Trace gas detection of molecular hydrogen H(2) by photoacoustic stimulated Raman spectroscopy (PARS)
Photoacoustic stimulated Raman spectroscopy (PARS) has been used for sensitive and selective trace gas detection of molecular hydrogen under ambient conditions. In one experiment, 532 nm output of a seeded pulsed Nd:YAG laser is employed as Raman pump source and a Raman shifter filled with gaseous H...
Gespeichert in:
Veröffentlicht in: | Analyst (London) 2012-03, Vol.137 (6), p.1384-1388 |
---|---|
Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 1388 |
---|---|
container_issue | 6 |
container_start_page | 1384 |
container_title | Analyst (London) |
container_volume | 137 |
creator | Spencer, Claire Louise Watson, Verity Hippler, Michael |
description | Photoacoustic stimulated Raman spectroscopy (PARS) has been used for sensitive and selective trace gas detection of molecular hydrogen under ambient conditions. In one experiment, 532 nm output of a seeded pulsed Nd:YAG laser is employed as Raman pump source and a Raman shifter filled with gaseous H(2) to obtain Stokes shifted radiation at 683 nm, suitable to stimulate H(2) Raman detection in a photoacoustic cell. A noise equivalent detection limit of 40 ppm by volume H(2) in 1 atm N(2) is obtained (14 mJ at 532 nm, 18 mJ at 683 nm, 10 Hz repetition rate, 58 s measurement time). Another experiment employs a dye laser for stimulating Raman radiation between 681-684 nm, allowing tuneable PARS. A Gaussian spectral fitting procedure has been applied giving a noise equivalent detection limit of 4.6 ppm by volume H(2) in 1 atm N(2) (35 mJ pulse energy at 532 nm, 45 mJ at 681-684 nm, 10 Hz repetition rate, 256 s measurement time). Spectroscopic detection offers the advantage of high selectivity along with the ability to obtain temperature and dynamic information from the rotational population and a line shape analysis, and also allows the discrimination between ortho- and para-H(2). |
doi_str_mv | 10.1039/c2an15990b |
format | Article |
fullrecord | <record><control><sourceid>proquest_pubme</sourceid><recordid>TN_cdi_proquest_miscellaneous_923188753</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>923188753</sourcerecordid><originalsourceid>FETCH-LOGICAL-p557-1614e949bcd30baecea77651d108456a5ac866d39c90e4c5b6b4c9a5653cd1dd3</originalsourceid><addsrcrecordid>eNo1kLFOwzAURS0kREth4QOQN8oQsOPYiceqAopUCVS6Ry_Pr21QEoc4GfL3RKIs9y5HR1eXsTspnqRQ9hljaKS2VhQXbC6VSSKt42zGrkP4FkJIocUVm8WxErHM0jlz-w6Q-BECd9QT9qVvuD_w2leEQwUdP42u80dq-GYZP_Ji5O3J9x7QD6EvkU9RT1xPju-ghoaHdrJ0PqBvR778XO2-Hm_Y5QGqQLfnXrD968t-vYm2H2_v69U2arVOI2lkQjaxBTolCiAkSFOjpZMiS7QBDZgZ45RFKyhBXZgiQQvaaIVOOqcW7OFP23b-Z6DQ53UZkKoKGprW5jZWMstSrSby_kwORU0ub7uyhm7M_39RvwQ9YoU</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>923188753</pqid></control><display><type>article</type><title>Trace gas detection of molecular hydrogen H(2) by photoacoustic stimulated Raman spectroscopy (PARS)</title><source>Royal Society of Chemistry Journals Archive (1841-2007)</source><source>Royal Society Of Chemistry Journals 2008-</source><source>Alma/SFX Local Collection</source><creator>Spencer, Claire Louise ; Watson, Verity ; Hippler, Michael</creator><creatorcontrib>Spencer, Claire Louise ; Watson, Verity ; Hippler, Michael</creatorcontrib><description>Photoacoustic stimulated Raman spectroscopy (PARS) has been used for sensitive and selective trace gas detection of molecular hydrogen under ambient conditions. In one experiment, 532 nm output of a seeded pulsed Nd:YAG laser is employed