The ν 3 − ν 4 difference band contribution to the CCl 4 symmetric stretch (ν 1 ) mode
The Raman spectrum of the symmetric stretching vibration (ν 1 ) of liquid carbon tetrachloride observed at 295 K and reported repeatedly over the last 80 years clearly shows four of the five more abundant isotopomers at 440–470 cm −1 . At the lower energy end of this spectrum, additional intensity d...
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Veröffentlicht in: | Journal of Raman spectroscopy 2015-01, Vol.46 (1), p.189-193 |
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creator | Gaynor, James D. Wetterer, Anna M. Valente, Edward J. Mayer, Steven G. |
description | The Raman spectrum of the symmetric stretching vibration (ν
1
) of liquid carbon tetrachloride observed at 295 K and reported repeatedly over the last 80 years clearly shows four of the five more abundant isotopomers at 440–470 cm
−1
. At the lower energy end of this spectrum, additional intensity due to isotopomeric contributions from the symmetric stretch for v = 1 → 2 (hotbands) partially overlaps the prominent v = 0 → 1 features, and accounts for about 18% of the integrated intensity at 295 K in agreement with theory. When these two patterns are modeled and subtracted from the experimental spectrum, a feature underlying almost exactly the C
35
Cl
4
(v = 0 → 1) band at 462.5 cm
−1
becomes apparent. We propose that this feature is the ν
3
− ν
4
difference band. Observations at lower temperatures, and of the combination bands, and the polarized Raman spectra are consistent with this hypothesis. Copyright © 2014 John Wiley & Sons, Ltd. |
doi_str_mv | 10.1002/jrs.4625 |
format | Article |
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1
) of liquid carbon tetrachloride observed at 295 K and reported repeatedly over the last 80 years clearly shows four of the five more abundant isotopomers at 440–470 cm
−1
. At the lower energy end of this spectrum, additional intensity due to isotopomeric contributions from the symmetric stretch for v = 1 → 2 (hotbands) partially overlaps the prominent v = 0 → 1 features, and accounts for about 18% of the integrated intensity at 295 K in agreement with theory. When these two patterns are modeled and subtracted from the experimental spectrum, a feature underlying almost exactly the C
35
Cl
4
(v = 0 → 1) band at 462.5 cm
−1
becomes apparent. We propose that this feature is the ν
3
− ν
4
difference band. Observations at lower temperatures, and of the combination bands, and the polarized Raman spectra are consistent with this hypothesis. Copyright © 2014 John Wiley & Sons, Ltd.</description><identifier>ISSN: 0377-0486</identifier><identifier>EISSN: 1097-4555</identifier><identifier>DOI: 10.1002/jrs.4625</identifier><language>eng</language><ispartof>Journal of Raman spectroscopy, 2015-01, Vol.46 (1), p.189-193</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c725-bb33f87360cbfca1aa35b2cfc9086405b37c783bd17718343052e44d360ee2303</citedby><cites>FETCH-LOGICAL-c725-bb33f87360cbfca1aa35b2cfc9086405b37c783bd17718343052e44d360ee2303</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></links><search><creatorcontrib>Gaynor, James D.</creatorcontrib><creatorcontrib>Wetterer, Anna M.</creatorcontrib><creatorcontrib>Valente, Edward J.</creatorcontrib><creatorcontrib>Mayer, Steven G.</creatorcontrib><title>The ν 3 − ν 4 difference band contribution to the CCl 4 symmetric stretch (ν 1 ) mode</title><title>Journal of Raman spectroscopy</title><description>The Raman spectrum of the symmetric stretching vibration (ν
1
) of liquid carbon tetrachloride observed at 295 K and reported repeatedly over the last 80 years clearly shows four of the five more abundant isotopomers at 440–470 cm
−1
