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- W1980520234 abstract "Two cylindrical tensor-form asymmetric rotator Hamiltonians are in general use. In one form, the operators are constructed as sums of Hermitian combinations of products of integral powers of the angular momentum operators P 2 , P c 2 , and ( P a 2 − P b 2 ), where P 2 = P a 2 + P b 2 + P c 2 . In the other form one uses integral powers of P 2 and P c 2 along with ( P + 2 n + P − 2 n ), n = 1, 2, 3, …, where P + = P a + iP b and P − = P a − iP b . Relations are developed between the operators occurring in the two formulations in order to facilitate comparison of empirical constants based on one or the other of the two formulations, especially when octic and higher-power angular momentum operators are included in the analysis." @default.
- W1980520234 created "2016-06-24" @default.
- W1980520234 creator A5091831940 @default.
- W1980520234 date "1985-02-01" @default.
- W1980520234 modified "2023-09-26" @default.
- W1980520234 title "Relating angular momentum operators in cylindrical tensor form asymmetric rotator Hamiltonians" @default.
- W1980520234 cites W2013265407 @default.
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- W1980520234 doi "https://doi.org/10.1016/0022-2852(85)90319-4" @default.
- W1980520234 hasPublicationYear "1985" @default.
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