Difference between revisions of "Sphten2zeeman.m"
m (Rename Arguments section heading to Parameters) |
(sync with Spinach main f053e432: note refers to the projector, not the matrix) |
||
| (One intermediate revision by the same user not shown) | |||
| Line 19: | Line 19: | ||
==Notes== | ==Notes== | ||
| − | The | + | The projector need not be square and may be huge. |
==See also== | ==See also== | ||
| − | [[pauli.m]], [[irr_sph_ten.m]] | + | [[pauli.m]], [[irr_sph_ten.m]], [[adelim.m]], [[coherence.m]], [[correlation.m]], [[dfpt.m]], [[homospoil.m]], [[human2opspec.m]], [[lin2lm.m]], [[lin2lmn.m]], [[lm2lin.m]], [[lmn2lin.m]], [[path_trace.m]], [[scomponents.m]], [[sinkhole.m]], [[sparse2csr.m]], [[stitch.m]], [[zte.m]], [[Kernel_utilities]] |
| − | |||
| − | [[Kernel_utilities | ||
''Version 2.9, authors: [[Ilya Kuprov]]'' | ''Version 2.9, authors: [[Ilya Kuprov]]'' | ||
Latest revision as of 08:39, 30 August 2026
Basis set conversion from irreducible spherical tensors into Zeeman basis. Returns a matrix that converts state vectors written in the spherical tensor basis set used by Spinach into state vectors written in the Zeeman basis set in Liouville space.
Syntax
P=sphten2zeeman(spin_system)
Parameters
spin_system - main Spinach data structure using sphten-liouv
formalism and including basis set information
Outputs
P - projector matrix that is to be used in the fol-
lowing way:
rho_zeeman=P*rho_sphten
Notes
The projector need not be square and may be huge.
See also
pauli.m, irr_sph_ten.m, adelim.m, coherence.m, correlation.m, dfpt.m, homospoil.m, human2opspec.m, lin2lm.m, lin2lmn.m, lm2lin.m, lmn2lin.m, path_trace.m, scomponents.m, sinkhole.m, sparse2csr.m, stitch.m, zte.m, Kernel_utilities
Version 2.9, authors: Ilya Kuprov
