Difference between revisions of "Orientation.m"
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| − | Anisotropic part of the Hamiltonian for a specific spin system | + | {{DISPLAYTITLE:orientation.m}} |
| − | orientation. | + | Anisotropic part of the Hamiltonian for a specific spin system orientation. |
| − | + | ==Syntax== | |
| − | + | H=orientation(Q,euler_angles) | |
| − | Q - | + | ==Arguments== |
| − | + | ||
| − | + | Q - rotational basis as returned by | |
| − | + | hamiltonian.m function | |
| − | |||
| − | euler_angles - a 1x3 vector | + | euler_angles - a 1x3 vector specifying Euler |
| − | + | angles (radians) relative to the | |
| − | + | input orientation | |
| − | + | ==Outputs== | |
| − | H - anisotropic part of the Hamiltonian | + | 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. | 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]] | ||
| − | ''Version | + | ''Version 2.2, authors: [[Ilya Kuprov]]'' |
Revision as of 11:55, 29 August 2018
Anisotropic part of the Hamiltonian for a specific spin system orientation.
Contents
Syntax
H=orientation(Q,euler_angles)
Arguments
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
Version 2.2, authors: Ilya Kuprov
