Difference between revisions of "Lm2lin.m"

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(Update function See also links and function index membership)
 
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     I=lm2lin(L,M)
 
     I=lm2lin(L,M)
  
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==Arguments==
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==Parameters==
  
 
     L  - ranks of the spin states
 
     L  - ranks of the spin states
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==See also==
 
==See also==
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[[lin2lm.m]], [[lin2lmn.m]], [[lmn2lin.m]], [[irr_sph_ten.m]]
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[[lin2lm.m]], [[lin2lmn.m]], [[lmn2lin.m]], [[irr_sph_ten.m]], [[adelim.m]], [[coherence.m]], [[correlation.m]], [[dfpt.m]], [[homospoil.m]], [[human2opspec.m]], [[path_trace.m]], [[scomponents.m]], [[sinkhole.m]], [[sparse2csr.m]], [[sphten2zeeman.m]], [[stitch.m]], [[zte.m]], [[Kernel_utilities]]
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''Version 2.3, authors: [[Ilya Kuprov]]''
 
''Version 2.3, authors: [[Ilya Kuprov]]''

Latest revision as of 19:38, 6 June 2026

Converts L,M indexing of spin states into linear indexing. In the linear indexing convention, spin states are listed in the order of increasing L rank, and, within ranks, in the order of decreasing M projection. Zero base counting is used:

                 (L=0,M=0) -> I=0
                 (L=1,M=1) -> I=1
                 (L=1,M=0) -> I=2, et cetera...

Syntax

    I=lm2lin(L,M)

Parameters

    L   - ranks of the spin states

    M   - projections of the spin states

Outputs

    I   - linear indices of spin states, with
          I=0 corresponding to L=0, M=0.

Notes

See the state indexing section for further information about how Spinach enumerates spherical tensor states.

See also

lin2lm.m, lin2lmn.m, lmn2lin.m, irr_sph_ten.m, adelim.m, coherence.m, correlation.m, dfpt.m, homospoil.m, human2opspec.m, path_trace.m, scomponents.m, sinkhole.m, sparse2csr.m, sphten2zeeman.m, stitch.m, zte.m, Kernel_utilities

Version 2.3, authors: Ilya Kuprov