{"id":1916,"date":"2022-04-05T10:13:45","date_gmt":"2022-04-05T09:13:45","guid":{"rendered":"https:\/\/pepsi.aip.de\/?p=1916"},"modified":"2022-04-05T10:15:19","modified_gmt":"2022-04-05T09:15:19","slug":"nodal-precession-and-tidal-evolution-of-two-hot-jupiterswasp-33-b-and-kelt-9-b","status":"publish","type":"post","link":"https:\/\/pepsi.aip.de\/?p=1916","title":{"rendered":"Nodal Precession and Tidal Evolution of Two Hot-Jupiters:WASP-33 b and KELT-9 b"},"content":{"rendered":"\n<p><span id=\"page19R_mcid1\" class=\"markedContent\"><span dir=\"ltr\" role=\"presentation\">Hot Jupiters orbiting rapidly rotating stars on inclined orbits undergo tidally i<\/span><span dir=\"ltr\" role=\"presentation\">nduced nodal precession <\/span><span dir=\"ltr\" role=\"presentation\">measurable over several years of observations. The Hot Jupiters WASP<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">33 b and KELT<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">9 b are <\/span><span dir=\"ltr\" role=\"presentation\">particularly interesting targets as they are among the hottest planets found to date, orbiting relatively <\/span><span dir=\"ltr\" role=\"presentation\">massive stars. Here, we analyze arc<\/span><span dir=\"ltr\" role=\"presentation\">hival and new data that span 11 and 5 years for WASP<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">33 b and <\/span><span dir=\"ltr\" role=\"presentation\">KELT<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">9 b, respectively, in order to to model and improve upon their tidal precession parameters. Our <\/span><span dir=\"ltr\" role=\"presentation\">work confirms the nodal precession for WASP<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">33 b and presents the first clear detection of th<\/span><span dir=\"ltr\" role=\"presentation\">e <\/span><span dir=\"ltr\" role=\"presentation\">precession of KELT<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">9 b. We determine that WASP<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">33 and KELT<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">9 have gravitational quadrupole <\/span><span dir=\"ltr\" role=\"presentation\">moments<\/span><span dir=\"ltr\" role=\"presentation\">. We estimate the planets&#8217; precession periods to be<\/span> <span dir=\"ltr\" role=\"presentation\">1460<\/span> <span dir=\"ltr\" role=\"presentation\">years and<\/span> <span dir=\"ltr\" role=\"presentation\">890<\/span> <span dir=\"ltr\" role=\"presentation\">years, respectively, <\/span><span dir=\"ltr\" role=\"presentation\">and that they will cease to transit their host stars around the years<\/span> <span dir=\"ltr\" role=\"presentation\">2090<\/span><span dir=\"ltr\" role=\"presentation\">CE and<\/span> <span dir=\"ltr\" role=\"presentation\">2074<\/span><span dir=\"ltr\" role=\"presentation\">CE, respectively. <\/span><span dir=\"ltr\" role=\"presentation\">Additionally, we investigate both planets&#8217; tidal and orbital evo<\/span><span dir=\"ltr\" role=\"presentation\">lution, suggesting that a high<\/span><span dir=\"ltr\" role=\"presentation\">&#8211;<\/span><span dir=\"ltr\" role=\"presentation\">eccentricity tidal migration scenario is possible to produce both system architectures and that they will <\/span><span dir=\"ltr\" role=\"presentation\">most likely not be engulfed by their hosts before the end of their main sequence lifetimes.<\/span><\/span><\/p>\n<figure id=\"attachment_1911\" aria-describedby=\"caption-attachment-1911\" style=\"width: 1498px\" class=\"wp-caption alignnone\"><a href=\"https:\/\/pepsi.aip.de\/wp-content\/uploads\/2022\/04\/WASP-33b.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-1911 size-full\" src=\"https:\/\/pepsi.aip.de\/wp-content\/uploads\/2022\/04\/WASP-33b.png\" alt=\"\" width=\"1498\" height=\"748\" srcset=\"https:\/\/pepsi.aip.de\/wp-content\/uploads\/2022\/04\/WASP-33b.png 1498w, https:\/\/pepsi.aip.de\/wp-content\/uploads\/2022\/04\/WASP-33b-300x150.png 300w, https:\/\/pepsi.aip.de\/wp-content\/uploads\/2022\/04\/WASP-33b-1024x511.png 1024w, https:\/\/pepsi.aip.de\/wp-content\/uploads\/2022\/04\/WASP-33b-768x383.png 768w\" sizes=\"auto, (max-width: 1498px) 100vw, 1498px\" \/><\/a><figcaption id=\"caption-attachment-1911\" class=\"wp-caption-text\">Modeling results for WASP-33 b data in 2016 (top panels from TULL; only one year shown), and 2019 (bottom panel; PEPSI). Left: Fourier-filtered residual map after subtracting the median line profile. The planet \u201cDoppler shadow&#8221; is the diagonal blue track running from the bottom-right to the top-left. Occasional gaps are due to interpolation onto a time array with a fixed interval. Middle: Modeled Doppler Tomography signal. The overall gradient along the time axis is due to the shift of stellar radial velocity. The enhanced red background during transit is due to the fact that we set the line profile normalization to unity for all line profiles. Right: difference of the two maps on the left and middle panel.<\/figcaption><\/figure>\n<p><span id=\"page19R_mcid5\" class=\"markedContent\"><span dir=\"ltr\" role=\"presentation\">Read more:<\/span> <a href=\"https:\/\/arxiv.org\/pdf\/2203.02546.pdf\"><span dir=\"ltr\" role=\"presentation\">Stephan et al. 2022, arXiv:2203.02546v1<\/span><\/a><\/span><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Hot Jupiters orbiting rapidly rotating stars on inclined orbits undergo tidally induced nodal precession measurable over several years of observations. The Hot Jupiters WASP&#8211;33 b and KELT&#8211;9 b are particularly interesting targets as they are among the hottest planets found to date, orbiting relatively massive stars. Here, we analyze archival and new data that span &hellip; <a href=\"https:\/\/pepsi.aip.de\/?p=1916\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">Nodal Precession and Tidal Evolution of Two Hot-Jupiters:WASP-33 b and KELT-9 b<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":5,"featured_media":0,"comment_status":"closed","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[11],"tags":[],"class_list":["post-1916","post","type-post","status-publish","format-standard","hentry","category-publications"],"_links":{"self":[{"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=\/wp\/v2\/posts\/1916","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=\/wp\/v2\/users\/5"}],"replies":[{"embeddable":true,"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=1916"}],"version-history":[{"count":2,"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=\/wp\/v2\/posts\/1916\/revisions"}],"predecessor-version":[{"id":1918,"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=\/wp\/v2\/posts\/1916\/revisions\/1918"}],"wp:attachment":[{"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1916"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=1916"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/pepsi.aip.de\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=1916"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}