Difference between revisions of "Lm2lin.m"
m (Rename Arguments section heading to Parameters) |
(Update function See also links and function index membership) |
||
| Line 25: | Line 25: | ||
==See also== | ==See also== | ||
| − | [[lin2lm.m]], [[lin2lmn.m]], [[lmn2lin.m]], [[irr_sph_ten.m]] | + | [[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]]'' | ''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