1988
DOI: 10.1016/0167-7977(88)90011-1
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Computer graphical and semiclassical approaches to molecular rotations and vibrations

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Cited by 97 publications
(65 citation statements)
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“…(25) for the state S y . The energy of the unstable stationary state S x corresponds to the top of the barrier responsible for the inversion doublets (K-doublets) in the upper and lower parts of the J-multiplets [3]. Another barrier appears because of the bifurcation for angular momentum at J > J c .…”
Section: Precessional and Vibrational Motions Of An Rotating Ab 2 Molmentioning
confidence: 99%
See 1 more Smart Citation
“…(25) for the state S y . The energy of the unstable stationary state S x corresponds to the top of the barrier responsible for the inversion doublets (K-doublets) in the upper and lower parts of the J-multiplets [3]. Another barrier appears because of the bifurcation for angular momentum at J > J c .…”
Section: Precessional and Vibrational Motions Of An Rotating Ab 2 Molmentioning
confidence: 99%
“…Energy level clustering in molecules is very interesting phenomenon, which has been studied for about twenty years [1,2,3,4]. However the main interest was concentrated on highly symmetrical molecules like tetrahydrides.…”
Section: Introductionmentioning
confidence: 99%
“…They introduced the classical rotational energy surface (CRES) which proved to be very helpful in understanding the qualitative features of RV spectra of such molecules [6,7]. The results presented in Table I and discussed When higher excitations are taken into account some new phenomena, generally connected with the RV coupling, perturb the clear picture presented above.…”
Section: Rotational Levels For J > 20mentioning
confidence: 86%
“…The large number of classical and semiclassical investigations [6][7][8][9][10][11][12] is a consequence of the fact that, in contrast to the traditional quantum methods, classical mechanics provides means for gathering information about the approximate dynamics in high-J regimes.…”
Section: J Pykamentioning
confidence: 99%
“…Of particular importance are the integrable cases of the rigid body problem [9,10], which include the free asymmetric top (Euler top) [1,4,6], the symmetric top in a uniform external gravitational field (Lagrange top) [6,11], and the Kovalevskaya top [6,12]. The theory of rigid body motion also provides the basis for analysis and interpretation of the rotational dynamics and spectra of semi-rigid molecules [2,5,13,14,15,16]. In molecular terms the Euler top is simply a free asymmetric top molecule [5,14,15], the Lagrange top models a symmetric top molecule with a dipole moment in an electric field [15,17], while there does not appear to be an obvious molecular analogue for the Kovalevskaya top.…”
Section: Introductionmentioning
confidence: 99%