as Raman pump source and a Raman shifter filled with gaseous H(2) to obtain Stokes shifted radiation at 683 nm, suitable to stimulate H(2) Raman detection in a photoacoustic cell. A noise equivalent detection limit of 40 ppm by volume H(2) in 1 atm N(2) is obtained (14 mJ at 532 nm, 18 mJ at 683 nm, 10 Hz repetition rate, 58 s measurement time). Another experiment employs a dye laser for stimulating Raman radiation between 681-684 nm, allowing tuneable PARS. A Gaussian spectral fitting procedure has been applied giving a noise equivalent detection limit of 4.6 ppm by volume H(2) in 1 atm N(2) (35 mJ pulse energy at 532 nm, 45 mJ at 681-684 nm, 10 Hz repetition rate, 256 s measurement time). Spectroscopic detection offers the advantage of high selectivity along with the ability to obtain temperature and dynamic information from the rotational population and a line shape analysis, and also allows the discrimination between ortho- and para-H(2).</description><identifier>EISSN: 1364-5528</identifier><identifier>DOI: 10.1039/c2an15990b</identifier><identifier>PMID: 22302187</identifier><language>eng</language><publisher>England</publisher><ispartof>Analyst (London), 2012-03, Vol.137 (6), p.1384-1388</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/22302187$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Spencer, Claire Louise</creatorcontrib><creatorcontrib>Watson, Verity</creatorcontrib><creatorcontrib>Hippler, Michael</creatorcontrib><title>Trace gas detection of molecular hydrogen H(2) by photoacoustic stimulated Raman spectroscopy (PARS)</title><title>Analyst (London)</title><addtitle>Analyst</addtitle><description>Photoacoustic stimulated Raman spectroscopy (PARS) has been used for sensitive and selective trace gas detection of molecular hydrogen under ambient conditions. In one experiment, 532 nm output of a seeded pulsed Nd:YAG laser is employed as Raman pump source and a Raman shifter filled with gaseous H(2) to obtain Stokes shifted radiation at 683 nm, suitable to stimulate H(2) Raman detection in a photoacoustic cell. A noise equivalent detection limit of 40 ppm by volume H(2) in 1 atm N(2) is obtained (14 mJ at 532 nm, 18 mJ at 683 nm, 10 Hz repetition rate, 58 s measurement time). Another experiment employs a dye laser for stimulating Raman radiation between 681-684 nm, allowing tuneable PARS. A Gaussian spectral fitting procedure has been applied giving a noise equivalent detection limit of 4.6 ppm by volume H(2) in 1 atm N(2) (35 mJ pulse energy at 532 nm, 45 mJ at 681-684 nm, 10 Hz repetition rate, 256 s measurement time). Spectroscopic detection offers the advantage of high selectivity along with the ability to obtain temperature and dynamic information from the rotational population and a line shape analysis, and also allows the discrimination between ortho- and para-H(2).</description><issn>1364-5528</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNo1kLFOwzAURS0kREth4QOQN8oQsOPYiceqAopUCVS6Ry_Pr21QEoc4GfL3RKIs9y5HR1eXsTspnqRQ9hljaKS2VhQXbC6VSSKt42zGrkP4FkJIocUVm8WxErHM0jlz-w6Q-BECd9QT9qVvuD_w2leEQwUdP42u80dq-GYZP_Ji5O3J9x7QD6EvkU9RT1xPju-ghoaHdrJ0PqBvR778XO2-Hm_Y5QGqQLfnXrD968t-vYm2H2_v69U2arVOI2lkQjaxBTolCiAkSFOjpZMiS7QBDZgZ45RFKyhBXZgiQQvaaIVOOqcW7OFP23b-Z6DQ53UZkKoKGprW5jZWMstSrSby_kwORU0ub7uyhm7M_39RvwQ9YoU</recordid><startdate>20120321</startdate><enddate>20120321</enddate><creator>Spencer, Claire Louise</creator><creator>Watson, Verity</creator><creator>Hippler, Michael</creator><scope>NPM</scope><scope>7X8</scope></search><sort><creationdate>20120321</creationdate><title>Trace