Doppler-free two-photon excitation spectroscopy and the Zeeman effects. Perturbations in the 14(0)1 and 1(0)(1)14(0)1 bands of the S1 <-- S0 transition of C6D6
Doppler-free two-photon excitation spectra and the Zeeman effects for the 1 band of the S1 1B2u
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Veröffentlicht in: | The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 2005-08, Vol.109 (32), p.7127-7133 |
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container_title | The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory |
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creator | Baek, Dae Youl Wang, Jinguo Doi, Atsushi Kasahara, Shunji Katô, Hajime Baba, Masaaki |
description | Doppler-free two-photon excitation spectra and the Zeeman effects for the 1 band of the S1 1B2u |
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Perturbations in the 14(0)1 and 1(0)(1)14(0)1 bands of the S1 <-- S0 transition of C6D6</title><source>ACS Publications</source><creator>Baek, Dae Youl ; Wang, Jinguo ; Doi, Atsushi ; Kasahara, Shunji ; Katô, Hajime ; Baba, Masaaki</creator><creatorcontrib>Baek, Dae Youl ; Wang, Jinguo ; Doi, Atsushi ; Kasahara, Shunji ; Katô, Hajime ; Baba, Masaaki</creatorcontrib><description>Doppler-free two-photon excitation spectra and the Zeeman effects for the 1 band of the S1 1B2u <-- S0 1A1g transition in gaseous benzene-d6 were measured. Although the spectral lines were strongly perturbed, almost all of the lines near the band origin could be assigned. From a deperturbation analysis, the perturbation near the band origin was identified as originating from an anharmonic resonance interaction. Perturbation centered at K = 28-29 in the 14(0)1 band was analyzed, and it was identified as originating from a perpendicular Coriolis interaction. The symmetry and the assignment of the perturbing state proposed by Schubert et al. (Schubert, U.; Riedle, E.; Neusser, H. J. J. Chem. Phys. 1989, 90, 5994.) were confirmed. No perturbation originating from an interaction with a triplet state was observed in both bands. From the Zeeman spectra and the analysis, it is demonstrated that rotationally resolved levels are not mixed with a triplet state. The intersystem mixing is not likely to occur at levels of low excess energy in the S1 state of an isolated benzene. Nonradiative decay of an isolated benzene in the low vibronic levels of the S1 state will occur through the internal mixing followed by the rotational and vibrational relaxation in the S0 state.</description><identifier>ISSN: 1089-5639</identifier><identifier>PMID: 16834076</identifier><language>eng</language><publisher>United States</publisher><ispartof>The journal of physical chemistry. 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Perturbations in the 14(0)1 and 1(0)(1)14(0)1 bands of the S1 <-- S0 transition of C6D6</title><title>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory</title><addtitle>J Phys Chem A</addtitle><description>Doppler-free two-photon excitation spectra and the Zeeman effects for the 1 band of the S1 1B2u <-- S0 1A1g transition in gaseous benzene-d6 were measured. Although the spectral lines were strongly perturbed, almost all of the lines near the band origin could be assigned. From a deperturbation analysis, the perturbation near the band origin was identified as originating from an anharmonic resonance interaction. Perturbation centered at K = 28-29 in the 14(0)1 band was analyzed, and it was identified as originating from a perpendicular Coriolis interaction. The symmetry and the assignment of the perturbing state proposed by Schubert et al. (Schubert, U.; Riedle, E.; Neusser, H. J. J. Chem. Phys. 1989, 90, 5994.) were confirmed. No perturbation originating from an interaction with a triplet state was observed in both bands. From the Zeeman spectra and the analysis, it is demonstrated that rotationally resolved levels are not mixed with a triplet state. The intersystem mixing is not likely to occur at levels of low excess energy in the S1 state of an isolated benzene. Nonradiative decay of an isolated benzene in the low vibronic levels of the S1 state will occur through the internal mixing followed by the rotational and vibrational relaxation in the S0 state.