1998
DOI: 10.1006/jmsp.1998.7566
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The Forbidden RotationalQ-Branch of CH3CF3: Torsional Properties and (A1−A2) Splittings

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Cited by 13 publications
(47 citation statements)
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“…By using the form of the zeroth-order torsion-rotation Hamiltonian given in Eq. [3], the Hamiltonian matrix for H T 0 in the PAM basis functions ͉J, k, ; k f ͘ has exactly the same form as that for a IAM Hamiltonian in a IAM basis. This occurs because, for a symmetric top, rotation about the symmetry axis does not affect the moment-of-inertia tensor.…”
Section: Ii1 the Effective Hamiltonianmentioning
confidence: 85%
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“…By using the form of the zeroth-order torsion-rotation Hamiltonian given in Eq. [3], the Hamiltonian matrix for H T 0 in the PAM basis functions ͉J, k, ; k f ͘ has exactly the same form as that for a IAM Hamiltonian in a IAM basis. This occurs because, for a symmetric top, rotation about the symmetry axis does not affect the moment-of-inertia tensor.…”
Section: Ii1 the Effective Hamiltonianmentioning
confidence: 85%
“…A torsion-rotation contact transformation has been used to eliminate terms like J ␣ 2 (1 Ϫ cos 3␣)/2 (4, 13). Finally, a rotational contact transformation has been used to simplify H S (3). In an effort to simplify the notation, no attempt has been made to distinguish the transformed and untransformed Hamiltonian operators.…”
Section: Ii1 the Effective Hamiltonianmentioning
confidence: 99%
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