Rovibrational Energy Transfer in the 4νCH Manifold of Acetylene, Viewed by IR−UV Double Resonance Spectroscopy. 1. Foundation Studies at Low J

Time-resolved infrared-ultraviolet double resonance (IR−UV DR) spectroscopy is used to prepare acetylene molecules (C2H2) in specific rovibrational states of the 12 700 cm-1 4νCH manifold of the electronic ground-state Χ, monitoring their direct excitation and collision-induced state-to-state energy...

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Veröffentlicht in:The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 2003-12, Vol.107 (49), p.10759-10770
Hauptverfasser: Payne, Mark A, Milce, Angela P, Frost, Michael J, Orr, Brian J
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container_title The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory
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creator Payne, Mark A
Milce, Angela P
Frost, Michael J
Orr, Brian J
description Time-resolved infrared-ultraviolet double resonance (IR−UV DR) spectroscopy is used to prepare acetylene molecules (C2H2) in specific rovibrational states of the 12 700 cm-1 4νCH manifold of the electronic ground-state Χ, monitoring their direct excitation and collision-induced state-to-state energy transfer, by probing at ∼299 or ∼296 nm with laser-induced fluorescence via the Α electronic state. The 4νCH manifold derives much of its IR brightness from the (ν1 + 3ν3) combination band, such that many of the rotational levels J monitored by IR−UV DR are derived from the (1 0 3 0 0)0 vibrational state. The 4νCH manifold of C2H2 is congested and affected by anharmonic, l-resonance, and Coriolis couplings that cause other IR-dark, UV-bright rovibrational levels to attain appreciable IR−UV DR intensity and to add to the complexity of intramolecular dynamics in that manifold. Consequently, collision-induced rovibrational satellites observed by IR−UV DR comprise not only regular even-ΔJ features but also supposedly forbidden odd-ΔJ features, of which the energy-transfer channel from J = 12 to J = 1 is particularly efficient. This paper focuses on low-J rovibrational levels of the 4νCH manifold, particularly those with J = 0 and J = 1 in view of their anomalously large Stark effects that are likely to make them susceptible to collision-induced rovibrational mixing. Three complementary forms of IR−UV DR experiment are reported:  IR-scanned, UV-scanned, and kinetic. These indicate that strong IR−UV DR signals observed by probing the (1 0 3 0 0)0 J = 0 rovibrational level are complicated by underlying IR-dark, UV-bright states, making J = 0 unsuitable for systematic IR−UV DR studies. The (1 0 3 0 0)0 J = 1 rovibrational level is more amenable to unambiguous characterization and yields insight concerning even- and odd-ΔJ collision-induced rovibrational energy transfer and associated mechanisms.
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Foundation Studies at Low J</title><source>ACS Publications</source><creator>Payne, Mark A ; Milce, Angela P ; Frost, Michael J ; Orr, Brian J</creator><creatorcontrib>Payne, Mark A ; Milce, Angela P ; Frost, Michael J ; Orr, Brian J</creatorcontrib><description>Time-resolved infrared-ultraviolet double resonance (IR−UV DR) spectroscopy is used to prepare acetylene molecules (C2H2) in specific rovibrational states of the 12 700 cm-1 4νCH manifold of the electronic ground-state Χ, monitoring their direct excitation and collision-induced state-to-state energy transfer, by probing at ∼299 or ∼296 nm with laser-induced fluorescence via the Α electronic state. The 4νCH manifold derives much of its IR brightness from the (ν1 + 3ν3) combination band, such that many of the rotational levels J monitored by IR−UV DR are derived from the (1 0 3 0 0)0 vibrational state. The 4νCH manifold of C2H2 is congested and affected by anharmonic, l-resonance, and Coriolis couplings that cause other IR-dark, UV-bright rovibrational levels to attain appreciable IR−UV DR intensity and to add to the complexity of intramolecular dynamics in that manifold. Consequently, collision-induced rovibrational satellites observed by IR−UV DR comprise not only regular even-ΔJ features but also supposedly forbidden odd-ΔJ features, of which the energy-transfer channel from J = 12 to J = 1 is particularly efficient. This paper focuses on low-J rovibrational levels of the 4νCH manifold, particularly those with J = 0 and J = 1 in view of their anomalously large Stark effects that are likely to make them susceptible to collision-induced rovibrational mixing. Three complementary forms of IR−UV DR experiment are reported:  IR-scanned, UV-scanned, and kinetic. These indicate that strong IR−UV DR signals observed by probing the (1 0 3 0 0)0 J = 0 rovibrational level are complicated by underlying IR-dark, UV-bright states, making J = 0 unsuitable for systematic IR−UV DR studies. The (1 0 3 0 0)0 J = 1 rovibrational level is more amenable to unambiguous characterization and yields insight concerning even- and odd-ΔJ collision-induced rovibrational energy transfer and associated mechanisms.