Difference between revisions of "Orientation.m"

From Spinach Documentation Wiki
Jump to: navigation, search
m (Rename Arguments section heading to Parameters)
(Update function See also links and function index membership)
 
Line 24: Line 24:
  
 
==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