H2O vibration: Difference between revisions

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*INCAR
*INCAR
  SYSTEM = H2O vibration
  SYSTEM = H2O vibration
PREC = A
# IBRION = 1 ; NSW = 10 ; NFREE = 2 ; EDIFFG = -1E-4
ENMAX = 400
  ISMEAR = 0    # Gaussian smearing
  ISMEAR = 0    # Gaussian smearing
  IBRION = 6    # finite differences with symmetry
  IBRION = 6    # finite differences with symmetry
  NFREE = 2    # central differences (default)
  NFREE = 2    # central differences (default)
  POTIM = 0.015 # default as well
  POTIM = 0.015 # default as well
  EDIFF = 1E-6
  EDIFF = 1E-8
  NSW = 1      # ionic steps > 0
  NSW = 1      # ionic steps > 0


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*POSCAR
*POSCAR
  H2O _2                                                                           
  H2O _2                                                                           
  0.5291800
1.0000000
   15.0000000  0.0000000  0.0000000
   8.0000000  0.0000000  0.0000000
    0.0000000 15.0000000  0.0000000
  0.0000000   8.0000000  0.0000000
    0.0000000  0.0000000 15.0000000
  0.0000000  0.0000000   8.0000000
    1    2
    1    2
cart
cart
    0.0000000  0.0000000  0.0000000
  0.0000000  0.0000000  0.0000000
    1.1269567 13.5477107   0.0000000
  0.5960812 -0.7677068   0.0000000
    1.1269567   1.4522893   0.0000000
  0.5960812   0.7677068   0.0000000


How many zero frequency modes are observed and why?  
How many zero frequency modes should be observed and why?  
Are the results sensitive to the step width {{TAG|POTIM}}
Try to use the linear response code ({{TAG|IBRION}}=8 and {{TAG|EDIFF}}=1E-8) to obtain
Also try to use the linear response code ({{TAG|IBRION}}=8).
reference results.
For finite differences, are the results sensitive to the step width {{TAG|POTIM}}.
In this specific case, errors are too large at the default
cutoff (drift in forces), and it is simplest to increase the
cutoff {{TAG|ENCUT}} to 600 eV. The important and physically meaningful
frequencies are however insensitive to the choice of the cutoff.


== Download ==
== Download ==

Revision as of 12:48, 6 June 2012

  • INCAR
SYSTEM = H2O vibration
PREC = A
  1. IBRION = 1 ; NSW = 10 ; NFREE = 2 ; EDIFFG = -1E-4
ENMAX = 400
ISMEAR = 0    # Gaussian smearing
IBRION = 6    # finite differences with symmetry
NFREE = 2     # central differences (default)
POTIM = 0.015 # default as well
EDIFF = 1E-8 
NSW = 1       # ionic steps > 0
  • KPOINTS
Gamma-point only
 1        ! one k-point
rec       ! in units of the reciprocal lattice vector
 0 0 0 1  ! 3 coordinates and weight
  • POSCAR
H2O _2                                                                          
1.0000000
  8.0000000   0.0000000   0.0000000
  0.0000000   8.0000000   0.0000000
  0.0000000   0.0000000   8.0000000
   1    2

cart

  0.0000000   0.0000000   0.0000000
  0.5960812  -0.7677068   0.0000000
  0.5960812   0.7677068   0.0000000

How many zero frequency modes should be observed and why? Try to use the linear response code (IBRION=8 and EDIFF=1E-8) to obtain reference results. For finite differences, are the results sensitive to the step width POTIM. In this specific case, errors are too large at the default cutoff (drift in forces), and it is simplest to increase the cutoff ENCUT to 600 eV. The important and physically meaningful frequencies are however insensitive to the choice of the cutoff.

Download

1_8_H2Ovib.tgz


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