{"id":2600,"date":"2003-07-19T22:00:09","date_gmt":"2003-07-20T03:00:09","guid":{"rendered":"https:\/\/kermitmurray.com\/murray\/?p=2600"},"modified":"2019-08-19T22:18:09","modified_gmt":"2019-08-20T03:18:09","slug":"two-laser-ir-and-uv-maldi","status":"publish","type":"post","link":"https:\/\/kermitmurray.com\/research\/2003\/07\/two-laser-ir-and-uv-maldi\/","title":{"rendered":"Two-laser infrared and ultraviolet matrix-assisted laser desorption\/ionization"},"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>M.W. Little, J.-K. Kim, K.K. Murray, &#8220;Two-laser infrared and ultraviolet matrix-assisted laser desorption\/ionization,&#8221; <em>J. Mass Spectrom.<\/em><strong>38<\/strong> (2003) 772\u2013777. doi:<a href=\"http:\/\/doi.org\/10.1002\/jms.494\">10.1002\/jms.494<\/a>. <\/p>\n\n\n\n<h4 class=\"wp-block-heading\">Abstract<\/h4>\n\n\n\n<p>Matrix\u2010assisted laser desorption\/ionization (MALDI) was performed using two pulsed lasers with wavelengths in the IR and UV regions. A 10.6 \u00b5m pulsed CO<sub>2<\/sub>&nbsp;laser was used to irradiate a MALDI target, followed after an adjustable delay by a 337 nm pulsed nitrogen laser. The sample consisted of a 2,5\u2010dihydroxybenzoic acid matrix and bovine insulin guest molecule. The pulse energy for both of the lasers was adjusted so that the ion of interest, either the matrix or guest ion, was not produced by either of the lasers alone. The delay time for maximum ion yield occurs at 1 \u00b5s for matrix and guest ions and the signal decayed to zero in \u223c400 \u00b5s. A mechanism is presented for enhanced UV MALDI ion yield following the IR laser pulse based on transient heating.<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"alignright is-resized\"><a href=\"https:\/\/kermitmurray.com\/murray\/little-jms-2003-fig-1\/\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2019\/08\/Little-JMS-2003-Fig-1-1024x309.jpg\" alt=\"Two-laser IR\/UV MALDI\" class=\"wp-image-2603\" width=\"768\" height=\"232\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/08\/Little-JMS-2003-Fig-1-1024x309.jpg 1024w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/08\/Little-JMS-2003-Fig-1-300x90.jpg 300w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/08\/Little-JMS-2003-Fig-1-768x232.jpg 768w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/08\/Little-JMS-2003-Fig-1-1568x473.jpg 1568w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2019\/08\/Little-JMS-2003-Fig-1.jpg 2000w\" sizes=\"auto, (max-width: 768px) 100vw, 768px\" \/><\/a><figcaption>Schematic layout of the two-laser IR\/UV MALDI experiments using a linear time-of-flight mass spectrometer (TOF MS). The infrared (IR) and ultraviolet (UV) lasers are directed at the same target spot from opposite sides of the instrument. The computer (PC) controls the delay generator (DG) and digital oscilloscope (DO).<\/figcaption><\/figure><\/div>\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\"><a href=\"https:\/\/kermitmurray.com\/murray\/11-20-04-05-32-pm\/\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"768\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2015\/07\/11-20-04-05-32-PM-1024x768.jpg\" alt=\"Home-built linear TOF mass spectrometer\" class=\"wp-image-883\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2015\/07\/11-20-04-05-32-PM-1024x768.jpg 1024w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2015\/07\/11-20-04-05-32-PM-300x225.jpg 300w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/a><figcaption>Linear time-of-flight mass spectrometer<\/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\"><a href=\"https:\/\/kermitmurray.com\/murray\/ltof_11_03\/\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"768\" src=\"https:\/\/kermitmurray.com\/murray\/wp-content\/uploads\/2015\/07\/LTOF_11_03-1024x768.jpg\" alt=\"Linear TOF MS source chamber\" class=\"wp-image-913\" srcset=\"https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2015\/07\/LTOF_11_03-1024x768.jpg 1024w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2015\/07\/LTOF_11_03-300x225.jpg 300w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2015\/07\/LTOF_11_03-768x576.jpg 768w, https:\/\/kermitmurray.com\/research\/wp-content\/uploads\/2015\/07\/LTOF_11_03-1568x1176.jpg 1568w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/a><figcaption>Linear time-of-flight mass spectrometer source chamber<\/figcaption><\/figure>\n<\/div><\/div>\n<\/div><\/div>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":2603,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[81,134,5],"tags":[8,9,149,75],"class_list":["post-2600","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-fundamentals","category-lsu","category-publication","tag-infrared","tag-maldi","tag-mechanism","tag-ultraviolet","entry"],"_links":{"self":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2600","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=2600"}],"version-history":[{"count":6,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2600\/revisions"}],"predecessor-version":[{"id":2607,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/posts\/2600\/revisions\/2607"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/media\/2603"}],"wp:attachment":[{"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/media?parent=2600"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/categories?post=2600"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/kermitmurray.com\/research\/wp-json\/wp\/v2\/tags?post=2600"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}