{"id":683,"date":"2023-09-11T13:28:32","date_gmt":"2023-09-11T13:28:32","guid":{"rendered":"https:\/\/awaca.ipsl.fr\/?page_id=683"},"modified":"2026-01-08T17:29:27","modified_gmt":"2026-01-08T17:29:27","slug":"publication","status":"publish","type":"page","link":"https:\/\/awaca.ipsl.fr\/en\/publication\/","title":{"rendered":"Publications"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"683\" class=\"elementor elementor-683\">\n\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-a88f3c1 elementor-section-height-min-height elementor-section-stretched elementor-section-boxed elementor-section-height-default elementor-section-items-middle\" data-id=\"a88f3c1\" data-element_type=\"section\" data-e-type=\"section\" data-settings=\"{&quot;stretch_section&quot;:&quot;section-stretched&quot;,&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t\t\t\t\t<div class=\"elementor-background-overlay\"><\/div>\n\t\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-03fd1a4\" data-id=\"03fd1a4\" data-element_type=\"column\" data-e-type=\"column\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-bd72d9c elementor-widget elementor-widget-heading\" data-id=\"bd72d9c\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">PUBLICATIONS<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-16d571d elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"16d571d\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-45b66ee\" data-id=\"45b66ee\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-c35b405 elementor-widget elementor-widget-spacer\" data-id=\"c35b405\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-6f5e73d elementor-section-full_width elementor-section-content-middle elementor-section-height-default elementor-section-height-default\" data-id=\"6f5e73d\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-b229d51\" data-id=\"b229d51\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-5497dac elementor-widget elementor-widget-heading\" data-id=\"5497dac\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Publications AWACA<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-4af74c4 elementor-widget__width-initial elementor-widget elementor-widget-qi_addons_for_elementor_timeline\" data-id=\"4af74c4\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"qi_addons_for_elementor_timeline.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<div class=\"qodef-shortcode qodef-m qodef-qi-timeline qodef-timeline--horizontal qodef-layout--columns qodef-timeline-layout--horizontal-standard qodef-point--standard qodef-qi--has-appear\" data-options=\"{&quot;colNum&quot;:&quot;3&quot;,&quot;colNum1440&quot;:&quot;3&quot;,&quot;colNum1366&quot;:&quot;3&quot;,&quot;colNum1024&quot;:&quot;3&quot;,&quot;colNum768&quot;:&quot;2&quot;,&quot;colNum680&quot;:&quot;1&quot;,&quot;colNum480&quot;:&quot;1&quot;}\">\n\t<div class=\"qodef-nav-prev\">\n\t\t<svg class=\"qodef-swiper-arrow-left\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\" x=\"0px\" y=\"0px\" viewBox=\"0 0 34.2 32.3\" xml:space=\"preserve\" style=\"stroke-width: 2;\"><line x1=\"0.5\" y1=\"16\" x2=\"33.5\" y2=\"16\"\/><line x1=\"0.3\" y1=\"16.5\" x2=\"16.2\" y2=\"0.7\"\/><line x1=\"0\" y1=\"15.4\" x2=\"16.2\" y2=\"31.6\"\/><\/svg>\t<\/div>\n\t<div class=\"qodef-nav-next\">\n\t\t<svg class=\"qodef-swiper-arrow-right\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\" x=\"0px\" y=\"0px\" viewBox=\"0 0 34.2 32.3\" xml:space=\"preserve\" style=\"stroke-width: 2;\"><line x1=\"0\" y1=\"16\" x2=\"33\" y2=\"16\"\/><line x1=\"17.3\" y1=\"0.7\" x2=\"33.2\" y2=\"16.5\"\/><line x1=\"17.3\" y1=\"31.6\" x2=\"33.5\" y2=\"15.4\"\/><\/svg>\t<\/div>\n\t<div class=\"qodef-grid-inner\">\n\t<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-6b06376 qodef-reverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img fetchpriority=\"high\" decoding=\"async\" width=\"1527\" height=\"589\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2026\/01\/article_chiabrando_vignon.png\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2026\/01\/article_chiabrando_vignon.png 1527w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2026\/01\/article_chiabrando_vignon-300x116.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2026\/01\/article_chiabrando_vignon-1024x395.png 1024w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2026\/01\/article_chiabrando_vignon-768x296.png 768w\" sizes=\"(max-width: 1527px) 100vw, 1527px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tJanvier 2026\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.5194\/gmd-19-239-2026\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Article] Intermediate-complexity parameterisation of blowing snow in the ICOLMDZ AGCM: development and first applications in Antarctica (Vignon et al., 2026)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tThe erosion of surface snow by the wind is an important process for the Antarctic surface mass balance. This study presents the first development of a parameterisation of blowing snow for a global climate model. Simulations avec evaluated using measurements in Antarctica. Results show an overall decrease of the snow accumulation in the escarpment region of the ice sheet due to snow erosion and an increase at the coast due to blowing snow deposition and increase in precipitation.