Difference between revisions of "Ct2ist.m"
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[states,coeffs]=ct2ist(mult,type) | [states,coeffs]=ct2ist(mult,type) | ||
| − | == | + | ==Parameters== |
mult - multipicity of the spin in question, an | mult - multipicity of the spin in question, an | ||
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==See also== | ==See also== | ||
| − | [[Kernel_functions | + | [[bos2ist.m]], [[boson_mono.m]], [[boson_ortho.m]], [[centrans.m]], [[enlev2bm.m]], [[enlev2ist.m]], [[hamiltonian.m]], [[kinetics.m]], [[lindbladian.m]], [[oper2bm.m]], [[oper2ist.m]], [[operator.m]], [[orientation.m]], [[propagator.m]], [[relaxation.m]], [[sin_tran.m]], [[weyl.m]], [[Kernel_functions]] |
''Version 2.9, authors: [[Ilya Kuprov]]'' | ''Version 2.9, authors: [[Ilya Kuprov]]'' | ||
Latest revision as of 19:35, 6 June 2026
Irreducible spherical tensor expansion of central transition operators of half-integer spins.
Syntax
[states,coeffs]=ct2ist(mult,type)
Parameters
mult - multipicity of the spin in question, an
even positive integer
type - operator type: 'z' for polarisation, '+'
for raising, '-' for lowering
Outputs
states - states, in the Spinach IST basis index-
ing, that contribute to the operator in
question; use lin2lm to convert to L,M
spherical tensor indices
coeffs - coefficients with which the ISTs enter
the linear combination
Notes
Central transition refers to the Zeeman basis.
See also
bos2ist.m, boson_mono.m, boson_ortho.m, centrans.m, enlev2bm.m, enlev2ist.m, hamiltonian.m, kinetics.m, lindbladian.m, oper2bm.m, oper2ist.m, operator.m, orientation.m, propagator.m, relaxation.m, sin_tran.m, weyl.m, Kernel_functions
Version 2.9, authors: Ilya Kuprov