{"id":259,"date":"2022-09-21T13:12:12","date_gmt":"2022-09-21T13:12:12","guid":{"rendered":"https:\/\/ybginat.com\/?page_id=259"},"modified":"2025-10-04T10:38:10","modified_gmt":"2025-10-04T10:38:10","slug":"demo","status":"publish","type":"page","link":"https:\/\/ybginat.com\/index.php\/demo\/","title":{"rendered":"Research"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"259\" class=\"elementor elementor-259\" data-elementor-post-type=\"page\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-9cfe0dd elementor-section-height-min-height elementor-section-content-middle elementor-section-boxed elementor-section-height-default elementor-section-items-middle\" data-id=\"9cfe0dd\" data-element_type=\"section\" data-e-type=\"section\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-37267c6\" data-id=\"37267c6\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-b085423 elementor-widget elementor-widget-heading\" data-id=\"b085423\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Research<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-8a149be elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"8a149be\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-84dcba9\" data-id=\"84dcba9\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-f0e07ff elementor-widget elementor-widget-text-editor\" data-id=\"f0e07ff\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>My research focuses on gravitational dynamics, both on small scales \u2013 studying few-body systems like the three-body problem \u2013 and on large scales, where I am interested in structure formation in the Universe. A motif that connects the various research topics described below is using gravitational astrophysics to learn about fundamental physics, for example the nature of dark matter or the nature of non-linearities in gravity.<\/p><p>Below are a few examples.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-01b326f elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"01b326f\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-dbf0688\" data-id=\"dbf0688\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-46f00da elementor-widget elementor-widget-text-editor\" data-id=\"46f00da\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><strong>Non-linear structure formation<\/strong><\/p><p>I am using kinetic theory to study large-scale structure formation for cold dark matter, via gravitational collapse. Gravitational collapse pertains to the evolution of a collection of massive particles, under their mutual gravitational pull, from an initially sparse distribution, to a more packed, dense one \u2013 they pull each other, so tend to cluster, hence \u2018collapse\u2019; it occurs continuously, on many scales, as haloes form. The fundamental quantity describing cold dark matter is the distribution function f(x,v), which specifies the probability of finding a particle at position x with velocity v. In Ginat <em>et al<\/em>. (<a href=\"https:\/\/journals.aps.org\/prd\/abstract\/10.1103\/ychs-2d5p\">2025<\/a>, where the video is from), we developed a theory (see video opposite for what 1D gravitational collapse looks like in phase-space) for the scaling of the power-spectrum on very small scales (accounting for the non-linear gravitational interactions). This work thus explained the universal power-law scaling at small scales, seen in cosmological simulations, for the matter power-spectrum, a key cosmological observable.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-4e50952\" data-id=\"4e50952\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-197f622 elementor-widget elementor-widget-video\" data-id=\"197f622\" data-element_type=\"widget\" data-e-type=\"widget\" data-settings=\"{&quot;video_type&quot;:&quot;hosted&quot;,&quot;controls&quot;:&quot;yes&quot;}\" data-widget_type=\"video.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"e-hosted-video elementor-wrapper elementor-open-inline\">\n\t\t\t\t\t<video class=\"elementor-video\" src=\"https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/video_high_res.mp4\" controls=\"\" preload=\"metadata\" controlsList=\"nodownload\"><\/video>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-9b4fdb4 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"9b4fdb4\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-a9e3834\" data-id=\"a9e3834\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-b53d7ec elementor-widget elementor-widget-text-editor\" data-id=\"b53d7ec\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p><span style=\"font-weight: bolder;\">Three-body problem<\/span><\/p><p>Three-body encounters are at the heart of the evolution of gravitational systems, in particular stellar clusters, where they manifest as the main interaction between stars and compact objects, and also facilitate the production of gravitational-wave sources. There is no analytic, closed-form solution to the three-body problem, because the motion is chaotic; indeed, the outcome of a close triple interaction is essentially random. Here is an example of an orbit:<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-679bc7d elementor-widget elementor-widget-image\" data-id=\"679bc7d\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<img fetchpriority=\"high\" decoding=\"async\" width=\"300\" height=\"225\" src=\"https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/trajectory-example-300x225.png\" class=\"attachment-medium size-medium wp-image-410\" alt=\"\" srcset=\"https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/trajectory-example-300x225.png 300w, https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/trajectory-example.png 678w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/>\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-2c7f70e elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"2c7f70e\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-1fd282b\" data-id=\"1fd282b\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-7e83fc9 elementor-widget elementor-widget-text-editor\" data-id=\"7e83fc9\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>In my work, I used this randomness to derive a closed-form statistical prediction for the\u00a0<em>probability<\/em>\u00a0of every possible outcome of a close triple encounter (see these 3 papers: Ginat &amp; Perets, <a href=\"https:\/\/journals.aps.org\/prx\/abstract\/10.1103\/PhysRevX.11.031020\">2021a<\/a>,<a href=\"https:\/\/academic.oup.com\/mnras\/article\/508\/1\/190\/6372917?login=false\">2021b<\/a>,<a href=\"https:\/\/academic.oup.com\/mnrasl\/article\/519\/1\/L15\/6835474?login=false\">2023<\/a>). In numerical simulations of the gravitational interaction of three stars, the interactions proceed as sequence of close triple approaches, interspersed with phases where one of the stars is ejected; if its energy is positive, it leaves, but otherwise it eventually returns to another close approach. I also modelled the intermediate steps \u2013 when the third body has a negative energy \u2013 while exactly accounting for all conservation laws. This model agreed well with simulations; see, e.g., this plot:<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-5097688 