Vibronic structure of TiO+ from multiphoton ionization photoelectron spectroscopy
We apply the techniques of resonance enhanced multiphoton ionization (REMPI) and time-of-flight photoelectron spectroscopy (TOF-PES) to TiO molecules cooled in a pulsed nozzle expansion to obtain vibronic spectra of gas phase TiO+. The adiabatic first ionization energy is refined to I1(TiO)=54 999±5...
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Veröffentlicht in: | The Journal of chemical physics 1989-02, Vol.90 (3), p.1415-1428 |
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creator | SAPPEY, A. D EIDEN, G HARRINGTON, J. E WEISSHAAR, J. C |
description | We apply the techniques of resonance enhanced multiphoton ionization (REMPI) and time-of-flight photoelectron spectroscopy (TOF-PES) to TiO molecules cooled in a pulsed nozzle expansion to obtain vibronic spectra of gas phase TiO+. The adiabatic first ionization energy is refined to I1(TiO)=54 999±52 cm−1=6.819±0.006 eV, which yields D0(Ti+–0) =159.9±2.2 kcal/mol. For the X 2Δ state of TiO+, we resolve spin–orbit pairs of vibrational levels for v=0–14, yielding ωe=1045±7 cm−1 and ωexe =4±1 cm−1. The spin–orbit splitting ΔEso =210±6 cm−1 permits confirmation of the state symmetry by comparison with the known spin–orbit splittings of the X 3Δ state of TiO. We also observe a new excited B 2∑+ state at T0=11 227±17 cm−1 with ωe =1020±9 cm−1 and ωexe =6±2 cm−1. This state is distinct from the A 2∑+ state (average frequency 860±60 cm−1) previously observed by Dyke and co-workers. From components of certain PESs apparently due to one or more metastable states of TiO, we infer the existence of a previously unobserved state of neutral TiO at T0=2980 cm−1, possibly the 3∑− state. Finally, we discuss the electronic structure and vibrational frequencies of TiO, TiO+, and other third row metal oxides from both molecular orbital and ligand field points of view in order to understand the ordering of electronic states and certain trends in vibrational frequencies. The molecular orbital model readily explains why nominally isoelectronic neutral and cationic metal oxides, such as TiO+ and ScO, are electronically quite dissimilar. |
doi_str_mv | 10.1063/1.456083 |
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D ; EIDEN, G ; HARRINGTON, J. E ; WEISSHAAR, J. C</creator><creatorcontrib>SAPPEY, A. D ; EIDEN, G ; HARRINGTON, J. E ; WEISSHAAR, J. C</creatorcontrib><description>We apply the techniques of resonance enhanced multiphoton ionization (REMPI) and time-of-flight photoelectron spectroscopy (TOF-PES) to TiO molecules cooled in a pulsed nozzle expansion to obtain vibronic spectra of gas phase TiO+. The adiabatic first ionization energy is refined to I1(TiO)=54 999±52 cm−1=6.819±0.006 eV, which yields D0(Ti+–0) =159.9±2.2 kcal/mol. For the X 2Δ state of TiO+, we resolve spin–orbit pairs of vibrational levels for v=0–14, yielding ωe=1045±7 cm−1 and ωexe =4±1 cm−1. The spin–orbit splitting ΔEso =210±6 cm−1 permits confirmation of the state symmetry by comparison with the known spin–orbit splittings of the X 3Δ state of TiO. We also observe a new excited B 2∑+ state at T0=11 227±17 cm−1 with ωe =1020±9 cm−1 and ωexe =6±2 cm−1. This state is distinct from the A 2∑+ state (average frequency 860±60 cm−1) previously observed by Dyke and co-workers. From components of certain PESs apparently due to one or more metastable states of TiO, we infer the existence of a previously unobserved state of neutral TiO at T0=2980 cm−1, possibly the 3∑− state. Finally, we discuss the electronic structure and vibrational frequencies of TiO, TiO+, and other third row metal oxides from both molecular orbital and ligand field points of view in order to understand the ordering of electronic states and certain trends in vibrational frequencies. The molecular orbital model readily explains why nominally isoelectronic neutral and cationic metal oxides, such as TiO+ and ScO, are electronically quite dissimilar.</description><identifier>ISSN: 0021-9606</identifier><identifier>EISSN: 1089-7690</identifier><identifier>DOI: 10.1063/1.456083</identifier><identifier>CODEN: JCPSA6</identifier><language>eng</language><publisher>Woodbury, NY: American Institute of Physics</publisher><subject>Atomic and molecular physics ; Exact sciences and technology ; Molecular properties and interactions with photons ; Photon interactions with molecules ; Physics</subject><ispartof>The Journal of chemical physics, 1989-02, Vol.90 (3), p.1415-1428</ispartof><rights>1990 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c320t-8ce0e266bc877c24ec25d02fe6680c71a013d665140dc93011bfc3c8952ccff53</citedby><cites>FETCH-LOGICAL-c320t-8ce0e266bc877c24ec25d02fe6680c71a013d665140dc93011bfc3c8952ccff53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=6638688$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>SAPPEY, A. D</creatorcontrib><creatorcontrib>EIDEN, G</creatorcontrib><creatorcontrib>HARRINGTON, J. E</creatorcontrib><creatorcontrib>WEISSHAAR, J. C</creatorcontrib><title>Vibronic structure of TiO+ from multiphoton ionization photoelectron spectroscopy</title><title>The Journal of chemical physics</title><description>We apply the techniques of resonance enhanced multiphoton ionization (REMPI) and time-of-flight photoelectron spectroscopy (TOF-PES) to TiO molecules cooled in a pulsed