{"id":502,"date":"2015-06-05T00:21:08","date_gmt":"2015-06-05T04:21:08","guid":{"rendered":"http:\/\/scholarblogs.emory.edu\/lianlab\/?page_id=502"},"modified":"2020-01-06T16:32:04","modified_gmt":"2020-01-06T20:32:04","slug":"transient-absorption-spectroscopy","status":"publish","type":"page","link":"https:\/\/scholarblogs.emory.edu\/lianlab\/transient-absorption-spectroscopy\/","title":{"rendered":"Transient Absorption Spectroscopy"},"content":{"rendered":"<p style=\"padding-left: 30px;text-align: justify\"><a href=\"http:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/05\/2.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-264 alignleft\" src=\"http:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/05\/2-1024x683.jpg\" alt=\"2\" width=\"495\" height=\"330\"><\/a>In the femtosecond transient absorption (fs-TA) technique a femtosecond pump pulse creates initial excited states, which are detected through changes in the transmission of a time-delayed probe pulse. In our lab, fs-TA experiments on quantum dot (QD) systems use UV or visible light as the pump, and white light continuum (WLC) as the probe, which can monitor electronic transitions. Meanwhile, we can also use mid-IR probe pulses obtained by difference-frequency mixing of two near-IR pulses provide an alternative way to study QD intraband transitions. This technique allow us to study the interfacial charge separation dynamics in photovoltaic nanomaterials.<\/p>\n<p>&nbsp;<\/p>\n<hr>\n<h4>Selected Publications<\/h4>\n<table style=\"width: 1057.38px\">\n<tbody>\n<tr>\n<td style=\"border-color: #ffffff;width: 473px\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/06\/QQ\u622a\u56fe20171120133906-e1511204183519.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-1008 size-thumbnail aligncenter\" src=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/06\/QQ\u622a\u56fe20171120133906-e1511204183519-150x150.jpg\" alt=\"\" width=\"150\" height=\"150\"><\/a><\/td>\n<td style=\"border-color: #ffffff;width: 575.383px\">Haiming Zhu, Ye Yang, Kaifeng Wu, Tianquan Lian, &nbsp;\u201d<a href=\"http:\/\/www.annualreviews.org\/doi\/abs\/10.1146\/annurev-physchem-040215-112128\" target=\"_blank\" rel=\"noopener noreferrer\">Charge Transfer Dynamics from Photoexcited Semiconductor Quantum Dots<\/a>\u201d,&nbsp;<strong>Annu. Rev. Phys. Chem.<\/strong>, 2016,&nbsp;67,1<\/td>\n<\/tr>\n<tr>\n<td style=\"border-color: #ffffff;width: 473px\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-972 size-thumbnail\" src=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/05\/CSR-150x150.jpg\" alt=\"\" width=\"150\" height=\"150\"><\/td>\n<td style=\"border-color: #ffffff;width: 575.383px\"><em>Kaifeng Wu, Tianquan Lian, \u201d<a href=\"http:\/\/pubs.rsc.org\/en\/content\/articlelanding\/2016\/cs\/c5cs00472a#!divAbstract\" target=\"_blank\" rel=\"noopener noreferrer\">Quantum confined colloidal nanorod heterostructures for solar-to-fuel conversion<\/a>\u201d&nbsp;Chem. Soc. Rev.,&nbsp;<\/em><strong>2016<\/strong>,&nbsp;<em>45<\/em>, 3781-810.<\/td>\n<\/tr>\n<tr>\n<td style=\"border-color: #ffffff;width: 473px\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/06\/QQ\u622a\u56fe20171120134411.jpg\"><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter wp-image-1009 size-thumbnail\" src=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/06\/QQ\u622a\u56fe20171120134411-150x150.jpg\" alt=\"\" width=\"150\" height=\"150\"><\/a><\/td>\n<td style=\"border-color: #ffffff;width: 575.383px\">Kaifeng Wu, Haiming Zhu, Tianquan Lian, \u201d<a href=\"http:\/\/pubs.acs.org\/doi\/abs\/10.1021\/ar500398g\">Ultrafast Exciton Dynamics and Light-Driven H<sub>2<\/sub> Evolution in Colloidal Semiconductor Nanorods and Pt-Tipped Nanorods<\/a>\u201d&nbsp;<strong>Acc. Chem. Res.