Structures and IR/UV spectra of neutral and ionic phenol-Ar-n cluster isomers (n <= 4): competition between hydrogen bonding and stacking

dc.contributor.authorSchmies, Matthias
dc.contributor.authorPatzer, Alexander
dc.contributor.authorFujii, Masaaki
dc.contributor.authorDopfer, Otto
dc.date.accessioned2016-07-01T06:27:32Z
dc.date.available2016-07-01T06:27:32Z
dc.date.issued2011
dc.descriptionDieser Beitrag ist mit Zustimmung des Rechteinhabers aufgrund einer (DFG geförderten) Allianz- bzw. Nationallizenz frei zugänglich.de
dc.descriptionThis publication is with permission of the rights owner freely accessible due to an Alliance licence and a national licence (funded by the DFG, German Research Foundation) respectively.en
dc.description.abstractThe structures, binding energies, and vibrational and electronic spectra of various isomers of neutral and ionic phenol–Arnclusters with n ≤ 4, PhOH(+)–Arn, are characterized by quantum chemical calculations. The properties in the neutral and ionic ground electronic states (S0, D0) are determined at the M06-2X/aug-cc-pVTZ level, whereas the S1 excited state of the neutral species is investigated at the CC2/aug-cc-pVDZ level. The Ar complexation shifts calculated for the S1 origin and the adiabatic ionisation potential, ΔS1 and ΔIP, sensitively depend on the Ar positions and thus the sequence of filling the first Ar solvation shell. The calculated shifts confirm empirical additivity rules for ΔS1 established recently from experimental spectra and enable thus a firm assignment of various S1 origins to their respective isomers. A similar additivity model is newly developed for ΔIP using the M06-2X data. The isomer assignment is further confirmed by Franck–Condon simulations of the intermolecular vibrational structure of the S1 ← S0 transitions. In neutral PhOH–Arn, dispersion dominates the attraction and π-bonding is more stable than H-bonding. The solvation sequence of the most stable isomers is derived as (10), (11), (30), and (31) for n ≤ 4, where (km) denotes isomers with k and m Ar ligands binding above and below the aromatic plane, respectively. The π interaction is somewhat stronger in the S1 state due to enhanced dispersion forces. Similarly, the H-bond strength increases in S1 due to the enhanced acidity of the OH proton. In the PhOH+–Arn cations, H-bonds are significantly stronger than π-bonds due to additional induction forces. Consequently, one favourable solvation sequence is derived as (H00), (H10), (H20), and (H30) for n ≤ 4, where (Hkm) denotes isomers with one H-bound ligand and k and m π-bonded Ar ligands above and below the aromatic plane, respectively. Another low-energy solvation motif for n = 2 is denoted (11)H and involves nonlinear bifurcated H-bonding to both equivalent Ar atoms in a C2v structure in which the OH group points toward the midpoint of an Ar2 dimer in a T-shaped fashion. This dimer core can also be further solvated by π-bonded ligands leading to the solvation sequence (H00), (11)H, (21)H, and (22) for n ≤ 4. The implications of the ionisation-induced π → H switch in the preferred interaction motif on the isomerisation and fragmentation processes of PhOH(+)–Arn are discussed in the light of the new structural and energetic cluster parameters.en
dc.identifier.eissn1463-9084
dc.identifier.issn1463-9076
dc.identifier.pmid21597606
dc.identifier.urihttp://depositonce.tu-berlin.de/handle/11303/5751
dc.identifier.urihttp://dx.doi.org/10.14279/depositonce-5371
dc.language.isoen
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/en
dc.subject.ddc540 Chemie und zugeordnete Wissenschaftende
dc.titleStructures and IR/UV spectra of neutral and ionic phenol-Ar-n cluster isomers (n <= 4): competition between hydrogen bonding and stackingen
dc.typeArticleen
dc.type.versionpublishedVersionen
dcterms.bibliographicCitation.doi10.1039/c1cp20676a
dcterms.bibliographicCitation.issue31
dcterms.bibliographicCitation.journaltitlePhysical chemistry, chemical physicsen
dcterms.bibliographicCitation.originalpublishernameRoyal Society of Chemistryde
dcterms.bibliographicCitation.originalpublisherplaceCambridgede
dcterms.bibliographicCitation.pageend13941
dcterms.bibliographicCitation.pagestart13926
dcterms.bibliographicCitation.volume13
tub.accessrights.dnbdomain
tub.affiliationFak. 2 Mathematik und Naturwissenschaften>Inst. Optik und Atomare Physikde
tub.affiliation.facultyFak. 2 Mathematik und Naturwissenschaftende
tub.affiliation.instituteInst. Optik und Atomare Physikde
tub.publisher.universityorinstitutionTechnische Universität Berlin
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