Difference between revisions of "Lin2lm.m"
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[L,M]=lin2lm(I) | [L,M]=lin2lm(I) | ||
| − | == | + | ==Parameters== |
I - linear indices of spin states, with | I - linear indices of spin states, with | ||
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==See also== | ==See also== | ||
| − | [[lm2lin.m]], [[lin2lmn.m]], [[lmn2lin.m]], [[irr_sph_ten.m]] | + | [[lm2lin.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 linear indexing of spin states into L,M 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:
I=0 -> (L=0,M=0)
I=1 -> (L=1,M=1)
I=2 -> (L=1,M=0), et cetera...
Syntax
[L,M]=lin2lm(I)
Parameters
I - linear indices of spin states, with
I=0 corresponding to L=0, M=0.
Outputs
L - ranks of the spin states
M - projections of the spin states
Notes
See the state indexing section for further information about how Spinach enumerates spherical tensor states.
See also
lm2lin.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