Vacuum UV spectroscopy and dynamics of CHF3: analysis of emissions and evidence for parent ion emission

The fluorescence observed following electron impact and vacuum UV photon excitation of fluoroform (CHF 3 ) are studied using three techniques: (a) electron beam excitation of a supersonic molecular beam with dispersed fluorescence detection; (b) He* and Ne* rare-gas metastable excitation at room tem...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Molecular physics 1990-12, Vol.71 (6), p.1355-1366
Hauptverfasser: Creasey, J.C., Lambert, I.R., Tuckett, R.P., Hopkirk, A.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 1366
container_issue 6
container_start_page 1355
container_title Molecular physics
container_volume 71
creator Creasey, J.C.
Lambert, I.R.
Tuckett, R.P.
Hopkirk, A.
description The fluorescence observed following electron impact and vacuum UV photon excitation of fluoroform (CHF 3 ) are studied using three techniques: (a) electron beam excitation of a supersonic molecular beam with dispersed fluorescence detection; (b) He* and Ne* rare-gas metastable excitation at room temperature with dispersed fluorescence detection; (c) photon excitation at room temperature using tunable vacuum UV radiation from a synchrotron source with undispersed fluorescence detection. Using the first two techniques, the spectra are dominated by CF 2 Ã-[Xtilde] fluorescence. The spectra are continuous owing to the high density of rovibrational transitions, but a vibrational progression in the bending mode is observed in the rare-gas metastable experiment at high gas pressure. Using photons in the energy range 11-35 eV, three distinct fluorescence decay channels are observed: (1) CF 3 fluorescence for photon energies 11-13 eV; (2) CF 2 fluorescence for energies 14-18 eV; (3) CHF + 3 fluorescence for energies greater than 20 eV. The shapes of the excitation functions confirm that (1) and (2) are resonant processes via Rydberg states of CHF 3 , but (3) is a non-resonant photoionisation process. The emitting state in CHF + 3 is the [Dtilde] 2 A 1 state, with a vertical ionisation potential of 20·5 eV. Using the synchrotron in its single-bunch mode, radiative lifetimes of the fluorescing electronic states of CF 3 , CF 2 and CHF + 3 have been measured to be 17, 52 and 80 ns respectively.
doi_str_mv 10.1080/00268979000102531
format Article
fullrecord <record><control><sourceid>pascalfrancis_infor</sourceid><recordid>TN_cdi_pascalfrancis_primary_19447936</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>19447936</sourcerecordid><originalsourceid>FETCH-LOGICAL-i236t-dbae5999ba1ac01e40205aabfda7c3e52de7f216d5df169be45a46ba22d6935b3</originalsourceid><addsrcrecordid>eNpl0D1PwzAQBmALgUQp_AA2L4wBf8ROjVhQRClSJRbaNbrYDjJK4shOQfn3uC2wMJ1099zp9CJ0TcktJQtyRwiTC1UoQgglTHB6gmaUS5ZxwhanaLafZwnIc3QR40diMsEZet-C3u06vNniOFg9Bh-1HyYMvcFm6qFzOmLf4HK15PepC-0U3aFjOxej8308WPvpjO21xY0PeIBg-xGn4Z-6RGcNtNFe_dQ52iyf3spVtn59fikf15ljXI6ZqcEKpVQNFDShNieMCIC6MVBobgUztmgYlUaYhkpV21xALmtgzEjFRc3n6OZ4d4CooW0C9NrFagiugzBVVOV5obhM7uHoXJ8-7uDLh9ZUI0ytD79LnJJqH271L1z-DSl1bhI</addsrcrecordid><sourcetype>Index Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Vacuum UV spectroscopy and dynamics of CHF3: analysis of emissions and evidence for parent ion emission</title><source>Taylor &amp; Francis Journals Complete</source><creator>Creasey, J.C. ; Lambert, I.R. ; Tuckett, R.P. ; Hopkirk, A.</creator><creatorcontrib>Creasey, J.C. ; Lambert, I.R. ; Tuckett, R.P. ; Hopkirk, A.</creatorcontrib><description>The fluorescence observed following electron impact and vacuum UV photon excitation of fluoroform (CHF 3 ) are studied using three techniques: (a) electron beam excitation of a supersonic molecular beam with dispersed fluorescence detection; (b) He* and Ne* rare-gas metastable excitation at room temperature with dispersed fluorescence detection; (c) photon excitation at room temperature using tunable vacuum UV radiation from a synchrotron source with undispersed fluorescence detection. Using the first two techniques, the spectra are dominated by CF 2 Ã-[Xtilde] fluorescence. The spectra are continuous owing to the high density of rovibrational transitions, but a vibrational progression in the bending mode is observed in the rare-gas metastable experiment at high gas pressure. Using photons in the energy range 11-35 eV, three distinct fluorescence decay channels are observed: (1) CF 3 fluorescence for photon energies 11-13 eV; (2) CF 2 fluorescence for energies 14-18 eV; (3) CHF + 3 fluorescence for energies greater than 20 eV. The shapes of the excitation functions confirm that (1) and (2) are resonant processes via Rydberg states of CHF 3 , but (3) is a non-resonant photoionisation process. The emitting state in CHF + 3 is the [Dtilde] 2 A 1 state, with a vertical ionisation potential of 20·5 eV. Using the synchrotron in its single-bunch mode, radiative lifetimes of the fluorescing electronic states of CF 3 , CF 2 and CHF + 3 have been measured to be 17, 52 and 80 ns respectively.