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-00a5a87 qodef-obverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img decoding=\"async\" width=\"2067\" height=\"1794\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/12\/article_valentin_wiener.png\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/12\/article_valentin_wiener.png 2067w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/12\/article_valentin_wiener-300x260.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/12\/article_valentin_wiener-1024x889.png 1024w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/12\/article_valentin_wiener-768x667.png 768w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/12\/article_valentin_wiener-1536x1333.png 1536w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/12\/article_valentin_wiener-2048x1778.png 2048w\" sizes=\"(max-width: 2067px) 100vw, 2067px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tNovembre 2025\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.5194\/egusphere-2025-2046\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Article] An extensive investigation of the ability of the ICOLMDZ model to simulate a katabatic wind event in Antarctica (Wiener et al., 2025)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tKatabatic winds are a key feature of the climate of Antarctica, but substantial biases remain in their representation in atmospheric models. This study investigates a katabatic wind event in an atmospheric circulation model using in-situ observations. The framework allows to disentangle which part of the bias is due to horizontal resolution, to parameter calibration and to structural deficiencies in the model. We underline in particular the need to refine the physics of the model snow cover.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-661af5b qodef-reverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img decoding=\"async\" width=\"1078\" height=\"943\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_ines_ollivier.png\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_ines_ollivier.png 1078w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_ines_ollivier-300x262.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_ines_ollivier-1024x896.png 1024w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_ines_ollivier-768x672.png 768w\" sizes=\"(max-width: 1078px) 100vw, 1078px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tOctobre 2025\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.5194\/essd-2025-35\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Article] Time series of the summertime atmospheric water vapour isotopic composition at Concordia station, East Antarctica (Ollivier et al., 2025)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tWe present a novel 2.5-month record of the atmospheric water vapour isotopic composition during the austral summer 2023\u20132024 at Concordia Station on the Antarctic Plateau. We show that two independent laser spectrometers accurately record the diurnal variability of the atmospheric water vapour \ud835\udeff18O, \ud835\udeffD, and d-excess. We compare the measurements against outputs of the isotope-enabled general circulation model LMDZ6-iso to show how the data can be used to evaluate such models.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-6bdb97a qodef-obverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img loading=\"lazy\" decoding=\"async\" width=\"1230\" height=\"679\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/figure_stage_maxime_coste.png\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/figure_stage_maxime_coste.png 1230w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/figure_stage_maxime_coste-300x166.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/figure_stage_maxime_coste-1024x565.png 1024w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/figure_stage_maxime_coste-768x424.png 768w\" sizes=\"(max-width: 1230px) 100vw, 1230px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tAo\u00fbt 2025\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/web.lmd.jussieu.fr\/~cgenthon\/SiteCALVA\/reports\/rapportMCENSTA.pdf\" target=\"_blank\" rel=\"nofollow\" title=\"Click to open file\">\n\t\t\ud83d\udcc4 [Rapport de stage] Caract\u00e9risation des pr\u00e9cipitations Antarctiques : \u00e9tude de cas, m\u00e9thodes statistiques de croisement de donn\u00e9es de diff\u00e9rents instruments de t\u00e9l\u00e9d\u00e9tection depuis la surface\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tDans le cadre de son projet de recherche \u00e0 l\u2019ENSTA, Maxime Coste a \u00e9valu\u00e9 la repr\u00e9sentativit\u00e9 d\u2019un \u00ab golden \u00e9v\u00e8nement \u00bb AWACA s\u00e9lectionn\u00e9 en f\u00e9vrier 2025 \u00e0 partir de 15 ann\u00e9es de donn\u00e9es MRR (Micro Rain Radar) \u00e0 Dumont d&#039;Urville, et a explor\u00e9, via des m\u00e9thodes d\u2019intelligence artificielle appliqu\u00e9es aux mesures de ceilom\u00e8tre, comment compl\u00e9ter la zone aveugle du MRR en surface.