LEFG

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LEFG = .TRUE. | .FALSE.
Default: LEFG = .FALSE. 

Description: The LEFG computes the electric field gradient (EFG) at positions of the atomic nuclei.


For LEFG=.TRUE., the electric field gradient tensors at the positions of the atomic nuclei are calculated using the method of Petrilli et al. [1].

The EFG tensors are symmetric. The principal components Vii and asymmetry parameter η are printed for each atom. Following convention the principal components Vii are ordered such that:

The asymmetry parameter is defined as . For so-called "quadrupolar nuclei", i.e., nuclei with nuclear spin I>1/2, NMR experiments can access Vzz and η.

To convert the Vzz values into the Cq often encountered in NMR literature, one has to specify the nuclear quadrupole moment by means of the QUAD_EFG-tag.

Mind: Several definitions of are used in the NMR community, ensure that you are comparing between the same definitions in calculation and experiment.
Important: For heavy nuclei inaccuracies are to be expected because of an incomplete treatment of relativistic effects.

Input

A typical INCAR file is given below:

 ENCUT = 400              
 ISMEAR = 0; SIGMA = 0.01 

 EDIFF = 1E-8             
 PREC = Accurate          
 LASPH = .TRUE.           

 LEFG = .TRUE.            
 QUAD_EFG = 0. -696. 20.44 0. 2.860  # Nuclear quadrupolar moments for Pb I N O D
Important: Make sure to replace the QUAD_EFG in the INCAR with the values for the isotopes in your system.

Output

The EFG is listed atom-wise after the SCF cycle has been completed. First, the full 3x3 tensor is printed:

  Electric field gradients (V/A^2)
 ---------------------------------------------------------------------
  ion       V_xx      V_yy      V_zz      V_xy      V_xz      V_yz
 ---------------------------------------------------------------------
    1        -         -         -         -         -         -       

The tensor is then diagonalized and reprinted:

  Electric field gradients after diagonalization (V/A^2)
  (convention: |V_zz| > |V_xx| > |V_yy|)
 ----------------------------------------------------------------------
  ion       V_xx      V_yy      V_zz     asymmetry (V_yy - V_xx)/ V_zz
 ----------------------------------------------------------------------
    1       -         -         -             -         

The corresponding eigenvectors are printed atom-wise. Finally, the quadrupolar parameters are presented, which are commonly reported in NMR experiments.

            NMR quadrupolar parameters

  Cq : quadrupolar parameter    Cq=e*Q*V_zz/h
  eta: asymmetry parameters     (V_yy - V_xx)/ V_zz
  Q  : nuclear electric quadrupole moment in mb (millibarn)
 ----------------------------------------------------------------------
  ion       Cq(MHz)       eta       Q (mb)
 ----------------------------------------------------------------------
    1        -             -         -                      

Related tags and articles

QUAD_EFG

Examples that use this tag

References