</description><identifier>ISSN: 0026-8976</identifier><identifier>EISSN: 1362-3028</identifier><identifier>DOI: 10.1080/00268979000102531</identifier><identifier>CODEN: MOPHAM</identifier><language>eng</language><publisher>London: Taylor &amp; Francis Group</publisher><subject>Atomic and molecular physics ; Exact sciences and technology ; Molecular properties and interactions with photons ; Photon interactions with molecules ; Physics</subject><ispartof>Molecular physics, 1990-12, Vol.71 (6), p.1355-1366</ispartof><rights>Copyright Taylor &amp; Francis Group, LLC 1990</rights><rights>1991 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.tandfonline.com/doi/pdf/10.1080/00268979000102531$$EPDF$$P50$$Ginformaworld$$H</linktopdf><linktohtml>$$Uhttps://www.tandfonline.com/doi/full/10.1080/00268979000102531$$EHTML$$P50$$Ginformaworld$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,59620,60409</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=19447936$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Creasey, J.C.</creatorcontrib><creatorcontrib>Lambert, I.R.</creatorcontrib><creatorcontrib>Tuckett, R.P.</creatorcontrib><creatorcontrib>Hopkirk, A.</creatorcontrib><title>Vacuum UV spectroscopy and dynamics of CHF3: analysis of emissions and evidence for parent ion emission</title><title>Molecular physics</title><description>The fluorescence observed following electron impact and vacuum UV photon excitation of fluoroform (CHF 3 ) are studied using three techniques: (a) electron beam excitation of a supersonic molecular beam with dispersed fluorescence detection; (b) He* and Ne* rare-gas metastable excitation at room temperature with dispersed fluorescence detection; (c) photon excitation at room temperature using tunable vacuum UV radiation from a synchrotron source with undispersed fluorescence detection. Using the first two techniques, the spectra are dominated by CF 2 Ã-[Xtilde] fluorescence. The spectra are continuous owing to the high density of rovibrational transitions, but a vibrational progression in the bending mode is observed in the rare-gas metastable experiment at high gas pressure. Using photons in the energy range 11-35 eV, three distinct fluorescence decay channels are observed: (1) CF 3 fluorescence for photon energies 11-13 eV; (2) CF 2 fluorescence for energies 14-18 eV; (3) CHF + 3 fluorescence for energies greater than 20 eV. The shapes of the excitation functions confirm that (1) and (2) are resonant processes via Rydberg states of CHF 3 , but (3) is a non-resonant photoionisation process. The emitting state in CHF + 3 is the [Dtilde] 2 A 1 state, with a vertical ionisation potential of 20·5 eV. Using the synchrotron in its single-bunch mode, radiative lifetimes of the fluorescing electronic states of CF 3 , CF 2 and CHF + 3 have been measured to be 17, 52 and 80 ns respectively.</description><subject>Atomic and molecular physics</subject><subject>Exact sciences and technology</subject><subject>Molecular properties and interactions with photons</subject><subject>Photon interactions with molecules</subject><subject>Physics</subject><issn>0026-8976</issn><issn>1362-3028</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1990</creationdate><recordtype>article</recordtype><recordid>eNpl0D1PwzAQBmALgUQp_AA2L4wBf8ROjVhQRClSJRbaNbrYDjJK4shOQfn3uC2wMJ1099zp9CJ0TcktJQtyRwiTC1UoQgglTHB6gmaUS5ZxwhanaLafZwnIc3QR40diMsEZet-C3u06vNniOFg9Bh-1HyYMvcFm6qFzOmLf4HK15PepC-0U3aFjOxej8308WPvpjO21xY0PeIBg-xGn4Z-6RGcNtNFe_dQ52iyf3spVtn59fikf15ljXI6ZqcEKpVQNFDShNieMCIC6MVBobgUztmgYlUaYhkpV21xALmtgzEjFRc3n6OZ4d4CooW0C9NrFagiugzBVVOV5obhM7uHoXJ8-7uDLh9ZUI0ytD79LnJJqH271L1z-DSl1bhI</recordid><startdate>19901220</startdate><enddate>19901220</enddate><creator>Creasey, J.C.</creator><creator>Lambert, I.R.</creator><creator>Tuckett, R.P.