6533b834fe1ef96bd129cc1f
RESEARCH PRODUCT
Analogue of oscillation theorem for nonadiabatic diatomic states: application to the A 1Σ+ and b 3Π states of KCs
M. TamanisAndrey V. StolyarovVladimir I. PupyshevRuvin FerberE. A. Pazyuksubject
PhysicsOscillationQuantum mechanicsOperator (physics)Degenerate energy levelsGeneral Physics and AstronomyState (functional analysis)Physical and Theoretical ChemistryEigenfunctionAdiabatic processWave functionDiatomic moleculedescription
Relative intensity measurements in the high resolution A (1)Sigma(+) approximately b (3)Pi--X (1)Sigma(+) laser induced fluorescence spectra of the KCs molecule highlighted a breakdown of the conventional one-dimensional oscillation theorem (L. D. Landau and E. M. Lifshitz, Quantum Mechanics, Pergamon, New York, 1965). For strongly spin-orbit coupled A (1)Sigma(+) and b (3)Pi states the number of nodes n(A) and n(b) of the non-adiabatic vibrational eigenfunctions phi and phi corresponding to the v-th eigenstate differs essentially from their adiabatic counterparts. It is found, however, that in the general case of two-component states with wavefunctions phi and phi coupled by the sign-constant potential operator V(12) not equal 0: (1) the lowest state v = 0 is not degenerate; and (2) the arithmetic mean of the number of nodes n(1) and n(2) of phi and phi never exceeds the ordering number v of eigenstate: (n(1) + n(2))/2or=v.
year | journal | country | edition | language |
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2010-04-30 | Physical Chemistry Chemical Physics |