{"id":2187,"date":"2010-01-25T14:34:33","date_gmt":"2010-01-25T20:34:33","guid":{"rendered":"https:\/\/kermitmurray.com\/murray\/?p=2187"},"modified":"2019-08-03T16:11:16","modified_gmt":"2019-08-03T21:11:16","slug":"fast-photography-ir-maldi","status":"publish","type":"post","link":"https:\/\/kermitmurray.com\/research\/2010\/01\/fast-photography-ir-maldi\/","title":{"rendered":"Wavelength and time-resolved imaging of material ejection in infrared matrix-assisted laser desorption"},"content":{"rendered":"\n<div class=\"wp-block-caxton-grid relative\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-columns caxton-grid-block\" style=\"padding-top:0;padding-left:0;padding-bottom:0;padding-right:0;grid-template-columns:repeat(12, 1fr)\" data-tablet-css=\"padding-left:em;padding-right:em;\" data-mobile-css=\"padding-left:em;padding-right:em;\">\n<div class=\"wp-block-caxton-section relative\" style=\"grid-area:span 1\/span 12\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-section-block\" style=\"padding-top:5px;padding-left:5px;padding-bottom:5px;padding-right:5px\" data-mobile-css=\"padding-left:1em;padding-right:1em;\" data-tablet-css=\"padding-left:1em;padding-right:1em;\">\n<p>X. Fan, K.K. Murray, &#8220;Wavelength and time-resolved imaging of material ejection in infrared matrix-assisted laser desorption,&#8221; <em>J. Phys. Chem. A.<\/em> <strong>114<\/strong> (2010) 1492\u20131497. doi:<a href=\"http:\/\/doi.org\/10.1021\/jp9077163.\">10.1021\/jp9077163<\/a>.<\/p>\n\n\n\n<h4 class=\"wp-block-heading\">Abstract<\/h4>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"alignright is-resized\"><a href=\"https:\/\/kermitmurray.com\/murray\/research\/infrared-laser-desorption-and-ablation\/figure-2\/\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2011\/02\/Figure-2-439x1024.jpg\" alt=\"\" class=\"wp-image-668\" width=\"329\" height=\"768\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2011\/02\/Figure-2-439x1024.jpg 439w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2011\/02\/Figure-2-129x300.jpg 129w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2011\/02\/Figure-2.jpg 1728w\" sizes=\"auto, (max-width: 329px) 100vw, 329px\" \/><\/a><figcaption>Glycerol ablation at 2.94 \u03bcm and 3000 J\/m2 fluence after (a) 10 ns, (b) 100 ns, (c) 1 \u03bcs, (d) 10 \u03bcs, (e) 24 \u03bcs, (f) 50 \u03bcs, (g) 100 \u03bcs, (h) 200 \u03bcs, (i) 500 \u03bcs, and (j) 1 ms.<\/figcaption><\/figure><\/div>\n\n\n\n<p>The dynamics of glycerol ablation at atmospheric pressure was studied using fast photography. A mid-infrared optical parametric oscillator was used to irradiate a droplet of glycerol at normal incidence. The wavelength of the infrared source was tunable and was varied between 2.7 and 3.5 \u03bcm for the studies. After an adjustable delay, an excimer pumped dye laser was used to illuminate the expanding plume, and the 90\u00b0 scattered light was imaged with a high-speed CMOS camera. The time delay between the IR and UV lasers was varied up to 1 ms with a particular emphasis in the early stages of plume evolution below 1 \u03bcs. The threshold fluence for plume formation varied between 1000 and 6000 J\/m^2, and the minimum fluence corresponded to the OH stretch absorption of glycerol near 3.0 \u03bcm, which also corresponded to the greatest scattered light signal and duration of material emission. The velocity of the expanding plume was measured and ranged from &gt;300 m\/s near the OH stretch absorption to &lt;100 m\/s near the 3.4 \u03bcm CH stretch. Plume modeling calculations suggest that material removal is driven by phase explosion in the stress confinement regime that is at a maximum near the wavelength of the OH stretch absorption.<\/p>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-caxton-grid relative\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-columns caxton-grid-block\" style=\"padding-top:0;padding-left:0;padding-bottom:0;padding-right:0;grid-template-columns:repeat(12, 1fr)\" data-tablet-css=\"padding-left:em;padding-right:em;\" data-mobile-css=\"padding-left:em;padding-right:em;\">\n<div class=\"wp-block-caxton-section relative\" style=\"grid-area:span 1\/span 6\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-section-block\" style=\"padding-top:5px;padding-left:5px;padding-bottom:5px;padding-right:5px\" data-mobile-css=\"padding-left:1em;padding-right:1em;\" data-tablet-css=\"padding-left:1em;padding-right:1em;\">\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"768\" height=\"1024\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-768x1024.jpg\" alt=\"Fast photography setup from Fan &amp; Murray, J. Phys. Chem. A. 114 (2010) 1492\" class=\"wp-image-2191\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-768x1024.jpg 768w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-225x300.jpg 225w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup.jpg 1500w\" sizes=\"auto, (max-width: 768px) 100vw, 768px\" \/><figcaption>Fast photography setup from Fan &amp; Murray, J. Phys. Chem. A. 114 (2010) 1492<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-caxton-section relative\" style=\"grid-area:span 1\/span 6\"><div class=\"absolute absolute--fill\"><div class=\"cover bg-center absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );\"><\/div><div class=\"absolute absolute--fill\" style=\"background-color:;background-image:linear-gradient( );opacity:1;\"><\/div><\/div><div class=\"relative caxton-section-block\" style=\"padding-top:5px;padding-left:5px;padding-bottom:5px;padding-right:5px\" data-mobile-css=\"padding-left:1em;padding-right:1em;\" data-tablet-css=\"padding-left:1em;padding-right:1em;\">\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"768\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-Closeup-1024x768.jpg\" alt=\"Fast photography setup (closeup) from Fan &amp; Murray, J. Phys. Chem. A. 114 (2010) 1492\" class=\"wp-image-2192\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-Closeup-1024x768.jpg 1024w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-Closeup-300x225.jpg 300w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-Closeup-768x576.jpg 768w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-Closeup-1568x1176.jpg 1568w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Setup-Closeup.jpg 2000w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption>Fast photography setup (closeup) from Fan &amp; Murray, J. Phys. Chem. A. 114 (2010) 1492<\/figcaption><\/figure>\n\n\n\n<figure class=\"wp-block-image\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"608\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2019\/07\/Fast-Photography-Figure_1-1024x608.gif\" alt=\"\" class=\"wp-image-2190\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Figure_1-1024x608.gif 1024w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Figure_1-300x178.gif 300w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Figure_1-768x456.gif 768w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/07\/Fast-Photography-Figure_1-1568x931.gif 1568w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption>Instrument diagram from Fan &amp; Murray, J. Phys. Chem. A. 114 (2010) 1492<\/figcaption><\/figure>\n<\/div><\/div>\n<\/div><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":2192,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[81,134,65,5],"tags":[64,96,8,135,103,77],"class_list":["post-2187","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-fundamentals","category-lsu","category-photo","category-publication","tag-ablation","tag-glycerol","tag-infrared","tag-lsu","tag-photography","tag-publication","entry"],"_links":{"self":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2187","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/comments?post=2187"}],"version-history":[{"count":4,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2187\/revisions"}],"predecessor-version":[{"id":2304,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2187\/revisions\/2304"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/media\/2192"}],"wp:attachment":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/media?parent=2187"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/categories?post=2187"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/tags?post=2187"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}