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-75fc265 qodef-reverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img loading=\"lazy\" decoding=\"async\" width=\"999\" height=\"814\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz2.png\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz2.png 999w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz2-300x244.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz2-768x626.png 768w\" sizes=\"(max-width: 999px) 100vw, 999px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tJuillet 2025\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.5194\/egusphere-2025-2590\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Preprint in review] Water vapour isotope anomalies during an atmospheric river event at Dome C, East Antarctica (Dutrievoz et al., 2025)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tIn December 2018, an atmospheric river event from the Atlantic reached Dome C, East Antarctica, causing a +18\u202f\u00b0C warming, tripled water vapour, and a strong isotopic anomaly in water vapour (+ 17 \u2030 for \u03b418O) at the surface. During the peak of the event, we found 70\u202f% of the water vapour came from local snow sublimation, and 30\u202f% from the atmospheric river itself, highlighting both large-scale advection and local interactions at the surface.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-1897939 qodef-obverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img loading=\"lazy\" decoding=\"async\" width=\"1593\" height=\"582\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_thomas_lauwers.png\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_thomas_lauwers.png 1593w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_thomas_lauwers-300x110.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_thomas_lauwers-1024x374.png 1024w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_thomas_lauwers-768x281.png 768w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_thomas_lauwers-1536x561.png 1536w\" sizes=\"(max-width: 1593px) 100vw, 1593px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tMars 2025\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.5194\/amt-18-1135-2025\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Article] OF\u2013CEAS laser spectroscopy to measure water isotopes in dry environments: example of application in Antarctica (Lauwers et al., 2025)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tWater vapour isotopes are important tools to better understand processes governing the atmospheric hydrological cycle. In polar regions, their measurement helps to improve the interpretation of water isotopic records in ice cores. However, in situ water vapour isotopic monitoring is an important challenge, especially in dry places of East Antarctica. We present here an alternative laser spectroscopy technique adapted for such measurements, with a limit of detection down to 10 ppm humidity.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-7c5c57e qodef-reverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img loading=\"lazy\" decoding=\"async\" width=\"2128\" height=\"1705\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz.jpg\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz.jpg 2128w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz-300x240.jpg 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz-1024x820.jpg 1024w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz-768x615.jpg 768w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz-1536x1231.jpg 1536w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_niels_dutrievoz-2048x1641.jpg 2048w\" sizes=\"(max-width: 2128px) 100vw, 2128px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tF\u00e9vrier 2025\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.1029\/2024JD042073\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Article] Antarctic Water Stable Isotopes in the Global Atmospheric Model LMDZ6: From Climatology to Boundary Layer Processes (Dutrievoz et al., 2025)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tThe transport of water isotopes by the atmosphere plays a key role in interpreting Antarctic climate archives. This study evaluates the LMDZ6iso atmospheric model using snow, precipitation and vapour isotope measurements from both coastal and inland East Antarctica. The model is assessed at spatial, seasonal and diurnal scales, and the contribution of individual processes to boundary layer vapour isotopes is analysed. Results highlight the importance of isotopic exchanges during sublimation and condensation at low temperature, and suggest that including these processes would improve the representation of water isotopes in climate models.