{"id":81437,"date":"2024-11-21T12:58:46","date_gmt":"2024-11-21T11:58:46","guid":{"rendered":"https:\/\/wfa.uwr.edu.pl\/?p=81437"},"modified":"2024-11-21T12:58:52","modified_gmt":"2024-11-21T11:58:52","slug":"studies-on-dark-matter","status":"publish","type":"post","link":"https:\/\/wfa.uwr.edu.pl\/en\/2024\/11\/21\/studies-on-dark-matter\/","title":{"rendered":"Studies on dark matter"},"content":{"rendered":"\n<div class=\"wp-block-columns is-layout-flex wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-large bs-news-primary-photo\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"653\" src=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-1024x653.jpg\" alt=\"Badanie ciemnej materii\" class=\"wp-image-53037\" srcset=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-1024x653.jpg 1024w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-300x191.jpg 300w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-768x490.jpg 768w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-24x15.jpg 24w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-36x23.jpg 36w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-48x31.jpg 48w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka.jpg 1088w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n<div class=\"wp-block-bonasoft-modular-recommended-posts2\">\r\n  <div class=\"bs_post-info\">\r\n    <div class=\"bs__post-info__section\">\r\n      <div class=\"bs__post-info__field\">\r\n        <p class=\"bs__post-info__field-desc\">Autor: <span class=\"bs__post-info__field-value\">Joanna Molenda-\u017bakowicz<\/span><\/p>\r\n      <\/div>\r\n    <\/div>\r\n    <div class=\"bs__post-info__section\">\r\n      <div class=\"bs__post-info__field\">\r\n        <p class=\"bs__post-info__field-desc\">Data Publikacji: <span class=\"bs__post-info__field-value\">21 November 2024<\/span><\/p>\r\n      <\/div>\r\n    <\/div>\r\n      <\/div>\r\n<\/div>\r\n\r\n<\/div>\n\n\n\n<div class=\"wp-block-column bs-column-short-news is-layout-flow wp-block-column-is-layout-flow\">\n<div class=\"wp-block-bonasoft-modular-breadcrumbs-block\"><div class=\"bs_add_breadcrumb_trail\"><\/div><\/div>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-black-color has-css-opacity has-black-background-color has-background is-style-wide bs-border-news\"\/>\n\n\n<h1 style=\"font-style:normal;font-weight:700;\" class=\"bs-naglowek-podstrony wp-block-post-title\">Studies on dark matter<\/h1>\n\n\n<p>In the article titled <em>Polarized target as a tool for probing the non-standard properties of dark matter <\/em>published in the journal <a href=\"https:\/\/www.sciencedirect.com\/science\/article\/abs\/pii\/S2212686423000766\" target=\"_blank\" rel=\"noreferrer noopener\">Physics of the Dark Universe Volume 41, August 2023, 101242<\/a>, Arkadiusz B\u0142aut and Wies\u0142aw Sobk\u00f3w study the properties of dark matter.<\/p>\n\n\n\n<p><\/p>\n<\/div>\n<\/div>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p>In the work we examine the possibility of applying a polarised nuclear shield in testing non-standard properties of fermionic dark matter. We assume that vector, axial, scalar, and tensor interactions take part in the process of dark matter scattering. We analyse energy and angle distributions of recoil nuclei for four experimental configurations determined by assumptions for measuring dark matter polarization and nuclear spin. In the first case, we assume that dark matter is unpolarized, and the spin of the scattered nucleus is not measured. The second option assumes measurement of its spin. The third variant permits hypothetical polarisation of dark matter; in this case the measurement is insensitive to nucleus polarisation. In the fourth experiment we assume the presence of polarised dark matter and possibility of measurement of nucleus spin. Each of the listed measurement scenarios offers new ways of testing dark matter properties and its interactions with visible matter molecules. In particular, measurements of angular distributions can be used to detect symmetry violations against time reversals.<\/p>\n<\/blockquote>\n\n\n\n<figure class=\"wp-block-image aligncenter size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"519\" src=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-1024x519.jpg\" alt=\"Rysunek 1\" class=\"wp-image-53043\" srcset=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-1024x519.jpg 1024w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-300x152.jpg 300w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-768x390.jpg 768w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-1536x779.jpg 1536w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-2048x1039.jpg 2048w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-1320x670.jpg 1320w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-24x12.jpg 24w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-36x18.jpg 36w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys1-48x24.jpg 48w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<p>Figure 1: Kinematics of polarized DM-nucleus scattering. \u00a0v\u02c6<sub>e<\/sub>\u00a0is the Earth\u2019s velocity in the galactic rest frame;\u00a0s\u02c6<sub>1<\/sub>\u00a0is the polarization vector of the nuclear target;\u00a0\u00a0v<sup>\u2192<\/sup><sub>\u03c7<\/sub>\u00a0,s\u02c6<sub>2<\/sub> &#8211; velocity and polarization vector of the DM incoming from the direction defined by the angles \u03b8,\u00a0\u03d5; \u00a0v<sup>\u2192<\/sup>, s\u02c6<sub>3<\/sub>\u00a0&#8211; velocity and polarization of the recoil nucleus outgoing in the direction defined by the angles \u03b1,\u00a0\u03b2.