Difference between revisions of "Geffect.m"

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{{DISPLAYTITLE:geffect.m}} __NOTOC__
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{{DISPLAYTITLE:geffect.m}}
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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==
  
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g=geffect(spin_system,states)
+
    g=geffect(spin_system,states)
 +
 
 +
==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.
  
 
==Arguments==
 
==Arguments==
  
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states - the numbers of the states to use
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    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)
  
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==Outputs==
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==Returns==
  
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g      - 3x3 g-tensor matrix in Bohr mag-
+
    g      - 3x3 g-tensor matrix in Bohr mag-
 
             neton units
 
             neton units
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ilya.kuprov@weizmann.ac.il
 
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e.suturina@soton.ac.uk
 
  
 
==Examples==
 
==Examples==
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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==
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[[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]]''
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−
==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 15:48, 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)

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.

Arguments

   states - the numbers of the states to use
            (numbered sequentially from the 
             lowest to the highest energy)

Returns

   g      - 3x3 g-tensor matrix in Bohr mag-
            neton units

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