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-a291874 qodef-obverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img loading=\"lazy\" decoding=\"async\" width=\"2128\" height=\"2163\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_etienne_vignon2.jpg\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_etienne_vignon2.jpg 2128w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_etienne_vignon2-295x300.jpg 295w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_etienne_vignon2-1007x1024.jpg 1007w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_etienne_vignon2-768x781.jpg 768w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_etienne_vignon2-1511x1536.jpg 1511w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_etienne_vignon2-2015x2048.jpg 2015w\" sizes=\"(max-width: 2128px) 100vw, 2128px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tOctobre 2024\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.1029\/2024MS004400\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Article] Designing a Fully-Tunable and Versatile TKE-l Turbulence Parameterization for the Simulation of Stable Boundary Layers (Vignon et al., 2024)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tThis study introduces a new fully tunable TKE-l parameterization for turbulent diffusion in planetary atmospheres. The scheme is designed with a minimal set of adjustable parameters and a mixing length formulation that accounts for both stability and wind shear, making it applicable to Earth and Mars. Emphasis is placed on ensuring numerical stability at large time steps, a key challenge in simulating stable boundary layers. After calibration on idealized 1D cases, the parameterization successfully reproduces Antarctic and Martian nocturnal boundary layers in 3D simulations, demonstrating its robustness and versatility.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-10e6a56 qodef-reverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t<div class=\"qodef-e-icon-holder\">\n\t\t<i aria-hidden=\"true\" class=\"fas fa-cloud\"><\/i>\t<\/div>\n\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img loading=\"lazy\" decoding=\"async\" width=\"800\" height=\"584\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2024\/07\/fig-justine-LMDZ_CALIPSO_clouds_2_res.png\" class=\"attachment-full size-full\" alt=\"figure CALIPSO\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2024\/07\/fig-justine-LMDZ_CALIPSO_clouds_2_res.png 800w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2024\/07\/fig-justine-LMDZ_CALIPSO_clouds_2_res-300x219.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2024\/07\/fig-justine-LMDZ_CALIPSO_clouds_2_res-768x561.png 768w\" sizes=\"(max-width: 800px) 100vw, 800px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tJuillet 2024\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/web.lmd.jussieu.fr\/~jcharrel\/Stages\/Stage_M2\/rapport\/CHARREL_2024_stage_M2_rapport.pdf\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Rapport de stage] Nuages antarctiques : \u00e9valuation du mod\u00e8le LMDZ \u00e0 partir d&#039;observations satellitaires\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tDans le cadre de son stage de M2, Justine Charrel a \u00e9valu\u00e9 la couverture nuageuse au-dessus de l\u2019Antarctique dans la derni\u00e8re version du mod\u00e8le climatique LMDZ6A \u00e0 partir des observations du satellite CALIPSO.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n<div class=\"qodef-e qodef-e-item qodef-grid-item elementor-repeater-item-ea78856 qodef-obverse\">\n\t<div class=\"qodef-e-line-holder\">\n\t\t<span class=\"qodef-e-line\"><\/span>\n\t\t<div class=\"qodef-e-point-holder\">\n\t\t\t<div class=\"qodef-e-point\">\n\t\t\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t<\/div>\n\t<div class=\"qodef-e-item-inner\">\n\t\t<div class=\"qodef-e-top-holder\">\n\t\t\t<div class=\"qodef-e-image\">\n\t<img loading=\"lazy\" decoding=\"async\" width=\"2067\" height=\"971\" src=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_cecile_davrinche.png\" class=\"attachment-full size-full\" alt=\"\" srcset=\"https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_cecile_davrinche.png 2067w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_cecile_davrinche-300x141.png 300w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_cecile_davrinche-1024x481.png 1024w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_cecile_davrinche-768x361.png 