1984
DOI: 10.1016/0022-2852(84)90086-9
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The effects of vibration-rotation interaction on the quadrupole hyperfine structure of molecular rotational levels

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Cited by 42 publications
(14 citation statements)
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“…The quadrupole coupling Hamiltonian W used here is the equivalent operator arising when only ∆J = 0 matrix elements are sought (Hougen & Oka 1981;Aliev & Hougen 1984): where α and β run over the molecule-fixed coordinates x, y, z, the symbol e denotes the electronic charge, Q is the nuclear quadrupole moment, q αβ is the electric field gradient tensor, J α are components of the rotational angular momentum J, and…”
Section: Hyperfine-coupling Hamiltonian and Energiesmentioning
confidence: 99%
“…The quadrupole coupling Hamiltonian W used here is the equivalent operator arising when only ∆J = 0 matrix elements are sought (Hougen & Oka 1981;Aliev & Hougen 1984): where α and β run over the molecule-fixed coordinates x, y, z, the symbol e denotes the electronic charge, Q is the nuclear quadrupole moment, q αβ is the electric field gradient tensor, J α are components of the rotational angular momentum J, and…”
Section: Hyperfine-coupling Hamiltonian and Energiesmentioning
confidence: 99%
“…(2) of Ref. [9], eQ is the quadrupole moment of a nitrogen atom; b, c run over the molecule-fixed coordinates x, y, z, the J b are components of the rotational angular momentum, q 3 b;c ðn 1 ; n 2 Þ and q 6 b;c ðn 1 ; n 2 Þ are components of the electric field gradient tensor at nitrogen atoms N 3 and N 6 , respectively, and F(I j , J) is an operator corresponding to the Casimir function. The field gradients depend on the two large amplitude coordinates n 1 and n 2 .…”
Section: Hyperfine Hamiltonianmentioning
confidence: 99%
“…Nonvanishing matrix elements of the rovibrational operators in Eq. (9) between such eigenfunctions are the following:…”
Section: Rovibrational-hyperfine Hamiltonian Matrixmentioning
confidence: 99%
“…The only limitation to be made is to consider the Hamiltonian of the quadrupole coupling diagonal in the quantum number J. In this case, the effective Hamiltonian for the vibrational state v t = 1 of an oblate symmetric top molecule with C 3v symmetry, including rovibrational and quadrupole interactions up to third order, can be written as (4,5) …”
Section: Theorymentioning
confidence: 99%