nozzle expansion to obtain vibronic spectra of gas phase TiO+. The adiabatic first ionization energy is refined to I1(TiO)=54 999±52 cm−1=6.819±0.006 eV, which yields D0(Ti+–0) =159.9±2.2 kcal/mol. For the X 2Δ state of TiO+, we resolve spin–orbit pairs of vibrational levels for v=0–14, yielding ωe=1045±7 cm−1 and ωexe =4±1 cm−1. The spin–orbit splitting ΔEso =210±6 cm−1 permits confirmation of the state symmetry by comparison with the known spin–orbit splittings of the X 3Δ state of TiO. We also observe a new excited B 2∑+ state at T0=11 227±17 cm−1 with ωe =1020±9 cm−1 and ωexe =6±2 cm−1. This state is distinct from the A 2∑+ state (average frequency 860±60 cm−1) previously observed by Dyke and co-workers. From components of certain PESs apparently due to one or more metastable states of TiO, we infer the existence of a previously unobserved state of neutral TiO at T0=2980 cm−1, possibly the 3∑− state. Finally, we discuss the electronic structure and vibrational frequencies of TiO, TiO+, and other third row metal oxides from both molecular orbital and ligand field points of view in order to understand the ordering of electronic states and certain trends in vibrational frequencies. The molecular orbital model readily explains why nominally isoelectronic neutral and cationic metal oxides, such as TiO+ and ScO, are electronically quite dissimilar.</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>0021-9606</issn><issn>1089-7690</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1989</creationdate><recordtype>article</recordtype><recordid>eNo9kEtLAzEUhYMoWKvgT8jChSBTb5KZO5mlFF9QKEJ1O6S3CUbmRZJZ1F_v2Iqrc7h851w4jF0LWAhAdS8WeYGg1QmbCdBVVmIFp2wGIEVWIeA5u4jxCwBEKfMZe_vw29B3nnhMYaQ0Bst7xzd-fcdd6Fvejk3yw2ef-o77Cfw2aRJ-uNjGUprSPA4HE6kf9pfszJkm2qs_nbP3p8fN8iVbrZ9flw-rjJSElGmyYCXilnRZkswtyWIH0llEDVQKA0LtEAuRw44qBUJsHSnSVSGJnCvUnN0ee2l6HIN19RB8a8K-FlD_TlGL-jjFhN4c0cFEMo0LpiMf_3lEpVFr9QPxFF6v</recordid><startdate>19890201</startdate><enddate>19890201</enddate><creator>SAPPEY, A. D</creator><creator>EIDEN, G</creator><creator>HARRINGTON, J. E</creator><creator>WEISSHAAR, J. C</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19890201</creationdate><title>Vibronic structure of TiO+ from multiphoton ionization photoelectron spectroscopy</title><author>SAPPEY, A. D ; EIDEN, G ; HARRINGTON, J. E ; WEISSHAAR, J. C</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c320t-8ce0e266bc877c24ec25d02fe6680c71a013d665140dc93011bfc3c8952ccff53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1989</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>SAPPEY, A. D</creatorcontrib><creatorcontrib>EIDEN, G</creatorcontrib><creatorcontrib>HARRINGTON, J. E</creatorcontrib><creatorcontrib>WEISSHAAR, J. C</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>The Journal of chemical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>SAPPEY, A. D</au><au>EIDEN, G</au><au>HARRINGTON, J. E</au><au>WEISSHAAR, J. C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Vibronic structure of TiO+ from multiphoton ionization photoelectron spectroscopy</atitle><jtitle>The Journal of chemical physics</jtitle><date>1989-02-01</date><risdate>1989</risdate><volume>90</volume><issue>3</issue><spage>1415</spage><epage>1428</epage><pages>1415-1428</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><coden>JCPSA6</coden><abstract>We apply the techniques of resonance enhanced multiphoton ionization (REMPI) and time-of-flight photoelectron spectroscopy (TOF-PES) to TiO molecules cooled in a pulsed nozzle expansion to obtain vibronic spectra of gas phase TiO+. The adiabatic first ionization energy is refined to I1(TiO)=54 999±52 cm−1=6.819±0.006 eV, which yields D0(Ti+–0) =159.9±2.2 kcal/mol. For the X 2Δ state of TiO+, we resolve spin–orbit pairs of vibrational levels for v=0–14, yielding ωe=1045±7 cm−1 and ωexe =4±1 cm−1. The spin–orbit splitting ΔEso =210±6 cm−1 permits confirmation of the state symmetry by comparison with the known spin–orbit splittings of the X 3Δ state of TiO. We also observe a new excited B 2∑+ state at T0=11 227±17 cm−1 with ωe =1020±9 cm−1 and ωexe =6±2 cm−1. This state is distinct from the A 2∑+ state (average frequency 860±60 cm−1) previously observed by Dyke and co-workers. From components of certain PESs apparently due to one or more metastable states of TiO, we infer the existence of a previously unobserved state of neutral TiO at T0=2980 cm−1, possibly the 3∑− state. Finally, we discuss the electronic structure and vibrational frequencies of TiO, TiO+, and other third row metal oxides from both molecular orbital and ligand field points of view in order to understand the ordering of electronic states and certain trends in vibrational frequencies. The molecular orbital model readily explains why nominally isoelectronic neutral and cationic metal oxides, such as TiO+ and ScO, are electronically quite dissimilar.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.456083</doi><tpages>14</tpages></addata></record> |
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subjects | Atomic and molecular physics Exact sciences and technology Molecular properties and interactions with photons Photon interactions with molecules Physics |
title | Vibronic structure of TiO+ from multiphoton ionization photoelectron spectroscopy |
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