{"id":1215,"date":"2022-12-25T18:38:19","date_gmt":"2022-12-25T17:38:19","guid":{"rendered":"http:\/\/s848664668.onlinehome.fr\/Wordpress\/?p=1215"},"modified":"2025-12-21T16:58:27","modified_gmt":"2025-12-21T15:58:27","slug":"picoseconde-et-femtoseconde-doubleur-de-frequence","status":"publish","type":"post","link":"https:\/\/www.swissrocketman.fr\/Wordpress\/?p=1215","title":{"rendered":"Doubleur de fr\u00e9quence pour laser femtoseconde titane saphir \u00e0 800 nm"},"content":{"rendered":"<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-0  el_before_av_one_full  avia-builder-el-first  \" style='border-radius:0px; '><div  style='padding-bottom:10px; ' class='av-special-heading av-special-heading-h2  blockquote classic-quote  avia-builder-el-1  avia-builder-el-no-sibling  '><h2 class='av-special-heading-tag '  itemprop=\"headline\"  >Doubleur de fr\u00e9quence pour laser femtoseconde titane saphir \u00e0 800 nm<\/h2><div class='special-heading-border'><div class='special-heading-inner-border' ><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-2  el_after_av_one_full  el_before_av_one_full  column-top-margin\" style='border-radius:0px; '><div  class='avia-image-container  av-styling-    avia-builder-el-3  avia-builder-el-no-sibling  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><img decoding=\"async\" class='wp-image-1406 avia-img-lazy-loading-not-1406 avia_image' src=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m.jpg\" alt='' title='m' height=\"816\" width=\"1086\"  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m.jpg 1086w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m-300x225.jpg 300w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m-1030x774.jpg 1030w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m-768x577.jpg 768w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m-705x530.jpg 705w\" sizes=\"(max-width: 1086px) 100vw, 1086px\" \/><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-4  el_after_av_one_full  el_before_av_one_half  column-top-margin\" style='border-radius:0px; '><section class=\"av_textblock_section \"  itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/BlogPosting\" itemprop=\"blogPost\" ><div class='avia_textblock  '   itemprop=\"text\" ><h4>Doubleur de fr\u00e9quence pour laser femtoseconde titane saphir \u00e0 800 nm muni d&rsquo;un cristal doubleur en LBO de 5x5x1 mm mont\u00e9 sur un rail lin\u00e9aire actionn\u00e9 par un micro moteur piezo \u00e9lectrique. Ce doubleur permet de r\u00e9aliser des pulses lasers de 90 femtoseconde entre 345 et 520 nm.<\/h4>\n<\/div><\/section><\/div>\n<div class=\"flex_column av_one_half  flex_column_div av-zero-column-padding first  avia-builder-el-6  el_after_av_one_full  el_before_av_one_half  column-top-margin\" style='border-radius:0px; '><div  class='avia-image-container  av-styling-    avia-builder-el-7  avia-builder-el-no-sibling  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><img decoding=\"async\" class='wp-image-1220 avia-img-lazy-loading-not-1220 avia_image' src=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-scaled.jpg\" alt='' title='P1020105' height=\"1920\" width=\"2560\"  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-scaled.jpg 2560w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-300x225.jpg 300w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-1030x773.jpg 1030w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-768x576.jpg 768w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-1536x1152.jpg 1536w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-2048x1536.jpg 2048w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-1500x1125.jpg 1500w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020105-1-705x529.jpg 705w\" sizes=\"(max-width: 2560px) 100vw, 2560px\" \/><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_half  flex_column_div av-zero-column-padding   avia-builder-el-8  el_after_av_one_half  el_before_av_one_half  column-top-margin\" style='border-radius:0px; '><div  class='avia-image-container  av-styling-    avia-builder-el-9  avia-builder-el-no-sibling  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><img decoding=\"async\" class='wp-image-1221 avia-img-lazy-loading-not-1221 avia_image' src=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-scaled.jpg\" alt='' title='P1020106' height=\"1920\" width=\"2560\"  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-scaled.jpg 2560w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-300x225.jpg 300w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-1030x773.jpg 1030w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-768x576.jpg 768w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-1536x1152.jpg 1536w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-2048x1536.jpg 2048w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-1500x1125.jpg 1500w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020106-705x529.jpg 705w\" sizes=\"(max-width: 2560px) 100vw, 2560px\" \/><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_half  flex_column_div av-zero-column-padding first  avia-builder-el-10  el_after_av_one_half  el_before_av_one_half  column-top-margin\" style='border-radius:0px; '><div  class='avia-image-container  av-styling-    avia-builder-el-11  avia-builder-el-no-sibling  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><img decoding=\"async\" class='wp-image-1226 avia-img-lazy-loading-not-1226 