through the rapid neutron capture process (so-called r-process) from relatively light elements like iron. For this process to occur, an extremely neutron-rich (i.e. proton-poor) environment is necessary \u2013 which can only be found in a relativistic setting. However, exactly which astrophysical phenomenon is the major site of this r-process <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/nucleosynthesis\/\">nucleosynthesis<\/a> is still unknown. Neutron star mergers are the most promising candidates, because they provide a very neutron-rich environment. During a neutron star merger, a fraction of the neutron-rich matter is explosively ejected from the system into the interstellar space. In the ejecta, heavy elements are supposed to be synthesized via the r-process nucleosynthesis. The initially synthesized heavy elements are very neutron-rich, and thus strongly radioactive. This causes them to subsequently decay, which heats up the ejecta and makes them shine. If one can observe high-luminosity ejecta with an electromagnetic telescope together with gravitational waves, one can verify that the r-process nucleosynthesis occurs in the neutron-star merger.<\/p>\n<div id=\"attachment_11737\" style=\"width: 2890px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-11737\" class=\"wp-image-11737 size-full\" title=\"Periodic table showing origin of elements in the Solar System, based on data by Jennifer Johnson at Ohio State University. \u00a9 Cmglee, CC BY-SA 3.0, https:\/\/commons.wikimedia.org\/w\/index.php?curid=31761437 \" src=\"https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl.png\" alt=\"a color-coded periodic table, where colors indicate the elements' origins.\" width=\"2880\" height=\"1440\" srcset=\"https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl.png 2880w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl-300x150.png 300w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl-1024x512.png 1024w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl-768x384.png 768w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl-1536x768.png 1536w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl-2048x1024.png 2048w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/2880px-Nucleosynthesis_periodic_table_engl-830x415.png 830w\" sizes=\"auto, (max-width: 2880px) 100vw, 2880px\" \/><p id=\"caption-attachment-11737\" class=\"wp-caption-text\">Periodic table showing origin of elements in the Solar System, based on data by Jennifer Johnson at Ohio State University. \u00a9 Cmglee, CC BY-SA 3.0, https:\/\/commons.wikimedia.org\/w\/index.php?curid=31761437<\/p><\/div>\n<h2>Multi-messenger observations and numerical relativity<\/h2>\n<p>Multi-messenger observation of neutron star mergers could thus help answer a number of long-standing open questions in physics, provided that we have a reliable theoretical model that describes this type of events, with their strong gravity regime and mass ejection. Theorists have to solve <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/einsteins-equation\/\">Einstein&#8217;s equation<\/a> for general relativity together with the associated matter equations like hydrodynamics equations and radiation transfer equations, which govern the evolution of neutron star matter and neutrino emission. Since these equations are highly nonlinear, multidimensional, and complicated, they can only be solved with a large-scale numerical simulation.<\/p>\n<h2>Findings of numerical relativity on neutron star mergers<\/h2>\n<p>One important finding of <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/numerical-relativity\/\">numerical relativity<\/a> concerns the nature of the remnant after a merger: If the total mass of the binary system is smaller than about 2.8 solar masses, a neutron star is formed. If the total mass of the binary system is larger than this threshold, the self gravity of the merger remnant cannot be sustained by the pressure associated primarily with the repulsive force among nucleons and <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/centrifugal-force\/\">centrifugal force<\/a> by rapid rotation of the merger remnant. As a consequence, the remnant collapses to form a black hole.<\/p>\n<p>In addition, numerical relativity has clarified that during and after the merger, a fraction of the matter is ejected. It accumulates in a large disk around the system, irrespective of the type of remnant. The simulations allow to identify two mechanisms of this mass ejection. Dynamical mass ejection occurs in less than 10 milliseconds after the onset of the merger. The matter ejected in this process is called \u201cmerger ejecta\u201d. Post-merger mass ejection occurs from the disk surrounding the central object. The time scale of this mass ejection is a tenth of a second to ten seconds, and the ejected matter is called \u201cpost-merger ejecta\u201d.<\/p>\n<p>Current state-of-the-art numerical relativity enables scientists to accurately predict the merger and mass ejection processes for a given neutron-star binary (see, e.g, a visualization of a binary neutron star below). Furthermore, astrophysicists can calculate an electromagnetic signal from the ejecta via a radiation transfer simulation, where the energy transport by photons is taken into account. This theoretical work is used to predict signals of gravitational and electromagnetic waves, and serves in the interpretation of the observational results.<\/p>\n<div id=\"attachment_11740\" style=\"width: 512px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-11740\" class=\"wp-image-11740 size-full\" title=\"Neutron star merger - \u00a9 S. Fujibayashi, M. Shibata (Max-Planck-Institut f\u00fcr Gravitationsphysik) \" src=\"https:\/\/www.einstein-online.info\/wp-content\/uploads\/neutron-star-merger.png\" alt=\"Three images show a neutron star merger: First, to objects are close to each other, second, they merge into one shape and third, a big disk of ejected mass is shown.