\u00a0<\/p>\n\n\n\n<p>\u00a0<\/p>\n\n\n\n<p>;<\/p>\n<\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-stackable-divider stk-block-divider stk-block stk-968ec58\" data-block-id=\"968ec58\"><hr class=\"stk-block-divider__hr\"\/><\/div>\n\n\n\n<figure class=\"wp-block-image aligncenter size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"792\" src=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-1024x792.jpg\" alt=\"RYsunki 2 i 3\" class=\"wp-image-53049\" srcset=\"https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-1024x792.jpg 1024w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-300x232.jpg 300w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-768x594.jpg 768w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-1536x1188.jpg 1536w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-2048x1584.jpg 2048w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-1320x1021.jpg 1320w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-24x19.jpg 24w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-36x28.jpg 36w, https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-rys2-3-48x37.jpg 48w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<p>Figure 2: Differential angular distribution of the number of events, <strong>\u0394<\/strong>R = R(s<sup>^<\/sup><sub>1<\/sub>) &#8211; R(-s<sup>^<\/sup><sub>2<\/sub>), recoil nuclei with energy E<sub>R<\/sub> = 20 keV. The graphs present the effects of scattering in the presence of axial-vector interactions with an additional involvement of scalar (left) and tensor (right) interactions for combined coupling phase of \ud835\udf45\/4.<\/p>\n\n\n\n<p>Figure 3: Distributions as in the previous figure for combined coupling phase of \ud835\udf45\/2. This case corresponds to the effect of maximum symmetry breaking time reversal.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>In the article titled Polarized target as a tool for probing the non-standard properties of dark matter published in the journal Physics of the Dark Universe Volume 41, August 2023, 101242, Arkadiusz B\u0142aut and Wies\u0142aw Sobk\u00f3w study the properties of dark matter. In the work we examine the possibility of applying a polarised nuclear shield [&hellip;]<\/p>\n","protected":false},"author":7182,"featured_media":53037,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"inline_featured_image":false,"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","ast-disable-related-posts":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"set","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"footnotes":""},"categories":[389],"tags":[392],"class_list":["post-81437","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-publikacje-en","tag-publikacje-en"],"featured_image_urls_v2":{"full":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka.jpg",1088,694,false],"thumbnail":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-150x150.jpg",150,150,true],"medium":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-300x191.jpg",300,191,true],"medium_large":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-768x490.jpg",768,490,true],"large":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-1024x653.jpg",1024,653,true],"1536x1536":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka.jpg",1088,694,false],"2048x2048":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka.jpg",1088,694,false],"menu-24x24":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-24x15.jpg",24,15,true],"menu-36x36":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-36x23.jpg",36,23,true],"menu-48x48":["https:\/\/wfa.uwr.edu.pl\/wp-content\/uploads\/sites\/216\/2023\/06\/publikacja-Blaut-notatka-48x31.jpg",48,31,true]},"post_excerpt_stackable_v2":"<p>Autor: Joanna Molenda-\u017bakowicz Data Publikacji: 21 November 2024 Studies on dark matter In the article titled Polarized target as a tool for probing the non-standard properties of dark matter published in the journal Physics of the Dark Universe Volume 41, August 2023, 101242, Arkadiusz B\u0142aut and Wies\u0142aw Sobk\u00f3w study the properties of dark matter. In the work we examine the possibility of applying a polarised nuclear shield in testing non-standard properties of fermionic dark matter. We assume that vector, axial, scalar, and tensor interactions take part in the process of dark matter scattering. We analyse energy and angle distributions of&hellip;<\/p>\n","category_list_v2":"<a href=\"https:\/\/wfa.uwr.edu.pl\/en\/category\/publikacje-en\/\" rel=\"category tag\">Publications<\/a>","author_info_v2":{"name":"kswistak","url":"https:\/\/wfa.uwr.edu.pl\/en\/author\/kswistak\/"},"comments_num_v2":"0 comments","acf":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.1.1 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Studies on dark matter - Faculty of Physics and Astronomy<\/title>\n<meta name=\"description\" content=\"Wydzia\u0142 Fizyki i Astronomii\" \/>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/wfa.uwr.edu.pl\/en\/2024\/11\/21\/studies-on-dark-matter\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Studies on dark matter - 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