avia_image' src=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-scaled.jpg\" alt='' title='P1020103' height=\"1920\" width=\"2560\"  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-scaled.jpg 2560w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-300x225.jpg 300w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-1030x773.jpg 1030w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-768x576.jpg 768w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-1536x1152.jpg 1536w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-2048x1536.jpg 2048w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-1500x1125.jpg 1500w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/P1020103-705x529.jpg 705w\" sizes=\"(max-width: 2560px) 100vw, 2560px\" \/><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_half  flex_column_div av-zero-column-padding   avia-builder-el-12  el_after_av_one_half  el_before_av_one_full  column-top-margin\" style='border-radius:0px; '><div  class='avia-image-container  av-styling-    avia-builder-el-13  avia-builder-el-no-sibling  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><img decoding=\"async\" class='wp-image-1413 avia-img-lazy-loading-not-1413 avia_image' src=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m2.jpg\" alt='' title='m2' height=\"816\" width=\"1086\"  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m2.jpg 1086w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m2-300x225.jpg 300w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m2-1030x774.jpg 1030w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m2-768x577.jpg 768w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/m2-705x530.jpg 705w\" sizes=\"(max-width: 1086px) 100vw, 1086px\" \/><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-14  el_after_av_one_half  el_before_av_one_full  column-top-margin\" style='border-radius:0px; '><div  class='avia-image-container  av-styling-    avia-builder-el-15  avia-builder-el-no-sibling  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><img decoding=\"async\" class='wp-image-2923 avia-img-lazy-loading-not-2923 avia_image' src=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2024-03-07-180714.jpg\" alt='' title='Capture d\u2019\u00e9cran 2024-03-07 180714' height=\"611\" width=\"1299\"  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2024-03-07-180714.jpg 1299w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2024-03-07-180714-300x141.jpg 300w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2024-03-07-180714-1030x484.jpg 1030w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2024-03-07-180714-768x361.jpg 768w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2024-03-07-180714-705x332.jpg 705w\" sizes=\"(max-width: 1299px) 100vw, 1299px\" \/><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-16  el_after_av_one_full  el_before_av_one_full  column-top-margin\" style='border-radius:0px; '><section class=\"av_textblock_section \"  itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/BlogPosting\" itemprop=\"blogPost\" ><div class='avia_textblock  '   itemprop=\"text\" ><h3 data-start=\"236\" data-end=\"276\"><span style=\"color: #ff00ff;\">1) Qu\u2019est-ce que c\u2019est:<\/span><\/h3>\n<p data-start=\"277\" data-end=\"670\">Un <strong data-start=\"280\" data-end=\"338\">doubleur de fr\u00e9quence (SHG, second-harmonic generator)<\/strong> transforme la sortie fondamentale d\u2019un Ti:Sapphire centr\u00e9e ~800 nm en sa seconde harmonique (~400 nm) via un cristal non lin\u00e9aire (typiquement BBO) mont\u00e9 dans un bo\u00eetier d\u2019accessoire : orientation de phase-matching, compenseurs de walk-off, et options THG\/FHG\/auto-tracking selon les versions. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<hr data-start=\"672\" data-end=\"675\" \/>\n<h3 data-start=\"677\" data-end=\"767\"><span style=\"color: #ff00ff;\">2) Ce que fait Coherent (produit type : <em data-start=\"720\" data-end=\"740\">Harmonic Generator<\/em> \/ accessoire Mira\/Mira-HP)<\/span><\/h3>\n<p data-start=\"768\" data-end=\"868\">Points-cl\u00e9s extraits du datasheet Coherent Harmonic Generator (accessoire pour Mira 900 \/ Mira-HP) :<\/p>\n<ul data-start=\"869\" data-end=\"1346\">\n<li data-start=\"869\" data-end=\"966\">\n<p data-start=\"871\" data-end=\"966\">Con\u00e7u pour SHG\/THG\/FHG avec cristaux index\u00e9s magn\u00e9tiquement (changement simple des cristaux).<\/p>\n<\/li>\n<li data-start=\"967\" data-end=\"1034\">\n<p data-start=\"969\" data-end=\"1034\">Walk-off compensator pour conserver la circularit\u00e9 du faisceau.<\/p>\n<\/li>\n<li data-start=\"1035\" data-end=\"1089\">\n<p data-start=\"1037\" data-end=\"1089\">Delay compensator pour g\u00e9n\u00e9ration en ligne du THG.<\/p>\n<\/li>\n<li data-start=\"1090\" data-end=\"1206\">\n<p data-start=\"1092\" data-end=\"1206\">Option <strong data-start=\"1099\" data-end=\"1114\">Autotracker<\/strong> : optimisation automatique du phase-matching quand on change la longueur d\u2019onde d\u2019entr\u00e9e.<\/p>\n<\/li>\n<li data-start=\"1207\" data-end=\"1346\">\n<p data-start=\"1209\" data-end=\"1346\">Plage d\u2019entr\u00e9e typique : <strong data-start=\"1234\" data-end=\"1249\">680\u20131080 nm<\/strong> ; sortie SHG autour de <strong data-start=\"1273\" data-end=\"1287\">340\u2013540 nm<\/strong> selon configuration. