Difference between revisions of "Geffect.m"
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| − | {{DISPLAYTITLE:geffect.m}} | + | {{DISPLAYTITLE:geffect.m}} __NOTOC__ |
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Effective g-tensor for the user-specified Kramers doublet, computed as described in http://dx.doi.org/10.1063/1.4793736 | Effective g-tensor for the user-specified Kramers doublet, computed as described in http://dx.doi.org/10.1063/1.4793736 | ||
==Syntax== | ==Syntax== | ||
| − | + | g=geffect(spin_system,states) | |
| − | |||
| − | |||
| − | |||
==Arguments== | ==Arguments== | ||
| − | + | states - the numbers of the states to use | |
(numbered sequentially from the | (numbered sequentially from the | ||
lowest to the highest energy) | lowest to the highest energy) | ||
| − | == | + | ==Outputs== |
| − | + | g - 3x3 g-tensor matrix in Bohr mag- | |
neton units | neton units | ||
| + | |||
| + | ilya.kuprov@weizmann.ac.il | ||
| + | e.suturina@soton.ac.uk | ||
==Examples== | ==Examples== | ||
| + | |||
See dy_lft_single.m file in examples/giant_spin folder of Spinach distribution. | See dy_lft_single.m file in examples/giant_spin folder of Spinach distribution. | ||
==Notes== | ==Notes== | ||
| + | |||
Make sure that the pair of levels specified actually is a Kramers doublet. | Make sure that the pair of levels specified actually is a Kramers doublet. | ||
==See also== | ==See also== | ||
| + | |||
[[chi_eff.m]], [[eqmag.m]], [[lpcs.m]], [[kpcs.m]], [[ppcs.m]] | [[chi_eff.m]], [[eqmag.m]], [[lpcs.m]], [[kpcs.m]], [[ppcs.m]] | ||
''Version 2.2, authors: [[Elizaveta Suturina]], [[Ilya Kuprov]]'' | ''Version 2.2, authors: [[Elizaveta Suturina]], [[Ilya Kuprov]]'' | ||
| + | |||
| + | ==Description== | ||
| + | |||
| + | Lanthanide systems often have multiple pairs of energy levels that are related to one another by a spin flip. These are called Kramers doublets. This function returns the effective g-tensor for the user-specified pair of levels. | ||
| + | |||
| + | ==Returns== | ||
| + | |||
| + | g - 3x3 g-tensor matrix in Bohr mag- | ||
| + | neton units | ||
Revision as of 15:05, 5 April 2026
Effective g-tensor for the user-specified Kramers doublet, computed as described in http://dx.doi.org/10.1063/1.4793736
Syntax
g=geffect(spin_system,states)
Arguments
states - the numbers of the states to use
(numbered sequentially from the
lowest to the highest energy)
Outputs
g - 3x3 g-tensor matrix in Bohr mag-
neton units
ilya.kuprov@weizmann.ac.il e.suturina@soton.ac.uk
Examples
See dy_lft_single.m file in examples/giant_spin folder of Spinach distribution.
Notes
Make sure that the pair of levels specified actually is a Kramers doublet.
See also
chi_eff.m, eqmag.m, lpcs.m, kpcs.m, ppcs.m
Version 2.2, authors: Elizaveta Suturina, Ilya Kuprov
Description
Lanthanide systems often have multiple pairs of energy levels that are related to one another by a spin flip. These are called Kramers doublets. This function returns the effective g-tensor for the user-specified pair of levels.
Returns
g - 3x3 g-tensor matrix in Bohr mag-
neton units