</description><issn>1089-5639</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNo1kM1OwzAQhHMA0VJ4BeQTKgcju_6JI3FBLX9SJZDaE5fIdjZqUBIH2xX0aXhVrFBOO5r5Zlfak2xKiSqwkKyYZOchfBBCKFvws2xCpWKc5HKa_azcMLTgce0BUPxyeNi56HoE37aJOjZJhgFs9C5YNxyQ7isUd4DeATqdsLpOYbhFb-Dj3puxEVDTjxDlc3JDxw5Nak5vjo5JVkCuHqkNRXcYow1B0es-NOPRlC3lSl5kp7VuA1we5yzbPj5sl894_fr0srxf40FwiY0wChi3ZkEVABCZF0RZKwpW0EpwC8ZIyAXVQtMciAApalsscsGVqZRgbJZd_60dvPvcQ4hl1wQLbat7cPtQ5iS9rOAqgVdHcG86qMrBN532h_L_o-wXpDNuQA</recordid><startdate>20050818</startdate><enddate>20050818</enddate><creator>Baek, Dae Youl</creator><creator>Wang, Jinguo</creator><creator>Doi, Atsushi</creator><creator>Kasahara, Shunji</creator><creator>Katô, Hajime</creator><creator>Baba, Masaaki</creator><scope>NPM</scope><scope>7X8</scope></search><sort><creationdate>20050818</creationdate><title>Doppler-free two-photon excitation spectroscopy and the Zeeman effects. Perturbations in the 14(0)1 and 1(0)(1)14(0)1 bands of the S1 <-- S0 transition of C6D6</title><author>Baek, Dae Youl ; Wang, Jinguo ; Doi, Atsushi ; Kasahara, Shunji ; Katô, Hajime ; Baba, Masaaki</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p546-b5b8e34cb218eee067908cc59391d54cebb6e751a5a17e05e65fc927548bd8533</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Baek, Dae Youl</creatorcontrib><creatorcontrib>Wang, Jinguo</creatorcontrib><creatorcontrib>Doi, Atsushi</creatorcontrib><creatorcontrib>Kasahara, Shunji</creatorcontrib><creatorcontrib>Katô, Hajime</creatorcontrib><creatorcontrib>Baba, Masaaki</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Baek, Dae Youl</au><au>Wang, Jinguo</au><au>Doi, Atsushi</au><au>Kasahara, Shunji</au><au>Katô, Hajime</au><au>Baba, Masaaki</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Doppler-free two-photon excitation spectroscopy and the Zeeman effects. Perturbations in the 14(0)1 and 1(0)(1)14(0)1 bands of the S1 <-- S0 transition of C6D6</atitle><jtitle>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory</jtitle><addtitle>J Phys Chem A</addtitle><date>2005-08-18</date><risdate>2005</risdate><volume>109</volume><issue>32</issue><spage>7127</spage><epage>7133</epage><pages>7127-7133</pages><issn>1089-5639</issn><abstract>Doppler-free two-photon excitation spectra and the Zeeman effects for the 1 band of the S1 1B2u <-- S0 1A1g transition in gaseous benzene-d6 were measured. Although the spectral lines were strongly perturbed, almost all of the lines near the band origin could be assigned. From a deperturbation analysis, the perturbation near the band origin was identified as originating from an anharmonic resonance interaction. Perturbation centered at K = 28-29 in the 14(0)1 band was analyzed, and it was identified as originating from a perpendicular Coriolis interaction. The symmetry and the assignment of the perturbing state proposed by Schubert et al. (Schubert, U.; Riedle, E.; Neusser, H. J. J. Chem. Phys. 1989, 90, 5994.) were confirmed. No perturbation originating from an interaction with a triplet state was observed in both bands. From the Zeeman spectra and the analysis, it is demonstrated that rotationally resolved levels are not mixed with a triplet state. The intersystem mixing is not likely to occur at levels of low excess energy in the S1 state of an isolated benzene. Nonradiative decay of an isolated benzene in the low vibronic levels of the S1 state will occur through the internal mixing followed by the rotational and vibrational relaxation in the S0 state.</abstract><cop>United States</cop><pmid>16834076</pmid><tpages>7</tpages></addata></record> |
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title | Doppler-free two-photon excitation spectroscopy and the Zeeman effects. Perturbations in the 14(0)1 and 1(0)(1)14(0)1 bands of the S1 <-- S0 transition of C6D6 |
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