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<\/ul>\n<h3 data-start=\"1348\" data-end=\"1410\">Rendements (exemples fournis par Coherent pour <strong data-start=\"1399\" data-end=\"1409\">800 nm<\/strong>)<\/h3>\n<p data-start=\"1411\" data-end=\"1469\">(les chiffres varient selon la source de pompage \/ mod\u00e8le)<\/p>\n<ul data-start=\"1470\" data-end=\"1794\">\n<li data-start=\"1470\" data-end=\"1560\">\n<p data-start=\"1472\" data-end=\"1560\"><strong data-start=\"1472\" data-end=\"1498\">Mira-HP-F (pompe 18 W)<\/strong> : SHG \u2248 <strong data-start=\"1507\" data-end=\"1514\">40%<\/strong> \u2192 ~1.4 W \u00e0 400 nm (pour certains r\u00e9glages).<\/p>\n<\/li>\n<li data-start=\"1561\" data-end=\"1642\">\n<p data-start=\"1563\" data-end=\"1642\"><strong data-start=\"1563\" data-end=\"1589\">Mira-900-F (10 W pump)<\/strong> : SHG \u2248 <strong data-start=\"1598\" data-end=\"1605\">40%<\/strong> \u2192 560 mW \u00e0 400 nm (exemple donn\u00e9).<\/p>\n<\/li>\n<li data-start=\"1643\" data-end=\"1794\">\n<p data-start=\"1645\" data-end=\"1794\">Pour versions \u00e0 plus faible pompe, les pourcentages chutent (voir tableau de Coherent pour valeurs d\u00e9taill\u00e9es). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<\/ul>\n<hr data-start=\"1796\" data-end=\"1799\" \/>\n<h3 data-start=\"1801\" data-end=\"1870\"><span style=\"color: #ff00ff;\">3) Cristaux et optique non lin\u00e9aire (aspects physiques importants)<\/span><\/h3>\n<ul data-start=\"1871\" data-end=\"2512\">\n<li data-start=\"1871\" data-end=\"2192\">\n<p data-start=\"1873\" data-end=\"2192\"><strong data-start=\"1873\" data-end=\"1909\">Cristal courant : BBO (\u03b2-BaB\u2082O\u2084)<\/strong> \u2014 large bande passante, bonne r\u00e9sistance \u00e0 la PV et utilis\u00e9 pour SHG autour de 800\u2192400 nm. La bande passante de phase-matching d\u00e9pend de l\u2019\u00e9paisseur : par ex. BBO 0.15\u20130.60 mm a une largeur de phase-matching importante (utile pour pulses fs). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.thorlabs.com\/newgrouppage9.cfm?objectgroup_id=15444&amp;utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">thorlabs.com<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"2193\" data-end=\"2512\">\n<p data-start=\"2195\" data-end=\"2512\"><strong data-start=\"2195\" data-end=\"2226\">Compromis cristal-\u00e9paisseur<\/strong> : cristaux plus \u00e9pais \u2192 conversion \u2191 mais bande passante (spectrale) \u2193 et walk-off temporel \u2191 (d\u00e9gradation pour pulses tr\u00e8s courts). Pour pulses femtosecondes il est courant d\u2019utiliser cristaux fins ou des sch\u00e9mas compens\u00e9s (walk-off compensator). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.laserfocusworld.com\/lasers-sources\/article\/16556439\/back-to-basics-tunable-solid-state-lasers?utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">laserfocusworld.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<\/ul>\n<hr data-start=\"2514\" data-end=\"2517\" \/>\n<h3 data-start=\"2519\" data-end=\"2591\"><span style=\"color: #ff00ff;\">4) Effets sp\u00e9cifiques aux pulses femtosecondes (pratiques et limites)<\/span><\/h3>\n<ul data-start=\"2592\" data-end=\"3432\">\n<li data-start=\"2592\" data-end=\"2868\">\n<p data-start=\"2594\" data-end=\"2868\"><strong data-start=\"2594\" data-end=\"2619\">Large bande spectrale<\/strong> d\u2019un pulse fs (ex. 10\u2013100 nm selon la dur\u00e9e) exige un phase-matching large : qui favorise cristaux fins ou doubles-cristaux compens\u00e9s. Sinon la conversion se r\u00e9duit et le SHG peut \u00eatre spectrale\u00adment \u00e9troite. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.thorlabs.com\/newgrouppage9.cfm?objectgroup_id=15444&amp;utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">thorlabs.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"2869\" data-end=\"3195\">\n<p data-start=\"2871\" data-end=\"3195\"><strong data-start=\"2871\" data-end=\"2904\">Group velocity mismatch (GVM)<\/strong> et <strong data-start=\"2908\" data-end=\"2920\">walk-off<\/strong> : s\u00e9paration temporelle entre fondamental et SH \u00e0 l\u2019int\u00e9rieur du cristal \u2192 limite la conversion efficace si le pulse est tr\u00e8s court ou le cristal trop \u00e9pais. Les accessoires Coherent incluent des compensateurs pour limiter ces effets. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"3196\" data-end=\"3432\">\n<p data-start=\"3198\" data-end=\"3432\"><strong data-start=\"3198\" data-end=\"3226\">Dispersion &amp; compression<\/strong> : si vous doublez avant un appareil sensible (OPA, exp\u00e9riences de spectroscopie), faites attention \u00e0 la dispersion introduite et au chirp ; souvent on pr\u00e9f\u00e8re compenser \/ g\u00e9rer la dispersion en amont\/aval.<\/p>\n<\/li>\n<\/ul>\n<hr data-start=\"3434\" data-end=\"3437\" \/>\n<h3 data-start=\"3439\" data-end=\"3494\"><span style=\"color: #ff00ff;\">5) R\u00e9glages pratiques d\u2019alignement et d\u2019optimisation<\/span><\/h3>\n<ul data-start=\"3495\" data-end=\"4183\">\n<li data-start=\"3495\" data-end=\"3747\">\n<p data-start=\"3497\" data-end=\"3747\"><strong data-start=\"3497\" data-end=\"3516\">Taille de waist<\/strong> : il existe un optimum (Boyd-Kleinman) \u2014 trop serr\u00e9 \u2192 effets de diffusion\/dommage ; trop large \u2192 conversion faible. Coherent donne des recommandations d\u2019implantation\/optique selon le mod\u00e8le. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"3748\" data-end=\"4007\">\n<p data-start=\"3750\" data-end=\"4007\"><strong data-start=\"3750\" data-end=\"3779\">Temp\u00e9rature &amp; orientation<\/strong> du cristal : la phase-matching est obtenu par orientation (angle), parfois par temp\u00e9rature pour d\u2019autres cristaux ; Coherent utilise des montures magn\u00e9tiques pour faciliter le changement. