Difference between revisions of "Sphten2zeeman.m"
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| − | Basis set conversion from irreducible spherical tensors into Zeeman basis. | + | 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== | ==Syntax== | ||
P=sphten2zeeman(spin_system) | P=sphten2zeeman(spin_system) | ||
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==Outputs== | ==Outputs== | ||
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==See also== | ==See also== | ||
[[pauli.m]], [[irr_sph_ten.m]] | [[pauli.m]], [[irr_sph_ten.m]] | ||
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| + | [[Kernel_utilities#State_space_indexing_and_manipulation|State space indexing and manipulation]] | ||
| − | ''Version 2. | + | ''Version 2.9, authors: [[Ilya Kuprov]]'' |
Revision as of 10:39, 13 May 2024
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)
Outputs
P - projector matrix that is to be used in the fol-
lowing way:
rho_zeeman=P*rho_sphten
Notes
The matrix need not be square and may be huge.
See also
State space indexing and manipulation
Version 2.9, authors: Ilya Kuprov
