Difference between revisions of "Twospinist.m"

From Spinach Documentation Wiki
Jump to: navigation, search
(Created page with "{{DISPLAYTITLE:twospinist.m}} __NOTOC__ Two-spin irreducible spherical tensor operators. ==Syntax== T=twospinist(spin_system,spin_a,spin_b,indices,type) ==Arguments==...")
 
(→‎See also)
Line 34: Line 34:
 
==See also==
 
==See also==
 
[[Kernel_utilities#SU.282.29_infrastructure|SU(2) infrastructure]]
 
[[Kernel_utilities#SU.282.29_infrastructure|SU(2) infrastructure]]
 +
 
[[Kernel_utilities#SO.283.29_infrastructure|SO(3) infrastructure]]
 
[[Kernel_utilities#SO.283.29_infrastructure|SO(3) infrastructure]]
 +
 
[[Kernel_utilities#Rotations|Rotations]]
 
[[Kernel_utilities#Rotations|Rotations]]
  
  
 
''Version 2.5, authors: [[Ilya Kuprov]]''
 
''Version 2.5, authors: [[Ilya Kuprov]]''

Revision as of 14:30, 18 September 2020

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

SU(2) infrastructure

SO(3) infrastructure

Rotations


Version 2.5, authors: Ilya Kuprov