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"4008\" data-end=\"4183\">\n<p data-start=\"4010\" data-end=\"4183\"><strong data-start=\"4010\" data-end=\"4025\">Autotracker<\/strong> utile si vous balayez la longueur d\u2019onde ou si l\u2019alimentation varie \u2014 maintient la conversion optimale automatiquement. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<\/ul>\n<hr data-start=\"4185\" data-end=\"4188\" \/>\n<h3 data-start=\"4190\" data-end=\"4263\"><span style=\"color: #ff00ff;\">6) Param\u00e8tres \u00e0 demander \/ v\u00e9rifier si vous voulez int\u00e9grer ou acheter<\/span><\/h3>\n<ul data-start=\"4264\" data-end=\"4703\">\n<li data-start=\"4264\" data-end=\"4422\">\n<p data-start=\"4266\" data-end=\"4422\">Quel mod\u00e8le de Ti:Sa (Mira-900 \/ Mira-HP \/ Chameleon \/ Astrella, etc.) \u2014 Coherent propose des options compatibles. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"4423\" data-end=\"4600\">\n<p data-start=\"4425\" data-end=\"4600\">Puissance d\u2019entr\u00e9e (mW\/W) et r\u00e9p\u00e9tition (MHz \/ kHz) \u2014 rendements donn\u00e9s par Coherent d\u00e9pendent fortement de la pompe et de la config. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"4601\" data-end=\"4703\">\n<p data-start=\"4603\" data-end=\"4703\">Besoin de THG \/ FHG en plus du SHG ? (accessoire modulaire). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<\/ul>\n<hr data-start=\"4705\" data-end=\"4708\" \/>\n<h3 data-start=\"4710\" data-end=\"4777\"><span style=\"color: #ff00ff;\">7) R\u00e9f\u00e9rences utiles (pour lire les fiches techniques compl\u00e8tes)<\/span><\/h3>\n<ul data-start=\"4778\" data-end=\"5355\">\n<li data-start=\"4778\" data-end=\"4890\">\n<p data-start=\"4780\" data-end=\"4890\">Coherent \u2014 <em data-start=\"4791\" data-end=\"4811\">Harmonic Generator<\/em> (datasheet pour Mira 900 \/ Mira-HP). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/Harmonic-Generator-Data-Sheet.pdf\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"4891\" data-end=\"5042\">\n<p data-start=\"4893\" data-end=\"5042\">Coherent \u2014 fiches produit Ti:Sapphire (Mira, Mira-HP, Chameleon, Astrella) selon votre source fondamentale. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.coherent.com\/resources\/datasheet\/lasers\/COHR_MiraHP_DS_0318_2.pdf?utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">Coherent Inc<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"5043\" data-end=\"5189\">\n<p data-start=\"5045\" data-end=\"5189\">Thorlabs \u2014 sp\u00e9cifications BBO et discussion sur la bande passante\/\u00e9paisseur (utile pour dimensionner). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.thorlabs.com\/newgrouppage9.cfm?objectgroup_id=15444&amp;utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between overflow-hidden\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">thorlabs.com<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"5190\" data-end=\"5355\">\n<p data-start=\"5192\" data-end=\"5355\">Article \/ revue technique sur la conversion de fr\u00e9quence et compromis pour fs pulses (revue technique \/ Laser Focus World)<\/p>\n<\/li>\n<\/ul>\n<\/div><\/section><\/div>\n<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-18  el_after_av_one_full  el_before_av_one_full  column-top-margin\" style='border-radius:0px; '><section class=\"av_textblock_section \"  itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/BlogPosting\" itemprop=\"blogPost\" ><div class='avia_textblock  '   itemprop=\"text\" ><h3 data-start=\"203\" data-end=\"231\">1. Structure g\u00e9n\u00e9rale<\/h3>\n<ul data-start=\"255\" data-end=\"477\">\n<li data-start=\"255\" data-end=\"380\">\n<p data-start=\"257\" data-end=\"380\"><span style=\"color: #ff0000;\"><strong data-start=\"257\" data-end=\"282\">Entr\u00e9e 800 nm (rouge)<\/strong> : le faisceau Ti:saphir arrive ici, g\u00e9n\u00e9ralement polaris\u00e9 lin\u00e9airement (p ou s selon le cristal).<\/span><\/p>\n<\/li>\n<li data-start=\"381\" data-end=\"477\">\n<p data-start=\"383\" data-end=\"477\"><span style=\"color: #3366ff;\"><strong data-start=\"383\" data-end=\"407\">Sortie 400 nm (bleu)<\/strong> : \u00e9mission du rayonnement doubl\u00e9, s\u00e9par\u00e9 spatialement du fondamental.<\/span><\/p>\n<\/li>\n<\/ul>\n<p data-start=\"479\" data-end=\"648\">Entre ces deux points, on voit une succession de <strong data-start=\"528\" data-end=\"553\">miroirs di\u00e9lectriques<\/strong>, un <strong data-start=\"558\" data-end=\"582\">cristal non lin\u00e9aire<\/strong> et plusieurs <strong data-start=\"596\" data-end=\"622\">optiques de s\u00e9paration<\/strong> (dichro\u00efques ou filtres).<\/p>\n<hr data-start=\"650\" data-end=\"653\" \/>\n<h3 data-start=\"655\" data-end=\"697\">2. Interpr\u00e9tation du trajet optique<\/h3>\n<h4 data-start=\"699\" data-end=\"744\">a) Pr\u00e9paration du faisceau (zone entr\u00e9e)<\/h4>\n<p data-start=\"745\" data-end=\"820\">Les <strong data-start=\"749\" data-end=\"774\">deux premiers miroirs<\/strong> (ceux proches de \u201centr\u00e9e 800 nm\u201d) servent \u00e0 :<\/p>\n<ul data-start=\"821\" data-end=\"932\">\n<li data-start=\"821\" data-end=\"876\">\n<p data-start=\"823\" data-end=\"876\">ajuster l\u2019angle d\u2019incidence vers le c\u0153ur du module,<\/p>\n<\/li>\n<li data-start=\"877\" data-end=\"932\">\n<p data-start=\"879\" data-end=\"932\">centrer et r\u00e9gler la taille du waist dans le cristal.