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Nuclear Spin Selective Torsional States: Implications of Molecular Symmetry

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dc.contributor.author Belz, S.
dc.contributor.author Deeb, O.
dc.contributor.author Gonzalez, L.
dc.contributor.author Grohmann, T.
dc.contributor.author Kinzel, D.
dc.contributor.author Leibscher, M.
dc.contributor.author Manz, J.
dc.contributor.author Obaid, R.
dc.contributor.author Oppel, M.
dc.date.accessioned 2021-05-26T09:44:58Z
dc.date.accessioned 2022-05-22T08:55:31Z
dc.date.available 2021-05-26T09:44:58Z
dc.date.available 2022-05-22T08:55:31Z
dc.date.issued 2013-04-22
dc.identifier.uri http://localhost:8080/xmlui/handle/123456789/8358
dc.description.abstract We consider a class of molecules with C2 symmetry axis and three segments A, B, C which can rotate independently about that axis, corresponding to two independent torsions (B vs. A and C vs. B). The torsions may be feasible either in the electronic ground or in the excited states. We determine the corresponding molecular symmetry group, i.e. the Abelian group GA 16 representing 16 feasible permutations and permutation-inversions, and its permutation subgroup with eight permutations, together with their properties, e.g. their character tables and the corresponding 16 or 8 irreducible representations (IREPs), respectively. Accordingly, the molecules which belong to this class have at most eight different nuclear spin isomers (NSIs). A subset of them “survives” at low temperature, T → 0. The corresponding NSI selective wavefunctions contain products of torsional times nuclear wavefunctions with specific IREPs. The NSIs are characterized by these IREPs. As an example, we determine the molecular symmetry adapted torsional wavefunctions of the model 2-[4- (cyclopenta-2,4-dien-1-ylidene)cyclohexa-2,5-dien-1-ylidene]-2H-1,3-dioxole, abbreviated as CCD. In order to demonstrate the principles of the derivations, we employ a simple model, with the C2 symmetry axis oriented along the laboratory Z-axis, and with all degrees of freedom frozen in the equilibrium structure of CCD, except the two torsional degrees of freedom. The resulting torsional wavefunctions represent different NSIs of CCD, ready for subsequent applications, e.g. for demonstrations of NSI selective dynamics. en_US
dc.language.iso en en_US
dc.subject Nuclear Spin Isomers / Molecular Torsion / Molecular Rotors / Molecular Symmetry / Group Theory / Quantum Chemistry / en_US
dc.title Nuclear Spin Selective Torsional States: Implications of Molecular Symmetry en_US
dc.type Article en_US


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