Difference between revisions of "Ct2ist.m"

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     [states,coeffs]=ct2ist(mult,type)
 
     [states,coeffs]=ct2ist(mult,type)
  
==Arguments==
+
==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#Elementary_operators|Elementary operators]]
+
[[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