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dc.contributor.authorKollipost, Franzen_US
dc.contributor.authorPapendorf, Kimen_US
dc.contributor.authorLee, Yu-Fangen_US
dc.contributor.authorLee, Yuan-Pernen_US
dc.contributor.authorSuhm, Martin A.en_US
dc.date.accessioned2014-12-08T15:36:37Z-
dc.date.available2014-12-08T15:36:37Z-
dc.date.issued2014en_US
dc.identifier.issn1463-9076en_US
dc.identifier.urihttp://hdl.handle.net/11536/24966-
dc.identifier.urihttp://dx.doi.org/10.1039/c4cp01418aen_US
dc.description.abstractThe OH bond of methanol, ethanol and t-butyl alcohol becomes more anharmonic upon hydrogen bonding and the infrared intensity ratio between the overtone and the fundamental transition of the bridging OH stretching mode decreases drastically. FTIR spectroscopy of supersonic slit jet expansions allows to quantify these effects for isolated alcohol dimers, enabling a direct comparison to anharmonic vibrational predictions. The diagonal anharmonicity increase amounts to 15-18%, growing with increasing alkyl substitution. The overtone/fundamental IR intensity ratio, which is on the order of 0.1 or more for isolated alcohols, drops to 0.004-0.001 in the hydrogen-bonded OH group, making overtone detection very challenging. Again, alkyl substitution enhances the intensity suppression. Vibrational second order perturbation theory appears to capture these effects in a semiquantitative way. Harmonic quantum chemistry predictions for the hydrogen bond-induced OH stretching frequency shift (the widely used infrared signature of hydrogen bonding) are insufficient, and diagonal anharmonicity corrections from experiment make the agreement between theory and experiment worse. Inclusion of anharmonic cross terms between hydrogen bond modes and the OH stretching mode is thus essential, as is a high level electronic structure theory. The isolated molecule results are compared to matrix isolation data, complementing earlier studies in N-2 and Ar by the more weakly interacting Ne and p-H-2 matrices. Matrix effects on the hydrogen bond donor vibration are quantified.en_US
dc.language.isoen_USen_US
dc.titleAlcohol dimers - how much diagonal OH anharmonicity?en_US
dc.typeArticleen_US
dc.identifier.doi10.1039/c4cp01418aen_US
dc.identifier.journalPHYSICAL CHEMISTRY CHEMICAL PHYSICSen_US
dc.citation.volume16en_US
dc.citation.issue30en_US
dc.citation.spage15948en_US
dc.citation.epage15956en_US
dc.contributor.department應用化學系zh_TW
dc.contributor.department應用化學系分子科學碩博班zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.contributor.departmentInstitute of Molecular scienceen_US
dc.identifier.wosnumberWOS:000339628400027-
dc.citation.woscount3-
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