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Spinor: spin magnetization density
Show the COSMO surface as used in a Cosmo calculation. Only accessible for .t21 files that contain COSMO results.
Only accessible in case of a spin-orbit coupled calculation with a TAPE21 (.t21) file
to visualize a spinor.
Visualization of spinors is more difficult than visualization of orbitals.
A spinor Ψ is a two-component complex wave function, which can be described
with four real functions φ: real part α φαR,
imaginary part α φαI,
real part β φβR,
imaginary part β φβI:
| Ψ = ( |
φαR + i φαI
φβR + i φβI
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)
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The density ρ is:
ρ = Ψ† Ψ
The spin magnetization density m is:
m = Ψ† σ Ψ
where σ is the vector of the Pauli spin matrices
σx, σy, and σz.
A spinor is fully determined by the spin magnetization density and a phase factor eiθ,
which both are functions of spatial coordinates.
The (square root of the) density and spin magnetization density are visualized as a double isosurface and
a vector field respectively.
The phase factor eiθ, reduced to a plus or minus sign, is visualized with the double isosurface
and with the color of the vector field.
The main control bar is identical to the control bar of a normal isosurface. If you show the details,
you will find that in addition to the controls available for a normal isosurface,
you can also specify coloring information. In this case, the two numbers for the HSV colors define the
colors of the minus and plus sign.
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