Difference between revisions of "Gtensorof.m"
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==See also== | ==See also== | ||
| − | [[spin.m]], [[isnucleus.m]], [[xyz2dd.m]] | + | [[spin.m]], [[isnucleus.m]], [[xyz2dd.m]], [[chemshifts.m]], [[cubic_lattice.m]], [[dilute.m]], [[get_coupling.m]], [[idxof.m]], [[iselectron.m]], [[isoswap.m]], [[kill_spin.m]], [[nearest_spin.m]], [[shift_iso.m]], [[Kernel_utilities]] |
''Version 2.1, authors: [[Ilya Kuprov]], [[Elizaveta Suturina]]'' | ''Version 2.1, authors: [[Ilya Kuprov]], [[Elizaveta Suturina]]'' | ||
Latest revision as of 19:37, 6 June 2026
Returns the g-tensor of the specified spin at the input orientation; input-stage Zeeman interaction specifications may vary, but the returned tensor is always in Bohr magneton units.
Syntax
g=gtensorof(spin_system,spin_number)
Parameters
spin_number - a positive integer specifying the number
of the spin in the sys.isotopes list
Outputs
g - a 3x3 matrix in Bohr magneton units
Notes
The same convention (mu=-mu_b*g*S/hbar) is used for the nuclei, meaning that their g-tensors are much smaller than those of electrons.
See also
spin.m, isnucleus.m, xyz2dd.m, chemshifts.m, cubic_lattice.m, dilute.m, get_coupling.m, idxof.m, iselectron.m, isoswap.m, kill_spin.m, nearest_spin.m, shift_iso.m, Kernel_utilities
Version 2.1, authors: Ilya Kuprov, Elizaveta Suturina