{"id":313,"date":"2022-08-18T14:27:29","date_gmt":"2022-08-18T12:27:29","guid":{"rendered":"https:\/\/caemi2i.in2p3.fr\/?page_id=313"},"modified":"2025-04-02T10:59:02","modified_gmt":"2025-04-02T08:59:02","slug":"tableau-des-publications","status":"publish","type":"page","link":"https:\/\/caemi2i.in2p3.fr\/index.php\/tableau-des-publications\/","title":{"rendered":"Tableau des publications"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<figure class=\"wp-block-table is-style-regular\"><table><tbody><tr><td>date<\/td><td>Conf \/ journal<\/td><td>localisation<\/td><td>Auteur<\/td><td>titre<\/td><\/tr><tr><td>2015<\/td><td>NSS-MIC<\/td><td>San Diego, USA<\/td><td>E. Bechetoille<\/td><td><a href=\"http:\/\/micrhau.in2p3.fr\/spip\/spip.php?article122\">Double Slope Dynamic Range and Low Noise CSA<\/a>,&nbsp;<a href=\"http:\/\/micrhau.in2p3.fr\/spip\/IMG\/pptx\/larzic_2014_nss-mic15.pptx\">slides<\/a><\/td><\/tr><tr><td>2016<\/td><td>Journal of Astronomical Telescopes, Instruments, and Systems<\/td><td><\/td><td>D. Pr\u00eale et al.<\/td><td>Gain drift compensation with no feedback-loop developed for the X-Ray Integral Field Unit\/ATHENA readout chain<\/td><\/tr><tr><td>2018<\/td><td>Journal of Low Temperature Physics<\/td><td><\/td><td>D. Pr\u00eale et al.<\/td><td>SiGe Integrated Circuit Developments for SQUID\/TES Readout<\/td><\/tr><tr><td>2019<\/td><td>Sensors &amp; Transducers<\/td><td><\/td><td>S. Chen et al.<\/td><td><a href=\"https:\/\/www.researchgate.net\/publication\/337403226_Dynamic_Base_Current_Compensation_for_Cascaded_Bipolar_Low_Noise_Amplifier\">Dynamic Base Current Compensation for Cascaded Bipolar Low Noise Amplifier<\/a><\/td><\/tr><tr><td>2020<\/td><td>Space Telescopes and Instrumentation<\/td><td><\/td><td>S. Chen et al.<\/td><td><a href=\"https:\/\/www.researchgate.net\/publication\/347601924_ATHENA_warm_ASIC_for_the_X-IFU_electronics\">ATHENA warm ASIC for the X-IFU electronics<\/a><\/td><\/tr><tr><td>2020<\/td><td>Space Telescopes and Instrumentation<\/td><td><\/td><td>D. Pr\u00eale et al.<\/td><td><a href=\"https:\/\/www.researchgate.net\/publication\/347605833_Warm_front_end_electronic_modelization_for_the_X-IFU_ATHENA_readout_chain_simulation\">Warm front end electronic modelization for the X-IFU ATHENA readout chain simulation<\/a><\/td><\/tr><tr><td>2022<\/td><td>AMICSA<\/td><td>Spain<\/td><td>Cyrille Derrien, Sebastien Extier, Julien Fleury, Salleh Ahmad, Si Chen, Manuel Gonzalez, Bernard Courty, Sylvie Blin, Damien Pr\u00eale, Jean Mesquida, Florence Ardellier<\/td><td>SLIME : a radhard, clockless, I2C slave for space application<\/td><\/tr><tr><td>2022<\/td><td>Wolte2022<\/td><td><\/td><td>M. Gonzalez, D. Pr\u00eale et al.<\/td><td>Ultra-low noise, temperature compensated amplifier characterization with cryogenic load<\/td><\/tr><tr><td>2022<\/td><td>Journal of Low Temperature Physics<\/td><td><\/td><td>M. Gonzalez et al.