gas detection of molecular hydrogen H(2) by photoacoustic stimulated Raman spectroscopy (PARS)</title><author>Spencer, Claire Louise ; Watson, Verity ; Hippler, Michael</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p557-1614e949bcd30baecea77651d108456a5ac866d39c90e4c5b6b4c9a5653cd1dd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Spencer, Claire Louise</creatorcontrib><creatorcontrib>Watson, Verity</creatorcontrib><creatorcontrib>Hippler, Michael</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>Analyst (London)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Spencer, Claire Louise</au><au>Watson, Verity</au><au>Hippler, Michael</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Trace gas detection of molecular hydrogen H(2) by photoacoustic stimulated Raman spectroscopy (PARS)</atitle><jtitle>Analyst (London)</jtitle><addtitle>Analyst</addtitle><date>2012-03-21</date><risdate>2012</risdate><volume>137</volume><issue>6</issue><spage>1384</spage><epage>1388</epage><pages>1384-1388</pages><eissn>1364-5528</eissn><abstract>Photoacoustic stimulated Raman spectroscopy (PARS) has been used for sensitive and selective trace gas detection of molecular hydrogen under ambient conditions. In one experiment, 532 nm output of a seeded pulsed Nd:YAG laser is employed as Raman pump source and a Raman shifter filled with gaseous H(2) to obtain Stokes shifted radiation at 683 nm, suitable to stimulate H(2) Raman detection in a photoacoustic cell. A noise equivalent detection limit of 40 ppm by volume H(2) in 1 atm N(2) is obtained (14 mJ at 532 nm, 18 mJ at 683 nm, 10 Hz repetition rate, 58 s measurement time). Another experiment employs a dye laser for stimulating Raman radiation between 681-684 nm, allowing tuneable PARS. A Gaussian spectral fitting procedure has been applied giving a noise equivalent detection limit of 4.6 ppm by volume H(2) in 1 atm N(2) (35 mJ pulse energy at 532 nm, 45 mJ at 681-684 nm, 10 Hz repetition rate, 256 s measurement time). Spectroscopic detection offers the advantage of high selectivity along with the ability to obtain temperature and dynamic information from the rotational population and a line shape analysis, and also allows the discrimination between ortho- and para-H(2).</abstract><cop>England</cop><pmid>22302187</pmid><doi>10.1039/c2an15990b</doi><tpages>5</tpages></addata></record> |
fulltext | fulltext |
identifier | EISSN: 1364-5528 |
ispartof | Analyst (London), 2012-03, Vol.137 (6), p.1384-1388 |
issn | 1364-5528 |
language | eng |
recordid | cdi_proquest_miscellaneous_923188753 |
source | Royal Society of Chemistry Journals Archive (1841-2007); Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
title | Trace gas detection of molecular hydrogen H(2) by photoacoustic stimulated Raman spectroscopy (PARS) |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-12T08%3A57%3A13IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_pubme&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Trace%20gas%20detection%20of%20molecular%20hydrogen%20H(2)%20by%20photoacoustic%20stimulated%20Raman%20spectroscopy%20(PARS)&rft.jtitle=Analyst%20(London)&rft.au=Spencer,%20Claire%20Louise&rft.date=2012-03-21&rft.volume=137&rft.issue=6&rft.spage=1384&rft.epage=1388&rft.pages=1384-1388&rft.eissn=1364-5528&rft_id=info:doi/10.1039/c2an15990b&rft_dat=%3Cproquest_pubme%3E923188753%3C/proquest_pubme%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=923188753&rft_id=info:pmid/22302187&rfr_iscdi=true |