By V. Aldaya, J. Guerrero, G. Marmo (auth.), Bruno Gruber, Michael Ramek (eds.)
Quantization on a Lie staff: Higher-Order Polarizations; V. Aldaya, etal. A comparability among Algebraic versions of Molecular Spectroscopy; R. Bijker, et al. On Discrete Media, Their interplay varieties and the beginning of Non-Exactness of the digital paintings; E. Binz. The k-Fermions and items Interpolating among Fermions Bosons; M. Daoud, et al. Polynomial cognizance of the Uq(sl(3)) Gel¿fand-(Weyl)-Zetlin foundation and abnormal Irreps at Roots of cohesion; V.K. Dobrev, R. Truini. Nonstandard Deformation U¿q(son): The Imbedding U¿q(son) £sub£ Uq(sln) and Representations; A.M. Gavrilik, et al. Algebraic equipment in Physics;F.Iachello. attainable Origins of Quantum Fluctuations; M. Kanenaga, M.Namiki. actual Equivalence in keeping with Observations and Equivalence by way of unfastened Ultra-Filters in Quantum Mechanics of Non-Standard area; T. Kobayashi. Discrete and non-stop Symmetry through Induction and Duality; P. Kramer, M. Lorente. triggered Representations of the Poincaré crew at the Lattice: Spin half and 1 Case; M. Lorente,P. Kramer. Nonlinear Quantum Mechanics and Locality; W. Lücke, P.Nattermann. sixteen extra Articles. Index.
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In the harmonic limit, the expectation value of the diagonal terms in Eq. (22) leads to the familiar Dunham expansion  % (23) Here di is the degeneracy of the vibration. The tij terms in Eq. (22) give rise to further splittings of the vibrational levels (VI, V2, V3, V4) into its possible sublevels. In the harmonic limit the tij terms have the same interpretation as in . 4) = (0,0°,22 ,0°), (0,0°,0°,22 ) and (0,0°,11,11 ) levels, respectively. Similarly, the 02s and 0 26 terms split the Fl and F2 vibrations belonging to the (0, 11 ,1 1 ,0°) and (0, 11 ,0°,11 ) overtones, respectively.
Symmetries in Science X by V. Aldaya, J. Guerrero, G. Marmo (auth.), Bruno Gruber, Michael Ramek (eds.)