Difference between revisions of "Twospinist.m"

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==See also==
 
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[[Kernel_utilities#SU.282.29_infrastructure|SU(2) infrastructure]]
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[[Kernel_utilities#Rotations|Rotations]]
  
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[[Kernel_utilities#SO.283.29_infrastructure|SO(3) infrastructure]]
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[[Kernel_utilities#SU.282.29.2C_SO.283.29.2C_and_other_groups|SU(2), SO(3), and other groups]]
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[[Kernel_utilities#Rotations|Rotations]]
 
  
  
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''Version 2.5, authors: [[Ilya Kuprov]]''
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''Version 2.8, authors: [[Ilya Kuprov]]''

Revision as of 09:57, 25 July 2023

Two-spin irreducible spherical tensor operators.

Syntax

    T=twospinist(spin_system,spin_a,spin_b,indices,type)

Arguments

    spin_a   - number of the first spin

    spin_b   - number of the second spin

    indices  - two-element vector [L,M] containing
               rank and projection index; L=1,2 are
               available

In Liouville space, type can be set to:

   'left' - produces left side product superoperator

   'right' - produces right side product superoperator

   'comm' - produces commutation superoperator (default)

   'acomm' - produces anticommutation superoperator

In Hilbert space calculations, the type parameter is ignored, and the operator itself is always returned.

Outputs

    T  - irreducible spherical tensor operator

See also

Rotations

SU(2), SO(3), and other groups


Version 2.8, authors: Ilya Kuprov