Difference between revisions of "Orientation.m"
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==See also== | ==See also== | ||
| − | [[hamiltonian.m]], [[operator.m]], [[wigner.m]], [[irr_sph_ten.m]] | + | [[hamiltonian.m]], [[operator.m]], [[wigner.m]], [[irr_sph_ten.m]], [[bos2ist.m]], [[boson_mono.m]], [[boson_ortho.m]], [[centrans.m]], [[ct2ist.m]], [[enlev2bm.m]], [[enlev2ist.m]], [[kinetics.m]], [[lindbladian.m]], [[oper2bm.m]], [[oper2ist.m]], [[propagator.m]], [[relaxation.m]], [[sin_tran.m]], [[weyl.m]], [[Kernel_functions]] |
''Version 2.2, authors: [[Ilya Kuprov]]'' | ''Version 2.2, authors: [[Ilya Kuprov]]'' | ||
Latest revision as of 19:39, 6 June 2026
Anisotropic part of the Hamiltonian for a specific spin system orientation.
Syntax
H=orientation(Q,euler_angles)
Parameters
Q - rotational basis as returned by
hamiltonian.m function
euler_angles - a 1x3 vector specifying Euler
angles (radians) relative to the
input orientation
Outputs
H - anisotropic part of the Hamiltonian
for the specified Euler angles
Notes
This function may be used in both Hilbert and Liouville space because the H -> [H, ] adjoint map is linear.
See also
hamiltonian.m, operator.m, wigner.m, irr_sph_ten.m, bos2ist.m, boson_mono.m, boson_ortho.m, centrans.m, ct2ist.m, enlev2bm.m, enlev2ist.m, kinetics.m, lindbladian.m, oper2bm.m, oper2ist.m, propagator.m, relaxation.m, sin_tran.m, weyl.m, Kernel_functions
Version 2.2, authors: Ilya Kuprov