elementor-widget elementor-widget-image\" data-id=\"5097688\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t<figure class=\"wp-caption\">\n\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" width=\"300\" height=\"225\" src=\"https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/SP_exch_4-300x225.png\" class=\"attachment-medium size-medium wp-image-403\" alt=\"\" srcset=\"https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/SP_exch_4-300x225.png 300w, https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/SP_exch_4-768x576.png 768w, https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/SP_exch_4.png 875w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/>\t\t\t\t\t\t\t\t\t\t\t<figcaption class=\"widget-image-caption wp-caption-text\">From: Ginat &amp; Perets, Physical Review X, 11, 031020<\/figcaption>\n\t\t\t\t\t\t\t\t\t\t<\/figure>\n\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-f5a351f elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"f5a351f\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-17edcfb\" data-id=\"17edcfb\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-17e53d9 elementor-widget elementor-widget-text-editor\" data-id=\"17e53d9\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>This solution allowed us to envision the sequence of close approaches as a random walk. Understanding the intermediate steps is a necessary ingredient in understanding dynamically formed gravitational-wave signals, and we used the random-walk model to predict the probability of forming GW sources during a triple encounter.\u00a0<\/p><p>Random walks are also a good model for some hierarchical systems (where there is a binary orbited by a faraway third body). In <a href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2025arXiv250902685G\/abstract\">this<\/a> paper we studied &#8220;quasi-hierarchical&#8221; triples, where there is a very large hierarchy of time-scales between the inner and outer orbits, but the outer orbit is extremely eccentric, so that its time at pericentre is only a few times the inner period. This turns out to lead to a quasi-random walk of the angular momentum of the inner binary, usually causing its eccentricity to increase (on average).<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-3853769 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"3853769\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-542b5f3\" data-id=\"542b5f3\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-ebfc362 elementor-widget elementor-widget-text-editor\" data-id=\"ebfc362\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p dir=\"auto\"><b>Relativistic effects in large-scale structure<\/b><\/p><p dir=\"auto\">The observed distribution of galaxies on the sky provides a plethora of cosmological information, both on the evolution of the Universe and on large-scale structure. To interpret these observations however, we need to relate the observed galaxy sky positions and redshifts to the underlying space-time and matter distribution, a relation which is nontrivial even on very large scales, because of general relativity: the Universe is not exactly homogeneous and isotropic, and this deviation from an exact FLRW space-time distorts its own image. Light from galaxies is distorted (lensed, redshifted) by the large-scale structure &#8211; by the very distribution that we seek to observe.<\/p><p dir=\"auto\">The papers Ginat et al. (<a href=\"https:\/\/iopscience.iop.org\/article\/10.1088\/1475-7516\/2021\/12\/031\">2021<\/a>), and Villey, Ginat et al., (<a href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2025arXiv250611260V\/abstract\">2025<\/a>) seek to study these effects, with the help of the &#8220;cosmic ruler&#8221; formulation of large-scale structure observables. The second calculates the cosmic rulers explicitly at second order in cosmological perturbation theory &#8211; no mean feat!<\/p><p dir=\"auto\">While standard theories of inflation predict that the primordial density fluctuations were Gaussian (the distribution of their amplitudes was a normal distribution), other theories predict some deviation from that, called &#8220;primordial non-Gaussianity&#8221;. However, the relativistic effects can mimic that, so it&#8217;s important to get them right. In the future, out formulae can be used to calculate the observed galaxy distribution, with relativistic corrections, to compare with data, e.g. from <a href=\"https:\/\/spherex.caltech.edu\/\">SPHEREx<\/a>, and help it to find (or rule out) primordial non-Gaussianity.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t<div class=\"elementor-column elementor-col-50 elementor-top-column elementor-element elementor-element-aca66d8\" data-id=\"aca66d8\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-5381f82 elementor-widget elementor-widget-image\" data-id=\"5381f82\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"image.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t\t\t\t<figure class=\"wp-caption\">\n\t\t\t\t\t\t\t\t\t\t<img decoding=\"async\" width=\"800\" height=\"600\" src=\"https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/c_ell.png\" class=\"attachment-large size-large wp-image-397\" alt=\"\" srcset=\"https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/c_ell.png 875w, https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/c_ell-300x225.png 300w, https:\/\/ybginat.com\/wp-content\/uploads\/2025\/10\/c_ell-768x576.png 768w\" sizes=\"(max-width: 800px) 100vw, 800px\" \/>\t\t\t\t\t\t\t\t\t\t\t<figcaption class=\"widget-image-caption wp-caption-text\">From: Ginat et al. JCAP12(2021)031<\/figcaption>\n\t\t\t\t\t\t\t\t\t\t<\/figure>\n\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-d25a8a6 elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"d25a8a6\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-c160c20\" data-id=\"c160c20\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-b542852 elementor-widget elementor-widget-text-editor\" data-id=\"b542852\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>Updated: 4 October 2025.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Research My research focuses on gravitational dynamics, both on small scales \u2013 studying few-body systems like the three-body problem \u2013 and on large scales, where I am interested in structure formation in the Universe. A motif that connects the various research topics described below is using gravitational astrophysics to learn about fundamental physics, for example [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"elementor_header_footer","meta":{"footnotes":""},"class_list":["post-259","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/pages\/259","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/comments?post=259"}],"version-history":[{"count":14,"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/pages\/259\/revisions"}],"predecessor-version":[{"id":413,"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/pages\/259\/revisions\/413"}],"wp:attachment":[{"href":"https:\/\/ybginat.com\/index.php\/wp-json\/wp\/v2\/media?parent=259"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}