\" width=\"502\" height=\"692\" srcset=\"https:\/\/www.einstein-online.info\/wp-content\/uploads\/neutron-star-merger.png 502w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/neutron-star-merger-218x300.png 218w\" sizes=\"auto, (max-width: 502px) 100vw, 502px\" \/><p id=\"caption-attachment-11740\" class=\"wp-caption-text\">A result of numerical-relativity simulation for the late inspiral (top), merger (middle), and post-merger (bottom) of a binary neutron star. In this example, after the merger, a massive neutron star is formed and a fraction of matter is ejected. \u00a9 S. Fujibayashi, M. Shibata (Max-Planck-Institute for Gravitational Physics)<\/p><\/div>\n<p>&nbsp;<\/p>\n<h2>Numerical relativity meets real observations<\/h2>\n<p>For the neutron-star merger event on August 17, 2017, electromagnetic observations were extensively performed from the gamma-ray to the radio bands. Gravitational wave observation revealed that the total mass of the binary neutron star was 2.73\u20132.78 solar masses, which is smaller than the 2.8 threshold for black-hole formation. Thus, according to the simulations, the remnant should be a high-mass neutron star. Based on the numerical relativity study, a schematic picture of the merger remnant and ejecta at about one second after the onset of the merger for GW170817 event becomes evident: A massive neutron star at the center is surrounded by a disk. In the outer region, merger ejecta and post-merger ejecta escape from the system with sub-relativistic speed of 5 to 30 percent of the speed of light.<\/p>\n<div id=\"attachment_11882\" style=\"width: 809px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-11882\" class=\"wp-image-11882 \" title=\"Schematic of remnant of GW170817 \/ \u00a9 Masaru Shibata, Redesign: Daniela Leitner \u2013 Einstein Online\" src=\"https:\/\/www.einstein-online.info\/wp-content\/uploads\/Black_Holes_and_Co_Rotation_Axis_Observer_Graphic_Daniela_Leitner_Einstein-Online.jpg\" alt=\"Material gathers in a disk around the rotational axis. An observer sees light emissions from the shining matter.\" width=\"799\" height=\"475\" srcset=\"https:\/\/www.einstein-online.info\/wp-content\/uploads\/Black_Holes_and_Co_Rotation_Axis_Observer_Graphic_Daniela_Leitner_Einstein-Online.jpg 1000w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/Black_Holes_and_Co_Rotation_Axis_Observer_Graphic_Daniela_Leitner_Einstein-Online-300x179.jpg 300w, https:\/\/www.einstein-online.info\/wp-content\/uploads\/Black_Holes_and_Co_Rotation_Axis_Observer_Graphic_Daniela_Leitner_Einstein-Online-768x457.jpg 768w\" sizes=\"auto, (max-width: 799px) 100vw, 799px\" \/><p id=\"caption-attachment-11882\" class=\"wp-caption-text\">Schematic picture for the remnant of GW170817 at about 1 second after the onset of merger.<\/p><\/div>\n<p>Based on these findings, it is possible to construct an ejecta model of a realistic density profile, velocity profile, composition, and temperature. In the case of GW170817, the observed optical and infrared light curves matched the theoretical calculations reasonably well for a variety of wavelengths. The estimated total ejecta mass was about 0.03 solar masses and in addition, it is strongly suggested that in the merger ejecta, a substantial fraction of heavy elements are included.<\/p>\n<p>During <a href=\"https:\/\/www.einstein-online.info\/en\/spotlight\/o3\/\">the third observation run<\/a> of the gravitational wave detectors LIGO and <a href=\"https:\/\/www.einstein-online.info\/en\/explandict\/virgo\/\">Virgo<\/a>, gravitational waves from what is most likely to be another neutron star merger were detected. Despite extensive immediate search triggered by a public alert system, no electromagnetic counterpart of GW190425 was found. Thus, the multi-messenger observation of a binary neutron star in GW170817 continues to be the primary example for a fruitful cooperation between experimental gravitational-wave physicists, electromagnetic astronomers, and numerical relativity researchers.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>During neutron star mergers, both gravitational wave and electromagnetic signals are emitted. This could help solve long-standing issues in basic physics research with multi-messenger astrophysics.<\/p>\n","protected":false},"author":10,"featured_media":11894,"menu_order":0,"template":"","meta":{"footnotes":""},"categories":[520],"tags":[],"class_list":["post-11736","spotlight","type-spotlight","status-publish","has-post-thumbnail","hentry","category-black-holes","eo_author-masaru-shibata-en","eo_topic-blackholes","eo_topic-gr","eo_topic-blackholes-sub02","eo_topic-gr-sub06"],"_links":{"self":[{"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/spotlight\/11736","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/spotlight"}],"about":[{"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/types\/spotlight"}],"author":[{"embeddable":true,"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/users\/10"}],"version-history":[{"count":7,"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/spotlight\/11736\/revisions"}],"predecessor-version":[{"id":11891,"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/spotlight\/11736\/revisions\/11891"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/media\/11894"}],"wp:attachment":[{"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/media?parent=11736"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/categories?post=11736"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.einstein-online.info\/en\/wp-json\/wp\/v2\/tags?post=11736"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}