<\/p>\n<\/li>\n<\/ul>\n<p data-start=\"934\" data-end=\"1082\">Le montage est typiquement en <strong data-start=\"964\" data-end=\"990\">configuration de repli<\/strong> pour augmenter la compacit\u00e9 et permettre un alignement fin du faisceau dans le cristal BBO.<\/p>\n<hr data-start=\"1084\" data-end=\"1087\" \/>\n<h4 data-start=\"1089\" data-end=\"1137\">b) Interaction non lin\u00e9aire (zone centrale)<\/h4>\n<p data-start=\"1138\" data-end=\"1386\">Le faisceau 800 nm passe ensuite dans le <strong data-start=\"1179\" data-end=\"1194\">cristal BBO<\/strong> (le petit composant mont\u00e9 verticalement ou l\u00e9g\u00e8rement inclin\u00e9, souvent entre deux optiques fines).<br data-start=\"1293\" data-end=\"1296\" \/>\u2192 C\u2019est ici qu\u2019a lieu la <strong data-start=\"1321\" data-end=\"1366\">g\u00e9n\u00e9ration de la seconde harmonique (SHG)<\/strong> par interaction \u03c7\u00b2.<\/p>\n<p data-start=\"1388\" data-end=\"1423\">Souvent, le cristal est mont\u00e9 sur :<\/p>\n<ul data-start=\"1424\" data-end=\"1590\">\n<li data-start=\"1424\" data-end=\"1486\">\n<p data-start=\"1426\" data-end=\"1486\">une <strong data-start=\"1430\" data-end=\"1450\">platine rotative<\/strong> (pour l\u2019angle de phase-matching),<\/p>\n<\/li>\n<li data-start=\"1487\" data-end=\"1590\">\n<p data-start=\"1489\" data-end=\"1590\">et un <strong data-start=\"1495\" data-end=\"1528\">support magn\u00e9tiquement index\u00e9<\/strong> (pour le remplacement rapide ou le changement d\u2019axe optique).<\/p>\n<\/li>\n<\/ul>\n<p data-start=\"1592\" data-end=\"1789\">La zone blanche cylindrique sur ta photo est tr\u00e8s probablement un <strong data-start=\"1658\" data-end=\"1686\">compensateur de walk-off<\/strong> (ou un second cristal mont\u00e9 t\u00eate-b\u00eache pour corriger la d\u00e9viation spatiale entre les deux fr\u00e9quences).<\/p>\n<hr data-start=\"1791\" data-end=\"1794\" \/>\n<h4 data-start=\"1796\" data-end=\"1828\">c) S\u00e9paration et extraction<\/h4>\n<p data-start=\"1829\" data-end=\"1886\">Apr\u00e8s la g\u00e9n\u00e9ration, tu observes deux chemins distincts :<\/p>\n<ul data-start=\"1887\" data-end=\"2183\">\n<li data-start=\"1887\" data-end=\"2026\">\n<p data-start=\"1889\" data-end=\"2026\"><strong data-start=\"1889\" data-end=\"1913\">Ligne bleue (400 nm)<\/strong> : le faisceau doubl\u00e9 est d\u00e9vi\u00e9 par un <strong data-start=\"1952\" data-end=\"1973\">miroir dichro\u00efque<\/strong> (haute r\u00e9flexion \u00e0 400 nm, transmission \u00e0 800 nm).<\/p>\n<\/li>\n<li data-start=\"2027\" data-end=\"2183\">\n<p data-start=\"2029\" data-end=\"2183\"><strong data-start=\"2029\" data-end=\"2063\">Ligne orange (800 nm r\u00e9siduel)<\/strong> : le fondamental continue, souvent absorb\u00e9 ou dirig\u00e9 vers un <strong data-start=\"2125\" data-end=\"2133\">dump<\/strong> optique interne pour \u00e9viter les r\u00e9tro-r\u00e9flexions.<\/p>\n<\/li>\n<\/ul>\n<p data-start=\"2185\" data-end=\"2359\">Le composant rouge \u00e0 la sortie (avec le connecteur) semble \u00eatre une <strong data-start=\"2253\" data-end=\"2278\">fibre optique UV\/bleu<\/strong> ou un <strong data-start=\"2285\" data-end=\"2310\">collimateur de sortie<\/strong> pour amener le 400 nm vers une autre exp\u00e9rience.<\/p>\n<hr data-start=\"2361\" data-end=\"2364\" \/>\n<h3 data-start=\"2366\" data-end=\"2402\">3. Points techniques notables<\/h3>\n<ul data-start=\"2403\" data-end=\"2919\">\n<li data-start=\"2403\" data-end=\"2541\">\n<p data-start=\"2405\" data-end=\"2541\"><strong data-start=\"2405\" data-end=\"2428\">Alignement critique<\/strong> : le 800 nm doit \u00eatre centr\u00e9 avec une incidence quasi-parall\u00e8le au plan du cristal pour un bon phase-matching.<\/p>\n<\/li>\n<li data-start=\"2542\" data-end=\"2698\">\n<p data-start=\"2544\" data-end=\"2698\"><strong data-start=\"2544\" data-end=\"2560\">Polarisation<\/strong> : la conversion BBO est polaris\u00e9e ; un demi-onde \u00e0 800 nm est souvent plac\u00e9 avant l\u2019entr\u00e9e pour optimiser la direction de polarisation.<\/p>\n<\/li>\n<li data-start=\"2699\" data-end=\"2799\">\n<p data-start=\"2701\" data-end=\"2799\"><strong data-start=\"2701\" data-end=\"2725\">S\u00e9paration spectrale<\/strong> : le dichro\u00efque final doit avoir un R(400 nm) &gt; 99 %, T(800 nm) &gt; 90 %.<\/p>\n<\/li>\n<li data-start=\"2800\" data-end=\"2919\">\n<p data-start=\"2802\" data-end=\"2919\"><strong data-start=\"2802\" data-end=\"2814\">S\u00e9curit\u00e9<\/strong> : attention \u00e0 la puissance UV \u2013 m\u00eame si elle para\u00eet faible, les 400 nm sont invisibles et phototoxiques.<\/p>\n<\/li>\n<\/ul>\n<hr data-start=\"2921\" data-end=\"2924\" \/>\n<h3 data-start=\"2926\" data-end=\"2945\">4. En r\u00e9sum\u00e9<\/h3>\n<div class=\"_tableContainer_1rjym_1\">\n<div class=\"group _tableWrapper_1rjym_13 flex w-fit flex-col-reverse\" tabindex=\"-1\">\n<table class=\"w-fit min-w-(--thread-content-width)\" data-start=\"2946\" data-end=\"3298\">\n<thead data-start=\"2946\" data-end=\"2974\">\n<tr data-start=\"2946\" data-end=\"2974\">\n<th data-start=\"2946\" data-end=\"2956\" data-col-size=\"sm\">\u00c9l\u00e9ment<\/th>\n<th data-start=\"2956\" data-end=\"2974\" data-col-size=\"md\">R\u00f4le principal<\/th>\n<\/tr>\n<\/thead>\n<tbody data-start=\"3005\" data-end=\"3298\">\n<tr data-start=\"3005\" data-end=\"3058\">\n<td data-start=\"3005\" data-end=\"3024\" data-col-size=\"sm\">Miroirs d\u2019entr\u00e9e<\/td>\n<td