<\/td><td>Fully Differential Broadband LNA with Active Impedance Matching for SQUID Readout<\/td><\/tr><tr><td>2022<\/td><td>Space Telescopes and Instrumentation<\/td><td><\/td><td>Si Chen et al.<\/td><td>Monolithic amplifier and current biasing for SQUID readout &#8211; AwaXe_v4<\/td><\/tr><tr><td>2022<\/td><td>Journal of Low Temperature Physics<\/td><td><\/td><td>Si Chen et al.<\/td><td>Room Temperature ASIC for Cryogenic TES\/SQUID Control and Readout<\/td><\/tr><tr><td>2023<\/td><td>Journ\u00e9es de la Mi2i<\/td><td>Meudon<\/td><td>D. Charrier<\/td><td><a href=\"https:\/\/caemi2i.in2p3.fr\/wp-content\/uploads\/2024\/09\/RetT_BiCMOS_IHP130_DC-comp.pdf\">R&amp;T BiCMOS &#8211; IHP130<\/a><\/td><\/tr><tr><td>2023<\/td><td>MicDAT<\/td><td><\/td><td>Si. Chen et al.<\/td><td><a href=\"https:\/\/apc.u-paris.fr\/~prele\/Poster_MicDAT2023_Iref_SiCHEN_APC.pdf\">10 ppm\/K BiCMOS Temperature-Compensated Current Source<\/a><\/td><\/tr><tr><td>2023<\/td><td>MicDAT<\/td><td><\/td><td>Bao TON et al.<\/td><td><a href=\"https:\/\/apc.u-paris.fr\/~prele\/Poster_MicDAT_Conference_Bao_APC.pdf\">High Sensitivity On-Chip BiCMOS Thermometer with Differential Output and Offset Nulling<\/a><\/td><\/tr><tr><td>2024<\/td><td>Sensors &amp; Transducers<\/td><td><\/td><td>Bao TON et al.<\/td><td><a href=\"https:\/\/sensorsportal.com\/HTML\/DIGEST\/december_2023\/Vol_263\/ST_Vol_263_December_2023.pdf\">Setting Point and Operation Range of a BiCMOS On-Chip<br>BiCMOS Thermometer<\/a><\/td><\/tr><tr><td>2024<\/td><td>Journal of Low Temperature Physics<\/td><td><\/td><td>D. Pr\u00eale et al.<\/td><td>Conceptual design and analysis of a cryogenic front-end ASIC for TES readout using ST-130 nm BiCMOS technology<\/td><\/tr><tr><td>2024<\/td><td>SPIE Astro Telescop<\/td><td>Japan<\/td><td>Bao TON et al.<\/td><td><a href=\"https:\/\/www.researchgate.net\/publication\/383294063_Impact_of_space_ionizing_environment_on_the_warm_front-end_electronics_flicker_noise_used_for_TESSQUID_readout?_sg%5B0%5D=OXZLw-ZA97twmBeQSGcuRVw-KvdGSkACT8Ho1YCjJsVO7XKC2wexUtTyNc8LQ4vgVbjC9yD3U1HTenkYjzqNM6susJcQXh4i5r9pU8CN.M1nnk9RoC0wmQoihpGKQeZsWpfrFGClLClitRfiotfZQAcfn4g-Z9FRtMVl6QRT7L3uqTK80Y3wrZ_AM23R88w&amp;_tp=eyJjb250ZXh0Ijp7ImZpcnN0UGFnZSI6InB1YmxpY2F0aW9uIiwicGFnZSI6InByb2ZpbGUiLCJwcmV2aW91c1BhZ2UiOiJwcm9maWxlIiwicG9zaXRpb24iOiJwYWdlQ29udGVudCJ9fQ\">Impact of space ionizing environment on the warm front-end electronics flicker noise used for TES\/SQUID readout<\/a><\/td><\/tr><tr><td>2024<\/td><td>SPIE Astro Telescop<\/td><td>Japan<\/td><td>Si CHEN et al.<\/td><td><a href=\"https:\/\/www.researchgate.net\/publication\/383294058_ASIC_design_evolution_of_ATHENA_X-IFU_warm_front-end_electronics?