{"id":12320,"date":"2022-01-02T21:06:13","date_gmt":"2022-01-03T07:06:13","guid":{"rendered":"http:\/\/www.eaobservatory.org\/jcmt\/?page_id=12320"},"modified":"2022-01-04T04:56:12","modified_gmt":"2022-01-04T14:56:12","slug":"jcmt-venus-monitoring-phosphine-and-other-molecules-in-venuss-atmosphere","status":"publish","type":"page","link":"https:\/\/www.eaobservatory.org\/jcmt\/science\/large-programs\/jcmt-venus-monitoring-phosphine-and-other-molecules-in-venuss-atmosphere\/","title":{"rendered":"JCMT-Venus &#8211; monitoring phosphine and other molecules in Venus\u2019s atmosphere"},"content":{"rendered":"<p>JCMT-Venus is a long term programme to study the molecular content of the atmosphere of Venus. This has been prompted by the unexpected discovery of phosphine, PH<sub>3<\/sub>, in the planet\u2019s cloud decks by observations at 267 GHz from the JCMT with RxA, from ALMA, and from JCMT with the new \u2019U\u2019u \u0304 receiver (see Fig. 1). While there remains some controversy about these detections and suggestions that the line might be a misidentified SO<sub>2<\/sub> feature, there are strong arguments that the line is both real and PH<sub>3<\/sub>, not a misidentification. Independent, <em>in situ<\/em> confirmation of the presence of PH<sub>3<\/sub> from the Pioneer Venus Probe Mass Spectrometer LMNS supports this conclusion.<\/p>\n<div>\n<div id=\"attachment_12364\" style=\"width: 840px\" class=\"wp-caption aligncenter\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig1_combined.jpg\"><img aria-describedby=\"caption-attachment-12364\" loading=\"lazy\" class=\"wp-image-12364 size-large\" src=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig1_combined-1024x437.jpg\" alt=\"\" width=\"830\" height=\"354\" srcset=\"https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig1_combined-1024x437.jpg 1024w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig1_combined-300x128.jpg 300w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig1_combined-768x328.jpg 768w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig1_combined-150x64.jpg 150w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig1_combined.jpg 1052w\" sizes=\"(max-width: 830px) 100vw, 830px\" \/><\/a><p id=\"caption-attachment-12364\" class=\"wp-caption-text\">Figure 1: The Phosphine 1.123mm 1-0 line as detected by ALMA (left) and JCMT with RxA (middle) and (right) in a preliminary reduction of 30 minutes of \u2019U\u2019u \u0304 observations. The black lines in the JCMT and ALMA spectra indicate the level of SO<sub>2<\/sub> absorption derived from simultaneous (ALMA) and near-simultaneous observations of a different SO<sub>2<\/sub> line. The black line in the rightmost spectrum indicates a 15 ppm model for phosphine absorption (Greaves et al., 2021 &amp; refs therein).<\/p><\/div>\n<\/div>\n<div><\/div>\n<div><span lang=\"EN-GB\">The presence of phosphine in the atmosphere of Venus is something of a mystery, since, according to all normal chemical-production processes, this molecule should not be there at all. Even exotic processes invoking volcanism, lightning, or injection from impactors are incapable of producing the <\/span><\/div>\n<div><span lang=\"EN-GB\">\u223c<\/span>15 ppb quantities of PH<sub>3<\/sub> seen in observations. We are left with the possibility that the PH<sub>3<\/sub> is generated by as-yet unknown chemical processes, which seems unlikely, or the even more speculative proposition that the source of phosphine is biological \u2013 i.e. PH<sub>3<\/sub> is a marker for the presence of life in the upper atmosphere of Venus, our nearest neighbour planet, even though the conditions in these clouds are hostile to all known forms of life (see Fig. 2).