data-col-size=\"md\" data-start=\"3024\" data-end=\"3058\">Alignement et r\u00e9glage du waist<\/td>\n<\/tr>\n<tr data-start=\"3059\" data-end=\"3109\">\n<td data-start=\"3059\" data-end=\"3082\" data-col-size=\"sm\">Cristal BBO (ou LBO)<\/td>\n<td data-col-size=\"md\" data-start=\"3082\" data-end=\"3109\">Conversion 800 \u2192 400 nm<\/td>\n<\/tr>\n<tr data-start=\"3110\" data-end=\"3189\">\n<td data-start=\"3110\" data-end=\"3133\" data-col-size=\"sm\">Compensateur (blanc)<\/td>\n<td data-col-size=\"md\" data-start=\"3133\" data-end=\"3189\">Correction du walk-off et maintien du profil spatial<\/td>\n<\/tr>\n<tr data-start=\"3190\" data-end=\"3236\">\n<td data-start=\"3190\" data-end=\"3209\" data-col-size=\"sm\">Dichro\u00efque final<\/td>\n<td data-col-size=\"md\" data-start=\"3209\" data-end=\"3236\">S\u00e9paration 800 \/ 400 nm<\/td>\n<\/tr>\n<tr data-start=\"3237\" data-end=\"3298\">\n<td data-start=\"3237\" data-end=\"3257\" data-col-size=\"sm\">Collimateur rouge<\/td>\n<td data-col-size=\"md\" data-start=\"3257\" data-end=\"3298\">Extraction vers fibre ou sortie libre<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n<\/div>\n<\/div><\/section><\/div>\n<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-20  el_after_av_one_full  el_before_av_one_full  column-top-margin\" style='border-radius:0px; '><div  class='avia-image-container  av-styling-    avia-builder-el-21  avia-builder-el-no-sibling  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><img decoding=\"async\" class='wp-image-3576 avia-img-lazy-loading-not-3576 avia_image' src=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2025-10-11-133522.png\" alt='' title='Capture d&#039;\u00e9cran 2025-10-11 133522' height=\"625\" width=\"827\"  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2025-10-11-133522.png 827w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2025-10-11-133522-300x227.png 300w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2025-10-11-133522-768x580.png 768w, https:\/\/www.swissrocketman.fr\/Wordpress\/wp-content\/uploads\/2022\/12\/Capture-decran-2025-10-11-133522-705x533.png 705w\" sizes=\"(max-width: 827px) 100vw, 827px\" \/><\/div><\/div><\/div><\/div>\n<div class=\"flex_column av_one_full  flex_column_div av-zero-column-padding first  avia-builder-el-22  el_after_av_one_full  avia-builder-el-last  column-top-margin\" style='border-radius:0px; '><section class=\"av_textblock_section \"  itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/BlogPosting\" itemprop=\"blogPost\" ><div class='avia_textblock  '   itemprop=\"text\" ><ul data-start=\"252\" data-end=\"1239\">\n<li data-start=\"759\" data-end=\"1239\">\n<p data-start=\"761\" data-end=\"779\">Les GVM utilis\u00e9s :<\/p>\n<ul data-start=\"782\" data-end=\"1239\">\n<li data-start=\"782\" data-end=\"978\">\n<p data-start=\"784\" data-end=\"978\"><strong data-start=\"784\" data-end=\"806\">800 \u2192 400 nm (BBO)<\/strong> : GVM \u2248 <strong data-start=\"815\" data-end=\"828\">192 fs\/mm<\/strong> (valeur tir\u00e9e de tables fournisseurs \/ litt\u00e9rature \u2014 coh\u00e9rente avec les tableaux fabricants pour BBO type I). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.newlightphotonics.com\/Thin-Ultrathin-BBO-Crystals?utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">newlightphotonics.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"981\" data-end=\"1239\">\n<p data-start=\"983\" data-end=\"1239\"><strong data-start=\"983\" data-end=\"1006\">1060 \u2192 530 nm (BBO)<\/strong> : GVM \u2248 <strong data-start=\"1015\" data-end=\"1028\">120 fs\/mm<\/strong> (estimation raisonnable bas\u00e9e sur tables fournisseurs \/ valeurs commerciales ; la valeur d\u00e9pend du cut cristallin et du type de phase-matching \u2014 voir remarques ci-dessous). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/eksmaoptics.com\/femtoline-components\/femtoline-nonlinear-laser-crystals\/bbo-crystals-for-shg-of-yb-kgw-kyw-frequency-conversion\/?utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">eksmaoptics.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<h3 data-start=\"1241\" data-end=\"1275\"><span style=\"color: #3366ff;\">Graphique et tableau (r\u00e9sultats)<\/span><\/h3>\n<p data-start=\"1276\" data-end=\"1293\">Je t\u2019ai affich\u00e9 :<\/p>\n<ul data-start=\"1294\" data-end=\"1476\">\n<li data-start=\"1294\" data-end=\"1349\">\n<p data-start=\"1296\" data-end=\"1349\">un graphique log\u2013log L_max(\u03c4) pour 800 nm et 1060 nm,<\/p>\n<\/li>\n<li data-start=\"1350\" data-end=\"1476\">\n<p data-start=\"1352\" data-end=\"1476\">un tableau d\u2019exemples pratiques (1 \u03bcs, 1 ps, 100 fs, 50 fs, 20 fs, 10 fs, 5 fs) avec L_max en mm et un commentaire pratique.<\/p>\n<\/li>\n<\/ul>\n<p data-start=\"1478\" data-end=\"1510\">Exemples (extraits du tableau) :<\/p>\n<ul data-start=\"1511\" data-end=\"1786\">\n<li data-start=\"1511\" data-end=\"1577\">\n<p data-start=\"1513\" data-end=\"1577\">100 fs \u2192 L_max \u2248 <strong data-start=\"1530\" data-end=\"1541\">0.52 mm<\/strong> (800 nm) ; <strong data-start=\"1553\" data-end=\"1564\">0.83 mm<\/strong> (1060 nm).<\/p>\n<\/li>\n<li data-start=\"1578\" data-end=\"1643\">\n<p data-start=\"1580\" data-end=\"1643\">50 fs \u2192 L_max \u2248 <strong data-start=\"1596\" data-end=\"1607\">0.26 mm<\/strong> (800 nm) ; <strong data-start=\"1619\" data-end=\"1630\">0.42 mm<\/strong> (1060 nm).