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Double resonance spectroscopy of phenol(H2O)1–12: evidence for ice-like structures in aromate–water clusters?

Identifieur interne : 000612 ( Main/Corpus ); précédent : 000611; suivant : 000613

Double resonance spectroscopy of phenol(H2O)1–12: evidence for ice-like structures in aromate–water clusters?

Auteurs : W. Roth ; M. Schmitt ; Ch Jacoby ; D. Spangenberg ; Ch Janzen ; K. Kleinermanns

Source :

RBID : ISTEX:41032207D1E61185EFD713A1308C79320D9C4B67

Abstract

Phenol(H2O)n clusters have been studied in the electronic ground state by dispersed fluorescence spectroscopy and in the electronically excited state by means of two-color resonant two-photon ionization (R2PI), spectral hole burning and rotationally resolved laser-induced fluorescence. Resonant spectra up to a cluster size of n=12 have been obtained by two-color R2PI under `soft' ionization conditions. The analysis of spectral shifts and of the intermolecular vibrations in both electronic states is used to assign structures for these bi-, tri- and (partially) tetracoordinated hydrogen bonded systems, which may be comparable to H-bond-deficient water structures at the surface of liquid water and ice.

Url:
DOI: 10.1016/S0301-0104(98)00252-3

Links to Exploration step

ISTEX:41032207D1E61185EFD713A1308C79320D9C4B67

Le document en format XML

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<note type="content">Fig. 1: Part of HRLIF of phenol(H2O)1. The upper trace shows a portion of 50 GHz, with the origin at 35996.47 cm−1 (0 at the scale of the figure). The central part of this spectrum is expanded to 14 GHz in the second trace. The last two traces show the simulation for the two torsional components together with the rotational constants used in the fit of the spectrum.</note>
<note type="content">Fig. 2: The lower trace shows the R2PI spectrum of phenol(H2O)1, the solid line represents the SHB spectrum upon analysis of the (+) component at 126 cm−1, the dashed trace the SHB spectrum upon analysis of the (−) component at 121 cm−1.</note>
<note type="content">Fig. 3: Hole burning spectra of phenol(H2O)2–5. The arrows indicate the analysis positions and the insets show the calculated minimum energy structures.</note>
<note type="content">Fig. 4: DF spectra of phenol(H2O)3–5 between the electronic origin and 230 cm−1. Accuracy of the band positions is ±1 cm−1.</note>
<note type="content">Fig. 5: Two-color R2PI spectra of phenol(H2O)5–8,12. The dashed lines connecting neighbored mass traces show the fragmentation paths. None of the stronger n=8 transitions could be traced back to fragmentation of n≥9 clusters upon ionization with 355 nm. The inset shows two tentative structures of phenol(H2O)8.</note>
<note type="content">Table 1: Intermolecular vibrational frequencies of the phenol–water cluster in the S1 state</note>
<note type="content">Table 2: Assigned intermolecular fundamental vibrations of phenol(H2O)2–5</note>
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<affiliation>Heinrich-Heine-Universität Düsseldorf, Institut für Physikalische Chemie und Elektrochemie I, D-40225 Düsseldorf, Germany</affiliation>
<description>Present address: Institut für Lasermedizin, Heinrich-Heine-Universität, Düsseldorf.</description>
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<namePart type="family">Spangenberg</namePart>
<affiliation>Heinrich-Heine-Universität Düsseldorf, Institut für Physikalische Chemie und Elektrochemie I, D-40225 Düsseldorf, Germany</affiliation>
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<namePart type="family">Janzen</namePart>
<affiliation>Heinrich-Heine-Universität Düsseldorf, Institut für Physikalische Chemie und Elektrochemie I, D-40225 Düsseldorf, Germany</affiliation>
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<roleTerm type="text">author</roleTerm>
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<namePart type="given">K</namePart>
<namePart type="family">Kleinermanns</namePart>
<affiliation>Heinrich-Heine-Universität Düsseldorf, Institut für Physikalische Chemie und Elektrochemie I, D-40225 Düsseldorf, Germany</affiliation>
