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...
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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 |
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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 & 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 & 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&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 & Francis Group</general><general>Taylor & 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 & Francis Group</pub><doi>10.1080/00268979000102531</doi><tpages>12</tpages></addata></record> |
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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 |
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