<\/strong>,&nbsp;2015,&nbsp;48, 851\u2013859<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<h4>&nbsp;<\/h4>\n<hr>\n<h4>Other research Fields<\/h4>\n<table>\n<tbody>\n<tr>\n<td style=\"border-color: #ffffff;vertical-align: middle\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/sum-frequency-generation\/\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-497 size-medium aligncenter\" src=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/06\/20150529-DSC_0932-300x200.jpg\" alt=\"\" width=\"300\" height=\"200\" srcset=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/06\/20150529-DSC_0932-300x200.jpg 300w, https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/06\/20150529-DSC_0932-1024x683.jpg 1024w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a> &nbsp;<\/p>\n<p style=\"text-align: center\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/sum-frequency-generation\/\">Sum Frenquency Generation<\/a><\/p>\n<\/td>\n<td style=\"border-color: #ffffff;vertical-align: middle\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-266 size-medium aligncenter\" src=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/05\/3-300x200.jpg\" alt=\"\" width=\"300\" height=\"200\" srcset=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/05\/3-300x200.jpg 300w, https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2015\/05\/3-1024x683.jpg 1024w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/p>\n<p style=\"text-align: center\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/atomic-force-microscopy\/\">Single particle spectroscopy<\/a><\/p>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<table style=\"border-collapse: collapse;width: 100%\">\n<tbody>\n<tr>\n<td style=\"border-color: #ffffff;width: 49.8667%;vertical-align: middle\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/electrical-field-induced-second-harmonic-response\/\"><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-1295 aligncenter\" src=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2020\/01\/EFISH-300x256.png\" alt=\"\" width=\"290\" height=\"248\" srcset=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2020\/01\/EFISH-300x256.png 300w, https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2020\/01\/EFISH.png 704w\" sizes=\"auto, (max-width: 290px) 100vw, 290px\" \/><\/a>&nbsp;&nbsp;<\/p>\n<p style=\"text-align: center\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/electrical-field-induced-second-harmonic-response\/\">Electric Field Induced Second harmonic generation<\/a><\/p>\n<\/td>\n<td style=\"border-color: #ffffff;width: 49.8667%;vertical-align: middle\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/surface-enhanced-raman-spectroscopy\/\"><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-1471 aligncenter\" src=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2020\/01\/Raman-setup-illustration.png\" alt=\"\" width=\"360\" height=\"143\" srcset=\"https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2020\/01\/Raman-setup-illustration.png 715w, https:\/\/scholarblogs.emory.edu\/lianlab\/files\/2020\/01\/Raman-setup-illustration-300x119.png 300w\" sizes=\"auto, (max-width: 360px) 100vw, 360px\" \/><\/a> &nbsp;<\/p>\n<p style=\"text-align: center\"><a href=\"https:\/\/scholarblogs.emory.edu\/lianlab\/surface-enhanced-raman-spectroscopy\/\">Surface enhanced Raman spectroscopy<\/a><\/p>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n","protected":false},"excerpt":{"rendered":"<p>In the femtosecond transient absorption (fs-TA) technique a femtosecond pump pulse creates initial excited states, which are detected through changes in the transmission of a time-delayed probe pulse. In our lab, fs-TA experiments on quantum<\/p>\n","protected":false},"author":2944,"featured_media":0,"parent":0,"menu_order":14,"comment_status":"closed","ping_status":"closed","template":"template-fullwidth.php","meta":{"ngg_post_thumbnail":0,"footnotes":"","_links_to":"","_links_to_target":""},"class_list":["post-502","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/pages\/502","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/users\/2944"}],"replies":[{"embeddable":true,"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/comments?post=502"}],"version-history":[{"count":26,"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/pages\/502\/revisions"}],"predecessor-version":[{"id":1542,"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/pages\/502\/revisions\/1542"}],"wp:attachment":[{"href":"https:\/\/scholarblogs.emory.edu\/lianlab\/wp-json\/wp\/v2\/media?parent=502"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}