_sg%5B0%5D=OXZLw-ZA97twmBeQSGcuRVw-KvdGSkACT8Ho1YCjJsVO7XKC2wexUtTyNc8LQ4vgVbjC9yD3U1HTenkYjzqNM6susJcQXh4i5r9pU8CN.M1nnk9RoC0wmQoihpGKQeZsWpfrFGClLClitRfiotfZQAcfn4g-Z9FRtMVl6QRT7L3uqTK80Y3wrZ_AM23R88w&amp;_tp=eyJjb250ZXh0Ijp7ImZpcnN0UGFnZSI6InB1YmxpY2F0aW9uIiwicGFnZSI6InByb2ZpbGUiLCJwcmV2aW91c1BhZ2UiOiJwcm9maWxlIiwicG9zaXRpb24iOiJwYWdlQ29udGVudCJ9fQ\">ASIC design evolution of ATHENA X-IFU warm front-end electronics<\/a><\/td><\/tr><tr><td>2024<\/td><td>TWEPP<\/td><td>Scotland<\/td><td>Alexandre Soulier (LPCA-MiCA) on behalf of ATLAS HGTD group<\/td><td><a href=\"https:\/\/indico.cern.ch\/event\/1381495\/contributions\/5988493\/attachments\/2869323\/5163702\/TWEPP2024_Soulier.pdf32_CMB-S4_SiGe_ASIC-based_daughter_board_for_low_temperature_detectors_front-end_analog_readout?_sg%5B0%5D=OXZLw-ZA97twmBeQSGcuRVw-KvdGSkACT8Ho1YCjJsVO7XKC2wexUtTyNc8LQ4vgVbjC9yD3U1HTenkYjzqNM6susJcQXh4i5r9pU8CN.M1nnk9RoC0wmQoihpGKQeZsWpfrFGClLClitRfiotfZQAcfn4g-Z9FRtMVl6QRT7L3uqTK80Y3wrZ_AM23R88w&amp;_tp=eyJjb250ZXh0Ijp7ImZpcnN0UGFnZSI6InB1YmxpY2F0aW9uIiwicGFnZSI6InByb2ZpbGUiLCJwcmV2aW91c1BhZ2UiOiJwcm9maWxlIiwicG9zaXRpb24iOiJwYWdlQ29udGVudCJ9fQ\">Implementation and performance of ALTIROC3 readout ASIC for the ATLAS HGTD timing detector<\/a><\/td><\/tr><tr><td>2024<\/td><td>IEEE<\/td><td>Florida<\/td><td>L. Alvado, N. Arveuf, R. Bonnefoy, L. Caponetto, T. Chaventr\u00e9, X. Chen, S. Drouet, F. Druillole, F. Jouve, I. Laktineh, L. Leterrier, S. Manen, H. Mathez, M-L. Mercier, A. Mhoudini, M. Morenas, G. Noel, L. Raux, P. Russo, C. Sylvia, P. Vallerand, R. Vandaele<\/td><td><a href=\"https:\/\/caemi2i.in2p3.fr\/wp-content\/uploads\/2025\/04\/Poster_FASTIME_IEEE_NSSMIC_2024_N13_008.pdf\" data-type=\"link\" data-id=\"https:\/\/caemi2i.in2p3.fr\/wp-content\/uploads\/2025\/04\/Poster_FASTIME_IEEE_NSSMIC_2024_N13_008.pdf\" target=\"_blank\" rel=\"noreferrer noopener\">Poster_FASTIME_IEEE_NSSMIC_2024_N13_008<\/a><\/td><\/tr><\/tbody><\/table><\/figure>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n","protected":false},"excerpt":{"rendered":"<p>date Conf \/ journal localisation Auteur titre 2015 NSS-MIC San Diego, USA E. Bechetoille Double Slope Dynamic Range and Low Noise CSA,&nbsp;slides 2016 Journal of Astronomical Telescopes, Instruments, and Systems D. Pr\u00eale et al. Gain drift compensation with no feedback-loop developed for the X-Ray Integral Field Unit\/ATHENA readout chain 2018 Journal of Low Temperature Physics [&hellip;]<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","ast-disable-related-posts":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"set","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ngg_post_thumbnail":0,"footnotes":""},"class_list":["post-313","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/pages\/313","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/comments?post=313"}],"version-history":[{"count":16,"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/pages\/313\/revisions"}],"predecessor-version":[{"id":1132,"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/pages\/313\/revisions\/1132"}],"wp:attachment":[{"href":"https:\/\/caemi2i.in2p3.fr\/index.php\/wp-json\/wp\/v2\/media?parent=313"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}