. At the lower energy end of this spectrum, additional intensity due to isotopomeric contributions from the symmetric stretch for v = 1 → 2 (hotbands) partially overlaps the prominent v = 0 → 1 features, and accounts for about 18% of the integrated intensity at 295 K in agreement with theory. When these two patterns are modeled and subtracted from the experimental spectrum, a feature underlying almost exactly the C
35
Cl
4
(v = 0 → 1) band at 462.5 cm
−1
becomes apparent. We propose that this feature is the ν
3
− ν
4
difference band. Observations at lower temperatures, and of the combination bands, and the polarized Raman spectra are consistent with this hypothesis. Copyright © 2014 John Wiley & Sons, Ltd.</description><issn>0377-0486</issn><issn>1097-4555</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNotkLtOwzAUhi0EEqEg8Qgey5By7GPHyYgiblIlluxR7NhqqiZBthm6McLK-_AKPESfBFewnF9H_2X4CLlmsGIA_Hbrw0oUXJ6QjEGlciGlPCUZoFI5iLI4JxchbAGgqgqWkbbZWPrzTZEe3j8PH1_ppk_QfnDOejsZS3U39dTMU_SDfovDPNE405hqdb1LybAfR5s8Q0P0NpoNXaYFRm_oOPf2kpy5bhfs1b8uSPNw39RP-frl8bm-W-dGcZlrjehKhQUY7UzHug6l5saZCspCgNSojCpR90wpVqJAkNwK0aeCtRwBF2T5N2v8HIK3rn31w9j5fcugPXJpE5f2yAV_AR6eWDw</recordid><startdate>201501</startdate><enddate>201501</enddate><creator>Gaynor, James D.</creator><creator>Wetterer, Anna M.</creator><creator>Valente, Edward J.</creator><creator>Mayer, Steven G.</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>201501</creationdate><title>The ν 3 − ν 4 difference band contribution to the CCl 4 symmetric stretch (ν 1 ) mode</title><author>Gaynor, James D. ; Wetterer, Anna M. ; Valente, Edward J. ; Mayer, Steven G.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c725-bb33f87360cbfca1aa35b2cfc9086405b37c783bd17718343052e44d360ee2303</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gaynor, James D.</creatorcontrib><creatorcontrib>Wetterer, Anna M.</creatorcontrib><creatorcontrib>Valente, Edward J.</creatorcontrib><creatorcontrib>Mayer, Steven G.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of Raman spectroscopy</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gaynor, James D.</au><au>Wetterer, Anna M.</au><au>Valente, Edward J.</au><au>Mayer, Steven G.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The ν 3 − ν 4 difference band contribution to the CCl 4 symmetric stretch (ν 1 ) mode</atitle><jtitle>Journal of Raman spectroscopy</jtitle><date>2015-01</date><risdate>2015</risdate><volume>46</volume><issue>1</issue><spage>189</spage><epage>193</epage><pages>189-193</pages><issn>0377-0486</issn><eissn>1097-4555</eissn><abstract>The Raman spectrum of the symmetric stretching vibration (ν
1
) of liquid carbon tetrachloride observed at 295 K and reported repeatedly over the last 80 years clearly shows four of the five more abundant isotopomers at 440–470 cm
−1
. At the lower energy end of this spectrum, additional intensity due to isotopomeric contributions from the symmetric stretch for v = 1 → 2 (hotbands) partially overlaps the prominent v = 0 → 1 features, and accounts for about 18% of the integrated intensity at 295 K in agreement with theory. When these two patterns are modeled and subtracted from the experimental spectrum, a feature underlying almost exactly the C
35
Cl
4
(v = 0 → 1) band at 462.5 cm
−1
becomes apparent. We propose that this feature is the ν
3
− ν
4
difference band. Observations at lower temperatures, and of the combination bands, and the polarized Raman spectra are consistent with this hypothesis. Copyright © 2014 John Wiley & Sons, Ltd.</abstract><doi>10.1002/jrs.4625</doi><tpages>5</tpages></addata></record> |
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title | The ν 3 − ν 4 difference band contribution to the CCl 4 symmetric stretch (ν 1 ) mode |
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