<\/p>\n<\/li>\n<li data-start=\"1644\" data-end=\"1727\">\n<p data-start=\"1646\" data-end=\"1727\">10 fs \u2192 L_max \u2248 <strong data-start=\"1662\" data-end=\"1674\">0.052 mm<\/strong> = 52 \u00b5m (800 nm) ; <strong data-start=\"1694\" data-end=\"1706\">0.083 mm<\/strong> = 83 \u00b5m (1060 nm).<\/p>\n<\/li>\n<li data-start=\"1728\" data-end=\"1786\">\n<p data-start=\"1730\" data-end=\"1786\">5 fs \u2192 L_max \u2248 <strong data-start=\"1745\" data-end=\"1754\">26 \u00b5m<\/strong> (800 nm) ; <strong data-start=\"1766\" data-end=\"1775\">42 \u00b5m<\/strong> (1060 nm).<\/p>\n<\/li>\n<\/ul>\n<p data-start=\"1788\" data-end=\"2110\">Ces valeurs donnent l\u2019\u00e9chelle \u00e0 laquelle il faut choisir (ou limiter) l\u2019\u00e9paisseur du cristal. Elles concordent qualitativement avec les recommandations des fournisseurs (ex. BBO \u00e9paisseur de 0.05\u20130.5 mm pour pulses de 10\u2013100 fs ; \u00e9paisseurs \u00ab ultrathin \u00bb 10\u201350 \u00b5m pour pulses ~10 fs). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/eksmaoptics.com\/nonlinear-and-laser-crystals\/nonlinear-crystals\/ultrathin-crystals-for-femtosecond-applications\/?utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">eksmaoptics.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<h3 data-start=\"2112\" data-end=\"2173\"><span style=\"color: #3366ff;\">Remarques importantes et limites<\/span><\/h3>\n<ol data-start=\"2174\" data-end=\"3970\">\n<li data-start=\"2174\" data-end=\"2907\">\n<p data-start=\"2177\" data-end=\"2275\"><strong data-start=\"2177\" data-end=\"2228\">C\u2019est une estimation de premi\u00e8re approximation.<\/strong> Le choix pratique du cristal d\u00e9pend aussi de :<\/p>\n<ul data-start=\"2279\" data-end=\"2907\">\n<li data-start=\"2279\" data-end=\"2444\">\n<p data-start=\"2281\" data-end=\"2444\">bande-passante spectrale du pulse (phase-matching spectral bandwidth) ; cristaux plus \u00e9pais r\u00e9duisent la largeur spectrale efficace \u2192 perte pour pulses fs larges ;<\/p>\n<\/li>\n<li data-start=\"2448\" data-end=\"2569\">\n<p data-start=\"2450\" data-end=\"2569\">walk-off spatial (birefringent walk-off) et maniement du profil spatial (compensateurs, configuration double-cristal) ;<\/p>\n<\/li>\n<li data-start=\"2573\" data-end=\"2708\">\n<p data-start=\"2575\" data-end=\"2708\">dispersion du cristal (GVD) qui peut \u00e9largir le pulse dans le cristal ; pour pulses tr\u00e8s courts la GVD peut aussi devenir limitante ;<\/p>\n<\/li>\n<li data-start=\"2712\" data-end=\"2804\">\n<p data-start=\"2714\" data-end=\"2804\">intensit\u00e9 (efficacit\u00e9 non lin\u00e9aire cro\u00eet avec longueur mais sature\/dommage si trop long) ;<\/p>\n<\/li>\n<li data-start=\"2808\" data-end=\"2907\">\n<p data-start=\"2810\" data-end=\"2907\">coupe et type de phase-matching (type I vs II, cut angle) qui modifient GVM pr\u00e9cis et efficacit\u00e9.<\/p>\n<\/li>\n<\/ul>\n<\/li>\n<li data-start=\"2908\" data-end=\"3331\">\n<p data-start=\"2911\" data-end=\"3331\"><strong data-start=\"2911\" data-end=\"2969\">GVM varie selon la coupe du cristal et la polarisation<\/strong> \u2014 les valeurs num\u00e9riques ci-dessus sont repr\u00e9sentatives (et concordent avec tables fabricants), mais pour un dimensionnement final il faut calculer GVM avec les \u00e9quations de Sellmeier pour la coupe exacte du cristal et la configuration (type I\/II). Voir Sellmeier ou tableaux fournisseurs (Eksma, Thorlabs, Newlight, etc.). <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.spiedigitallibrary.org\/conference-proceedings-of-spie\/11670\/116701E\/Updated-Sellmeier-equations-of-%CE%B2-BaB2O4\/10.1117\/12.2576038.full?sessionGUID=ead49a28-531a-b0d3-a6b0-3c97c009b6bc&amp;webSyncID=ad059329-ad88-3c9d-902b-c9993ced268b&amp;utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">spiedigitallibrary.org<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"3332\" data-end=\"3609\">\n<p data-start=\"3335\" data-end=\"3609\"><strong data-start=\"3335\" data-end=\"3363\">Pour des pulses &lt; ~20 fs<\/strong>, on passe souvent \u00e0 des cristaux mont\u00e9s tr\u00e8s fins (10\u201350 \u00b5m) ou \u00e0 des sch\u00e9mas compens\u00e9s (deux cristaux t\u00eate-b\u00eache + compensateur temporel) pour r\u00e9cup\u00e9rer l\u2019efficacit\u00e9 tout en pr\u00e9servant la largeur spectrale. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/eksmaoptics.com\/nonlinear-and-laser-crystals\/nonlinear-crystals\/ultrathin-crystals-for-femtosecond-applications\/?utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">eksmaoptics.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+1<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"3610\" data-end=\"3970\">\n<p data-start=\"3613\" data-end=\"3970\"><strong data-start=\"3613\" data-end=\"3640\">Pour des dur\u00e9es longues<\/strong> (ps \u2192 \u00b5s), la limite dominante devient plut\u00f4t la tol\u00e9rance angulaire \/ longueur de coh\u00e9rence \u0394k (phase matching) et la transparence (on peut utiliser des cristaux de plusieurs mm voire cm selon application) \u2014 la formule \u03c4\/GVM devient triviale (donne des longueurs \u00e9normes), mais on est alors limit\u00e9 par d\u2019autres effets pratiques.