{"id":833,"date":"2023-05-24T08:28:27","date_gmt":"2023-05-24T08:28:27","guid":{"rendered":"http:\/\/desarrollo-vm.ciai.inm.es\/testbed\/?page_id=833"},"modified":"2023-07-18T07:03:59","modified_gmt":"2023-07-18T07:03:59","slug":"project_21","status":"publish","type":"page","link":"https:\/\/testbed.aemet.es\/index.php\/project_21\/","title":{"rendered":"Correction of a lunar-irradiance model for aerosol optical depth retrieval and comparison with a star photometer"},"content":{"rendered":"<p style=\"text-align: justify;\">New technological advances permit lunar-irradiance to be measured with classical photometers. Lunar photometry has appeared as a suitable technique to retrieve aerosol information in nocturnal period, increasing the potential to derive AOD at night-time. However, the fast change in illumination throughout the Moon\u2019s cycle implies that an accurate and time-dependent knowledge of the extraterrestrial lunar irradiance is mandatory in lunar photometry.<\/p>\n<p style=\"text-align: justify;\">The RIMO model (an implementation of the ROLO \u2013 RObotic Lunar Observatory \u2013 model) has been considered a useful tool to estimate the AOD at night-time (Barreto et al., 2019).<\/p>\n<p style=\"text-align: justify;\">A new empirical correction factor to the RIMO model (RCF or RIMO Correction Factor) has been implemented in Roman et al. (2020) by means of Cimel CE318-T Sun\u2013sky\u2013Moon photometer for 98 pristine nights with low and stable AOD conditions at the Iza\u00f1a Observatory. The expected day-to-night coherence allowed the authors to estimate the inaccuracies inherent to the RIMO model and provides a RIMO corrected lunar irradiance model. The RCF correction applied to the RIMO model varies both with the Moon Phase Angle (MPA) and with wavelength, ranging from 1.01 to 1.14.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter size-large wp-image-868\" src=\"http:\/\/desarrollo-vm.ciai.inm.es\/testbed\/wp-content\/uploads\/2023\/05\/Figure23-1-1024x558.png\" alt=\"\" width=\"950\" height=\"518\" srcset=\"https:\/\/testbed.aemet.es\/wp-content\/uploads\/2023\/05\/Figure23-1-1024x558.png 1024w, https:\/\/testbed.aemet.es\/wp-content\/uploads\/2023\/05\/Figure23-1-300x163.png 300w, https:\/\/testbed.aemet.es\/wp-content\/uploads\/2023\/05\/Figure23-1-768x419.png 768w, https:\/\/testbed.aemet.es\/wp-content\/uploads\/2023\/05\/Figure23-1.png 1189w\" sizes=\"auto, (max-width: 950px) 100vw, 950px\" \/><\/p>\n<p style=\"text-align: justify;\"><strong> Figure 1.-&nbsp;<\/strong> AOD values from the Sun, Moon, and star photometer at Granada (Spain) from the first to third Moon quarters in July 2016. Panel (f) shows the \u00c5ngstr\u00f6m Exponent calculated with the wavelengths of 440, 500, 675 and 870\u2009nm (436, 500, 670, and 880\u2009nm for the star photometer). Moon phase angle is represented with a black line in each panel. Reprinted from Rom\u00e1n et al. (2020).<\/p>\n<p style=\"text-align: justify;\">These results revealed an expected overall underestimation of the RIMO model. The AOD derived by this corrected method is compared with the independent and co-located two-year AOD dataset made by a star photometer at Granada (Spain) (Figure 1). Average differences between \u22120.015 and \u22120.005 were found, and standard deviations are between 0.03 and 0.04 for 440, 500, 675, and 870 nm. Differences were higher for the 380 nm spectral band. No significant dependences on the Moon\u2013star AOD differences as a function of MPA were found (Roman et al., 2020).<\/p>\n<p><strong>Publicacions:<\/strong><\/p>\n<ul>\n<li style=\"text-align: justify;\"><span style=\"font-size: 11pt;\">Barreto, A., R. Rom\u00e1n, E. Cuevas, D. P\u00e9rez-Ram\u00edrez, A.J. Berj\u00f3n, N. Kouremeti, S. Kazadzis, J. Gr\u00f6bner, M. Mazzola, C. Toledano, J.A. Benavent-Oltra, L. Doppler, J. Jury\u0161ek, A.F. Almansa, S. Victori, F. Maupin, C. Guirado-Fuentes, R. Gonz\u00e1lez, V. Vitale, P. Goloub, L. Blarel, L. Alados-Arboledas, E. Woolliams, S. Taylor, J.C. Antu\u00f1a, M. Yela:&nbsp;<a href=\"https:\/\/doi.org\/10.1016\/j.atmosenv.2019.01.006\" target=\"_blank\" rel=\"noopener noreferrer\">Evaluation of night-time aerosols measurements and lunar irradiance models in the frame of the first multi-instrument nocturnal intercomparison campaign,<\/a> Atmospheric Environment, Volume 202, Pages 190-211, ISSN 1352-2310, https:\/\/doi.org\/10.1016\/j.atmosenv.2019.01.006,2019.<\/span><\/li>\n<\/ul>\n<ul>\n<li style=\"text-align: justify;\"><span style=\"font-size: 11pt;\">Rom\u00e1n, R., Gonz\u00e1lez, R., Toledano, C., Barreto, \u00c1., P\u00e9rez-Ram\u00edrez, D., Benavent-Oltra, J. A., Olmo, F. J., Cachorro, V. E., Alados-Arboledas, L., and de Frutos, \u00c1. M.:&nbsp;<a href=\"https:\/\/amt.copernicus.org\/articles\/13\/6293\/2020\/amt-13-6293-2020.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Correction of a lunar-irradiance model for aerosol optical depth retrieval and comparison with a star photometer,<\/a>, Atmos. Meas. Tech., 13, 6293\u20136310, https:\/\/doi.org\/10.5194\/amt-13-6293-2020, 2020.<\/span><\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>New technological advances permit lunar-irradiance to be measured with classical photometers. Lunar photometry has appeared as a suitable technique to<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"colormag_page_container_layout":"default_layout","colormag_page_sidebar_layout":"default_layout","footnotes":""},"class_list":["post-833","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/pages\/833","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/comments?post=833"}],"version-history":[{"count":12,"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/pages\/833\/revisions"}],"predecessor-version":[{"id":1701,"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/pages\/833\/revisions\/1701"}],"wp:attachment":[{"href":"https:\/\/testbed.aemet.es\/index.php\/wp-json\/wp\/v2\/media?parent=833"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}