</creator><creator>Hopkirk, A.</creator><general>Taylor &amp; Francis Group</general><general>Taylor &amp; Francis</general><scope>IQODW</scope></search><sort><creationdate>19901220</creationdate><title>Vacuum UV spectroscopy and dynamics of CHF3: analysis of emissions and evidence for parent ion emission</title><author>Creasey, J.C. ; Lambert, I.R. ; Tuckett, R.P. ; Hopkirk, A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i236t-dbae5999ba1ac01e40205aabfda7c3e52de7f216d5df169be45a46ba22d6935b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1990</creationdate><topic>Atomic and molecular physics</topic><topic>Exact sciences and technology</topic><topic>Molecular properties and interactions with photons</topic><topic>Photon interactions with molecules</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Creasey, J.C.</creatorcontrib><creatorcontrib>Lambert, I.R.</creatorcontrib><creatorcontrib>Tuckett, R.P.</creatorcontrib><creatorcontrib>Hopkirk, A.</creatorcontrib><collection>Pascal-Francis</collection><jtitle>Molecular physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Creasey, J.C.</au><au>Lambert, I.R.</au><au>Tuckett, R.P.</au><au>Hopkirk, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Vacuum UV spectroscopy and dynamics of CHF3: analysis of emissions and evidence for parent ion emission</atitle><jtitle>Molecular physics</jtitle><date>1990-12-20</date><risdate>1990</risdate><volume>71</volume><issue>6</issue><spage>1355</spage><epage>1366</epage><pages>1355-1366</pages><issn>0026-8976</issn><eissn>1362-3028</eissn><coden>MOPHAM</coden><abstract>The fluorescence observed following electron impact and vacuum UV photon excitation of fluoroform (CHF 3 ) are studied using three techniques: (a) electron beam excitation of a supersonic molecular beam with dispersed fluorescence detection; (b) He* and Ne* rare-gas metastable excitation at room temperature with dispersed fluorescence detection; (c) photon excitation at room temperature using tunable vacuum UV radiation from a synchrotron source with undispersed fluorescence detection. Using the first two techniques, the spectra are dominated by CF 2 Ã-[Xtilde] fluorescence. The spectra are continuous owing to the high density of rovibrational transitions, but a vibrational progression in the bending mode is observed in the rare-gas metastable experiment at high gas pressure. Using photons in the energy range 11-35 eV, three distinct fluorescence decay channels are observed: (1) CF 3 fluorescence for photon energies 11-13 eV; (2) CF 2 fluorescence for energies 14-18 eV; (3) CHF + 3 fluorescence for energies greater than 20 eV. The shapes of the excitation functions confirm that (1) and (2) are resonant processes via Rydberg states of CHF 3 , but (3) is a non-resonant photoionisation process. The emitting state in CHF + 3 is the [Dtilde] 2 A 1 state, with a vertical ionisation potential of 20·5 eV. Using the synchrotron in its single-bunch mode, radiative lifetimes of the fluorescing electronic states of CF 3 , CF 2 and CHF + 3 have been measured to be 17, 52 and 80 ns respectively.</abstract><cop>London</cop><pub>Taylor &amp; Francis Group</pub><doi>10.1080/00268979000102531</doi><tpages>12</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0026-8976
ispartof Molecular physics, 1990-12, Vol.71 (6), p.1355-1366
issn 0026-8976
1362-3028
language eng
recordid cdi_pascalfrancis_primary_19447936
source Taylor & Francis Journals Complete
subjects Atomic and molecular physics
Exact sciences and technology
Molecular properties and interactions with photons
Photon interactions with molecules
Physics
title Vacuum UV spectroscopy and dynamics of CHF3: analysis of emissions and evidence for parent ion emission
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-09T22%3A54%3A18IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-pascalfrancis_infor&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Vacuum%20UV%20spectroscopy%20and%20dynamics%20of%20CHF3:%20analysis%20of%20emissions%20and%20evidence%20for%20parent%20ion%20emission&rft.jtitle=Molecular%20physics&rft.au=Creasey,%20J.C.&rft.date=1990-12-20&rft.volume=71&rft.issue=6&rft.spage=1355&rft.epage=1366&rft.pages=1355-1366&rft.issn=0026-8976&rft.eissn=1362-3028&rft.coden=MOPHAM&rft_id=info:doi/10.1080/00268979000102531&rft_dat=%3Cpascalfrancis_infor%3E19447936%3C/pascalfrancis_infor%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true