<description>Corresponding author. Fax: +49-211-81-15195.</description>
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<publisher>ELSEVIER</publisher>
<dateIssued encoding="w3cdtf">1997</dateIssued>
<dateCaptured encoding="w3cdtf">1997-11-10</dateCaptured>
<copyrightDate encoding="w3cdtf">1998</copyrightDate>
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<languageTerm type="code" authority="iso639-2b">eng</languageTerm>
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<abstract lang="en">Phenol(H2O)n clusters have been studied in the electronic ground state by dispersed fluorescence spectroscopy and in the electronically excited state by means of two-color resonant two-photon ionization (R2PI), spectral hole burning and rotationally resolved laser-induced fluorescence. Resonant spectra up to a cluster size of n=12 have been obtained by two-color R2PI under `soft' ionization conditions. The analysis of spectral shifts and of the intermolecular vibrations in both electronic states is used to assign structures for these bi-, tri- and (partially) tetracoordinated hydrogen bonded systems, which may be comparable to H-bond-deficient water structures at the surface of liquid water and ice.</abstract>
<note type="content">Fig. 1: Part of HRLIF of phenol(H2O)1. The upper trace shows a portion of 50 GHz, with the origin at 35996.47 cm−1 (0 at the scale of the figure). The central part of this spectrum is expanded to 14 GHz in the second trace. The last two traces show the simulation for the two torsional components together with the rotational constants used in the fit of the spectrum.</note>
<note type="content">Fig. 2: The lower trace shows the R2PI spectrum of phenol(H2O)1, the solid line represents the SHB spectrum upon analysis of the (+) component at 126 cm−1, the dashed trace the SHB spectrum upon analysis of the (−) component at 121 cm−1.</note>
<note type="content">Fig. 3: Hole burning spectra of phenol(H2O)2–5. The arrows indicate the analysis positions and the insets show the calculated minimum energy structures.</note>
<note type="content">Fig. 4: DF spectra of phenol(H2O)3–5 between the electronic origin and 230 cm−1. Accuracy of the band positions is ±1 cm−1.</note>
<note type="content">Fig. 5: Two-color R2PI spectra of phenol(H2O)5–8,12. The dashed lines connecting neighbored mass traces show the fragmentation paths. None of the stronger n=8 transitions could be traced back to fragmentation of n≥9 clusters upon ionization with 355 nm. The inset shows two tentative structures of phenol(H2O)8.</note>
<note type="content">Table 1: Intermolecular vibrational frequencies of the phenol–water cluster in the S1 state</note>
<note type="content">Table 2: Assigned intermolecular fundamental vibrations of phenol(H2O)2–5</note>
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<titleInfo>
<title>Chemical Physics</title>
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<titleInfo type="abbreviated">
<title>CHEMPH</title>
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<genre type="Journal">journal</genre>
<originInfo>
<dateIssued encoding="w3cdtf">19981215</dateIssued>
</originInfo>
<identifier type="ISSN">0301-0104</identifier>
<identifier type="PII">S0301-0104(00)X0096-1</identifier>
<part>
<date>19981215</date>
<detail type="volume">
<number>239</number>
<caption>vol.</caption>
</detail>
<detail type="issue">
<number>1–3</number>
<caption>no.</caption>
</detail>
<extent unit="issue pages">
<start>1</start>
<end>622</end>
</extent>
<extent unit="pages">
<start>1</start>
<end>9</end>
</extent>
</part>
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<identifier type="istex">41032207D1E61185EFD713A1308C79320D9C4B67</identifier>
<identifier type="DOI">10.1016/S0301-0104(98)00252-3</identifier>
<identifier type="PII">S0301-0104(98)00252-3</identifier>
<accessCondition type="use and reproduction" contentType="">© 1998Elsevier Science B.V.</accessCondition>
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<recordOrigin>Elsevier Science B.V., ©1998</recordOrigin>
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