<\/div>\n<div><\/div>\n<div>\n<div id=\"attachment_12365\" style=\"width: 985px\" class=\"wp-caption aligncenter\"><a href=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig2.jpg\"><img aria-describedby=\"caption-attachment-12365\" loading=\"lazy\" class=\"size-full wp-image-12365\" src=\"http:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig2.jpg\" alt=\"\" width=\"975\" height=\"491\" srcset=\"https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig2.jpg 975w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig2-300x151.jpg 300w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig2-768x387.jpg 768w, https:\/\/www.eaobservatory.org\/jcmt\/wp-content\/uploads\/sites\/2\/2021\/12\/venus_fig2-150x76.jpg 150w\" sizes=\"(max-width: 975px) 100vw, 975px\" \/><\/a><p id=\"caption-attachment-12365\" class=\"wp-caption-text\">Figure 2: A schematic diagram of the vertical structure of the atmosphere of Venus (Seager et al., 2021).<\/p><\/div>\n<\/div>\n<div>\n<p>Much remains to be determined about the phosphine in Venus\u2019 atmosphere. The altitude at which the molecules reside is highly uncertain, with a strongly decreasing gradient above the cloud tops likely given non-detections in the near- &amp; mid-IR, and we know little about any temporal or spatial variation.<\/p>\n<div><span lang=\"EN-GB\">The JCMT-Venus project will use \u2019U\u2019u \u0304 to monitor PH<sub>3<\/sub> and several other species, including HDO, SO, HCO<sup>+\u00a0<\/sup>and SO<sub>2 <\/sub>over a range of timescales, from hours to years. We already know the abundance of several of these species varies with time, but we do not know the degree to which phosphine varies, or if any variation is correlated with other species or with other factors such as illumination phase. Correlations, or anticorrelations, between phosphine and other species will provide clues to the processes that produce phosphine. These observations will additionally provide legacy information on the variability of other molecular species and higher S\/N observations of phosphine line wings, thanks to multiple observations and the improved stability of \u2019U\u2019u \u0304 over RxA. This will allow us to better determine the height in the atmosphere at which PH<sub>3<\/sub> absorption takes place, resolving one of the current major uncertainties in our understanding of PH<sub>3<\/sub>.<\/span><\/div>\n<\/div>\n<div><\/div>\n<div>\n<div><span lang=\"EN-GB\">References: Greaves et al., 2021, ApJ, submitted, arXiv:2108.08393; Seager et al., 2021, arXiv:2009.06474;<\/span><\/div>\n<div><\/div>\n<\/div>\n<p style=\"text-align: right\"><strong>Coordinators:\u00a0<\/strong>David Clements (UK),\u00a0<span lang=\"EN-GB\">Jane Greaves (UK), Masataka Imai (Japan), Kitiyanee Asanok (Thailand), Gerald Schieven (Canada), and Steve Mairs (EAO)<\/span><\/p>\n<p style=\"text-align: right\"><strong>\u2013 JCMT program code: M22AL006<\/strong><\/p>\n","protected":false},"excerpt":{"rendered":"<p>JCMT-Venus is a long term programme to study the molecular content of the atmosphere of Venus. This has been prompted by the unexpected discovery of phosphine, PH3, in the planet\u2019s cloud decks by observations at 267 GHz from the JCMT with RxA, from ALMA, and from JCMT with the new\u2026 <a class=\"continue-reading-link\" href=\"https:\/\/www.eaobservatory.org\/jcmt\/science\/large-programs\/jcmt-venus-monitoring-phosphine-and-other-molecules-in-venuss-atmosphere\/\">Continue reading<\/a><\/p>\n","protected":false},"author":5,"featured_media":0,"parent":3659,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/12320"}],"collection":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/users\/5"}],"replies":[{"embeddable":true,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/comments?post=12320"}],"version-history":[{"count":5,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/12320\/revisions"}],"predecessor-version":[{"id":12386,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/12320\/revisions\/12386"}],"up":[{"embeddable":true,"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/pages\/3659"}],"wp:attachment":[{"href":"https:\/\/www.eaobservatory.org\/jcmt\/wp-json\/wp\/v2\/media?parent=12320"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}