{"id":475,"date":"2024-10-11T12:43:00","date_gmt":"2024-10-11T12:43:00","guid":{"rendered":"https:\/\/oca.camk.edu.pl\/?p=475"},"modified":"2025-12-17T05:32:57","modified_gmt":"2025-12-17T05:32:57","slug":"surface-brightness-color-technique-applied-to-nearby-rr-lyrae-stars","status":"publish","type":"post","link":"https:\/\/oca.camk.edu.pl\/index.php\/2024\/10\/11\/surface-brightness-color-technique-applied-to-nearby-rr-lyrae-stars\/","title":{"rendered":"Surface brightness-color technique applied to nearby RR Lyrae stars"},"content":{"rendered":"\n<p>Near-infrared data from OCM combined with high-resolution spectroscopic data and Gaia parallaxes lead to the determination of projection factors and mean radii for nine Galactic RR Lyrae stars.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-text-color has-alpha-channel-opacity has-background is-style-dots\" style=\"background-color:#1b155c;color:#1b155c\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">Infrared surface brightness technique applied to RR Lyrae stars from the solar neighborhood<\/h3>\n\n\n\n<p><em>B. Zgirski, W. Gieren, G. Pietrzy\u0144ski, M. G\u00f3rski, P. Wielg\u00f3rski, J. Storm, G. Bras, P. Kervella, N. Nardetto, G. Hajdu, R. Chini, M. Haas<\/em><\/p>\n\n\n\n<p><a href=\"https:\/\/ui.adsabs.harvard.edu\/abs\/2024A%26A...690A.295Z\/abstract\">2024, A&amp;A, 690A, 295<\/a><\/p>\n\n\n\n<p>The Baade\u2013Wesselink (BW) method is also known as the pulsation parallax method because it allows us to estimate distances to individual pulsating stars. For this method to be accurate, one needs to know the projection factor (p-factor), i.e. the conversion between the real, pulsational velocity of the stars and their projected, radial velocity, as observed spectroscopically.<\/p>\n\n\n\n<p>In order to determine the p-factor, we first gathered multi-band photometric data (including near-infrared <em>K<\/em>-band data from the IRIS telescope at OCM), spectroscopic data, and parallaxes from Gaia DR3 for nine Galactic RR Lyrae stars. Using Gaia parallaxes we determined absolute magnitudes for these stars, and next we used the infrared surface-brightness (IRSB) version of the surface brightness\u2013color relation, which depends on the (<em>V\u2212K<\/em>) color, to estimate stellar angular diameters. Radial velocity measurements obtained from spectroscopy traced variations of the stellar radius.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"393\" src=\"https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig12-1-1024x393.webp\" alt=\"\" class=\"wp-image-486\" style=\"width:646px;height:auto\" srcset=\"https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig12-1-1024x393.webp 1024w, https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig12-1-300x115.webp 300w, https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig12-1-768x295.webp 768w, https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig12-1.webp 1454w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n<\/div>\n\n\n<p>The ratio of each star&#8217;s angular radius to its physical radius can be fitted with a line, where the slope represents the p-factor, and the intercept &#8211; the mean stellar radius.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"755\" height=\"439\" src=\"https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig3.png\" alt=\"\" class=\"wp-image-487\" style=\"width:561px;height:auto\" srcset=\"https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig3.png 755w, https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig3-300x174.png 300w\" sizes=\"auto, (max-width: 755px) 100vw, 755px\" \/><\/figure>\n<\/div>\n\n\n<p>The p-factors determined from the IRSB method range between 1.39 and 1.45, and are systematically larger by 0.14\u20130.20 than p-factors determined by Bras et al. (2024) using the SPIPS method.<\/p>\n\n\n\n<p>Using our sample we also derive a relation between the p-factor and the pulsation period, and between the radius and the pulsation period.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"629\" src=\"https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig89-1024x629.webp\" alt=\"\" class=\"wp-image-488\" style=\"width:739px;height:auto\" srcset=\"https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig89-1024x629.webp 1024w, https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig89-300x184.webp 300w, https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig89-768x472.webp 768w, https:\/\/oca.camk.edu.pl\/wp-content\/uploads\/2024\/10\/Zgirski2024_fig89.webp 1026w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n<\/div>\n\n\n<p>Listen to AI-generated podcast on this topic (credit: <a href=\"https:\/\/notebooklm.google\">https:\/\/notebooklm.google<\/a>)<\/p>\n\n\n\n<figure class=\"wp-block-embed is-type-video is-provider-youtube wp-block-embed-youtube wp-embed-aspect-16-9 wp-has-aspect-ratio\"><div class=\"wp-block-embed__wrapper\">\n<iframe loading=\"lazy\" title=\"Paper &quot;Infrared surface brightness technique applied to RR Lyrae stars...&quot; by Zgirski et al. (2024)\" width=\"680\" height=\"383\" src=\"https:\/\/www.youtube.com\/embed\/OSkbFdye2yI?feature=oembed\" frameborder=\"0\" allow=\"accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture; web-share\" referrerpolicy=\"strict-origin-when-cross-origin\" allowfullscreen><\/iframe>\n<\/div><\/figure>\n\n\n\n<p>The data were collected using the IRIS telescope in years 2017-2019, i.e. before the reconstruction of OCM.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Near-infrared data from OCM combined with high-resolution spectroscopic data and Gaia parallaxes lead to the determination of projection factors and mean radii for nine Galactic RR Lyrae stars.<\/p>\n","protected":false},"author":1,"featured_media":490,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[11],"tags":[24,21,22,34,25],"class_list":["post-475","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-science","tag-baade-wesselink","tag-iris","tag-p-factor","tag-pre-ocm","tag-rr-lyrae"],"_links":{"self":[{"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts\/475","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/comments?post=475"}],"version-history":[{"count":7,"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts\/475\/revisions"}],"predecessor-version":[{"id":715,"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/posts\/475\/revisions\/715"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/media\/490"}],"wp:attachment":[{"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/media?parent=475"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/categories?post=475"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/oca.camk.edu.pl\/index.php\/wp-json\/wp\/v2\/tags?post=475"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}