</description><identifier>ISSN: 1089-5639</identifier><identifier>EISSN: 1520-5215</identifier><identifier>DOI: 10.1021/jp035224t</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>The journal of physical chemistry. 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The 4νCH manifold of C2H2 is congested and affected by anharmonic, l-resonance, and Coriolis couplings that cause other IR-dark, UV-bright rovibrational levels to attain appreciable IR−UV DR intensity and to add to the complexity of intramolecular dynamics in that manifold. Consequently, collision-induced rovibrational satellites observed by IR−UV DR comprise not only regular even-ΔJ features but also supposedly forbidden odd-ΔJ features, of which the energy-transfer channel from J = 12 to J = 1 is particularly efficient. This paper focuses on low-J rovibrational levels of the 4νCH manifold, particularly those with J = 0 and J = 1 in view of their anomalously large Stark effects that are likely to make them susceptible to collision-induced rovibrational mixing. Three complementary forms of IR−UV DR experiment are reported:  IR-scanned, UV-scanned, and kinetic. These indicate that strong IR−UV DR signals observed by probing the (1 0 3 0 0)0 J = 0 rovibrational level are complicated by underlying IR-dark, UV-bright states, making J = 0 unsuitable for systematic IR−UV DR studies. 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Foundation Studies at Low J</title><author>Payne, Mark A ; Milce, Angela P ; Frost, Michael J ; Orr, Brian J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a1428-6e8ce5660e7765198979e34ee72f00c679e7cfa73b4155a425cfabf9d76ef68e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Payne, Mark A</creatorcontrib><creatorcontrib>Milce, Angela P</creatorcontrib><creatorcontrib>Frost, Michael J</creatorcontrib><creatorcontrib>Orr, Brian J</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><jtitle>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, &amp; general theory</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Payne, Mark A</au><au>Milce, Angela P</au><au>Frost, Michael J</au><au>Orr, Brian J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Rovibrational Energy Transfer in the 4νCH Manifold of Acetylene, Viewed by IR−UV Double Resonance Spectroscopy. 1. Foundation Studies at Low J</atitle><jtitle>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, &amp; general theory</jtitle><addtitle>J. Phys. Chem. A</addtitle><date>2003-12-11</date><risdate>2003</risdate><volume>107</volume><issue>49</issue><spage>10759</spage><epage>10770</epage><pages>10759-10770</pages><issn>1089-5639</issn><eissn>1520-5215</eissn><abstract>Time-resolved infrared-ultraviolet double resonance (IR−UV DR) spectroscopy is used to prepare acetylene molecules (C2H2) in specific rovibrational states of the 12 700 cm-1 4νCH manifold of the electronic ground-state Χ, monitoring their direct excitation and collision-induced state-to-state energy transfer, by probing at ∼299 or ∼296 nm with laser-induced fluorescence via the Α electronic state. The 4νCH manifold derives much of its IR brightness from the (ν1 + 3ν3) combination band, such that many of the rotational levels J monitored by IR−UV DR are derived from the (1 0 3 0 0)0 vibrational state. The 4νCH manifold of C2H2 is congested and affected by anharmonic, l-resonance, and Coriolis couplings that cause other IR-dark, UV-bright rovibrational levels to attain appreciable IR−UV DR intensity and to add to the complexity of intramolecular dynamics in that manifold. Consequently, collision-induced rovibrational satellites observed by IR−UV DR comprise not only regular even-ΔJ features but also supposedly forbidden odd-ΔJ features, of which the energy-transfer channel from J = 12 to J = 1 is particularly efficient. This paper focuses on low-J rovibrational levels of the 4νCH manifold, particularly those with J = 0 and J = 1 in view of their anomalously large Stark effects that are likely to make them susceptible to collision-induced rovibrational mixing. Three complementary forms of IR−UV DR experiment are reported:  IR-scanned, UV-scanned, and kinetic. These indicate that strong IR−UV DR signals observed by probing the (1 0 3 0 0)0 J = 0 rovibrational level are complicated by underlying IR-dark, UV-bright states, making J = 0 unsuitable for systematic IR−UV DR studies. The (1 0 3 0 0)0 J = 1 rovibrational level is more amenable to unambiguous characterization and yields insight concerning even- and odd-ΔJ collision-induced rovibrational energy transfer and associated mechanisms.</abstract><pub>American Chemical Society</pub><doi>10.1021/jp035224t</doi><tpages>12</tpages></addata></record>
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title Rovibrational Energy Transfer in the 4νCH Manifold of Acetylene, Viewed by IR−UV Double Resonance Spectroscopy. 1. Foundation Studies at Low J
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