<\/p>\n<\/li>\n<\/ol>\n<h3 data-start=\"3972\" data-end=\"4003\"><span style=\"color: #3366ff;\">Sources et lecture conseill\u00e9e<\/span><\/h3>\n<ul data-start=\"4004\" data-end=\"4422\">\n<li data-start=\"4004\" data-end=\"4206\">\n<p data-start=\"4006\" data-end=\"4206\">Tables et recommandations fournisseur (EKSMA, Newlight Photonics, Thorlabs, Eksma datasheets) \u2014 montrent valeurs de GVM et \u00e9paisseurs commerciales pour fs \u2192 ps. <span class=\"\" data-state=\"closed\"><span class=\"ms-1 inline-flex max-w-full items-center relative top-&#091;-0.094rem&#093; animate-&#091;show_150ms_ease-in&#093;\" data-testid=\"webpage-citation-pill\"><a class=\"flex h-4.5 overflow-hidden rounded-xl px-2 text-&#091;9px&#093; font-medium transition-colors duration-150 ease-in-out text-token-text-secondary! bg-&#091;#F4F4F4&#093;! dark:bg-&#091;#303030&#093;!\" href=\"https:\/\/www.newlightphotonics.com\/Thin-Ultrathin-BBO-Crystals?utm_source=chatgpt.com\" target=\"_blank\" rel=\"noopener\"><span class=\"relative start-0 bottom-0 flex h-full w-full items-center\"><span class=\"flex h-4 w-full items-center justify-between\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">newlightphotonics.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+2<\/span><\/span><span class=\"flex h-4 w-full items-center justify-between absolute\"><span class=\"max-w-&#091;15ch&#093; grow truncate overflow-hidden text-center\">eksmaoptics.com<\/span><span class=\"-me-1 flex h-full items-center rounded-full px-1 text-&#091;#8F8F8F&#093;\">+2<\/span><\/span><\/span><\/a><\/span><\/span><\/p>\n<\/li>\n<li data-start=\"4207\" data-end=\"4422\">\n<p data-start=\"4209\" data-end=\"4422\">Documents th\u00e9oriques sur GVM \/ phase-matching et calculs Sellmeier pour BBO si tu veux une valeur pr\u00e9cise (selon coupe) : articles SPIE \/ Optica et mises \u00e0 jour des Sellmeier.<\/p>\n<\/li>\n<li data-start=\"4207\" data-end=\"4422\">\n<p data-start=\"166\" data-end=\"212\">Tr\u00e8s probablement <strong data-start=\"184\" data-end=\"202\">BBO (\u03b2-BaB\u2082O\u2084)<\/strong>, pas LBO.<\/p>\n<h2 data-start=\"214\" data-end=\"240\">Pourquoi (raisonnement)<\/h2>\n<ol data-start=\"241\" data-end=\"1443\">\n<li data-start=\"241\" data-end=\"890\">\n<p data-start=\"244\" data-end=\"392\"><strong data-start=\"244\" data-end=\"307\">Livre d\u2019usage pour Ti:Saphir femtoseconde (\u2248800 nm, 140 fs)<\/strong> : les doubles pour pulses femto utilisent quasi syst\u00e9matiquement <strong data-start=\"373\" data-end=\"380\">BBO<\/strong> parce que<\/p>\n<ul data-start=\"396\" data-end=\"890\">\n<li data-start=\"396\" data-end=\"507\">\n<p data-start=\"398\" data-end=\"507\">il a un <strong data-start=\"406\" data-end=\"440\">coefficient non lin\u00e9aire \u00e9lev\u00e9<\/strong> \u2192 rendement de conversion important m\u00eame sur cristaux tr\u00e8s fins,<\/p>\n<\/li>\n<li data-start=\"511\" data-end=\"601\">\n<p data-start=\"513\" data-end=\"601\">large <strong data-start=\"519\" data-end=\"543\">acceptance spectrale<\/strong> compatible avec la large bande spectrale des pulses fs,<\/p>\n<\/li>\n<li data-start=\"605\" data-end=\"890\">\n<p data-start=\"607\" data-end=\"890\">possibilit\u00e9 d\u2019utiliser des <strong data-start=\"634\" data-end=\"658\">cristaux tr\u00e8s minces<\/strong> (r\u00e9duit la dispersion \/ group velocity mismatch) \u2014 critique pour 140 fs.<br data-start=\"731\" data-end=\"734\" \/><strong data-start=\"737\" data-end=\"744\">LBO<\/strong> est plut\u00f4t pr\u00e9f\u00e9r\u00e9 pour CW ou ps\/longs pulses \u00e0 haute puissance o\u00f9 la faible bir\u00e9fringence (moins de walk-off) et la robustesse sont importantes.<\/p>\n<\/li>\n<\/ul>\n<\/li>\n<li data-start=\"892\" data-end=\"1131\">\n<p data-start=\"895\" data-end=\"1131\"><strong data-start=\"895\" data-end=\"921\">Contrainte d\u2019\u00e9paisseur<\/strong> : pour 140 fs on choisit souvent des \u00e9paisseurs de l\u2019ordre de quelques centaines de microm\u00e8tres (BBO). LBO typique est plus \u00e9pais (millim\u00e8tres), ce qui d\u00e9graderait les pulses tr\u00e8s courts par dispersion et GVM.<\/p>\n<\/li>\n<li data-start=\"1133\" data-end=\"1301\">\n<p data-start=\"1136\" data-end=\"1301\"><strong data-start=\"1136\" data-end=\"1164\">Sensibilit\u00e9 d\u2019alignement<\/strong> : BBO demande un r\u00e9glage angulaire tr\u00e8s fin (on voit des supports microm\u00e9triques sur la photo) \u2014 coh\u00e9rent avec un BBO mont\u00e9 pour SHG fs.<\/p>\n<\/li>\n<li data-start=\"1303\" data-end=\"1443\">\n<p data-start=\"1306\" data-end=\"1443\"><strong data-start=\"1306\" data-end=\"1331\">Pratique industrielle<\/strong> : les accessoires \/ modules SHG fournis avec lasers Ti:Sapphire (MIRA\/Coherent) ont historiquement utilis\u00e9 BBO.<\/p>\n<\/li>\n<\/ol>\n<\/li>\n<\/ul>\n<\/div><\/section><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":1218,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[6],"tags":[],"class_list":["post-1215","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-lasers-a-solides"],"_links":{"self":[{"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=\/wp\/v2\/posts\/1215","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=1215"}],"version-history":[{"count":28,"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=\/wp\/v2\/posts\/1215\/revisions"}],"predecessor-version":[{"id":4067,"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=\/wp\/v2\/posts\/1215\/revisions\/4067"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=\/wp\/v2\/media\/1218"}],"wp:attachment":[{"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1215"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=1215"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.swissrocketman.fr\/Wordpress\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=1215"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}