768w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_cecile_davrinche-1536x722.png 1536w, https:\/\/awaca.ipsl.fr\/wp-content\/uploads\/2025\/08\/article_cecile_davrinche-2048x962.png 2048w\" sizes=\"(max-width: 2067px) 100vw, 2067px\" \/><\/div>\n\t\t<\/div>\n\t\t<div class=\"qodef-e-content-holder\">\n\t\t\t\t<div class=\"qodef-e-date\">\n\t\tMai 2024\t<\/div>\n\t\t\t\t\t<h4 class=\"qodef-e-title\">\n\t\t\t<a itemprop=\"url\" href=\"https:\/\/doi.org\/10.5194\/tc-18-2239-2024\" target=\"_blank\">\n\t\t\ud83d\udcc4 [Article] Understanding the drivers of near-surface winds in Ad\u00e9lie Land, East Antarctica (Davrinche et al., 2024)\t\t\t<\/a>\n\t\t<\/h4>\n\t\t\t\t\t<p class=\"qodef-e-text\">\n\t\tCoastal surface winds in Antarctica are amongst the strongest winds on Earth. They are either driven by the cooling of the surface air mass by the ice sheet (katabatic) or by large-scale pressure systems. Here we compute the relative contribution of these drivers. We find that seasonal variations in the wind speed come from the katabatic acceleration, but, at a 3-hourly timescale, none of the large-scale or katabatic accelerations can be considered as the main driver.\t<\/p>\n\t\t\t<\/div>\n\t<\/div>\n<\/div>\n\t<\/div>\n<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-442b5fd elementor-widget elementor-widget-spacer\" data-id=\"442b5fd\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"spacer.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"elementor-spacer\">\n\t\t\t<div class=\"elementor-spacer-inner\"><\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-a9065fb elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"a9065fb\" data-element_type=\"section\" data-e-type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-134adac\" data-id=\"134adac\" data-element_type=\"column\" data-e-type=\"column\">\n\t\t\t<div class=\"elementor-widget-wrap elementor-element-populated\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-703de19 elementor-widget elementor-widget-heading\" data-id=\"703de19\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Publications associ\u00e9es \u00e0 AWACA<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-df53e9f elementor-widget elementor-widget-text-editor\" data-id=\"df53e9f\" data-element_type=\"widget\" data-e-type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<ul><li><div>Landais, A., Agosta, C., Vimeux, F., Magand, O., Solis, C., Cauquoin, A., Dutrievoz, N., Risi, C., Leroy-Dos Santos, C., Fourr\u00e9, E., Cattani, O., Jossoud, O., Minster, B., Pri\u00e9, F., Casado, M., Dommergue, A., Bertrand, Y., and Werner, M.: Abrupt excursions in water vapor isotopic variability at the Pointe Benedicte observatory on Amsterdam Island, Atmos. Chem. Phys., 24, 4611\u20134634,\u00a0<span style=\"text-decoration: underline;\"><span id=\"OBJ_PREFIX_DWT388_com_zimbra_url\" class=\"Object\" role=\"link\"><span id=\"OBJ_PREFIX_DWT397_com_zimbra_url\" class=\"Object\" role=\"link\"><a class=\"moz-txt-link-freetext\" href=\"https:\/\/doi.org\/10.5194\/acp-24-4611-2024\" target=\"_blank\" rel=\"noopener\">https:\/\/doi.org\/10.5194\/acp-24-4611-2024<\/a><\/span><\/span><\/span>, 2024.<\/div><\/li><\/ul>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>PUBLICATIONS Publications AWACA Janvier 2026 \ud83d\udcc4 [Article] Intermediate-complexity parameterisation of blowing snow in the ICOLMDZ AGCM: development and first applications in Antarctica (Vignon et al., 2026) The erosion of surface snow by the wind is an important process for the Antarctic surface mass balance. This study presents the first development of a parameterisation of blowing [&hellip;]<\/p>\n","protected":false},"author":3,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-683","page","type-page","status-publish","hentry","entry"],"rttpg_featured_image_url":null,"rttpg_author":{"display_name":"Tess Kane","author_link":"https:\/\/awaca.ipsl.fr\/en\/author\/tkane\/"},"rttpg_comment":0,"rttpg_category":null,"rttpg_excerpt":"PUBLICATIONS Publications AWACA Janvier 2026 \ud83d\udcc4 [Article] Intermediate-complexity parameterisation of blowing snow in the ICOLMDZ AGCM: development and first applications in Antarctica (Vignon et al., 2026) The erosion of surface snow by the wind is an important process for the Antarctic surface mass balance. This study presents the first development of a parameterisation of blowing&hellip;","_links":{"self":[{"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/pages\/683","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/comments?post=683"}],"version-history":[{"count":122,"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/pages\/683\/revisions"}],"predecessor-version":[{"id":2298,"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/pages\/683\/revisions\/2298"}],"wp:attachment":[{"href":"https:\/\/awaca.ipsl.fr\/en\/wp-json\/wp\/v2\/media?parent=683"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}