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Re: [abinit-forum] negative phonon frequencies at gamma point


Chronological Thread 
  • From: "Aldo Humberto Romero" <aromero@qro.cinvestav.mx>
  • To: forum@abinit.org
  • Cc: forum@abinit.org
  • Subject: Re: [abinit-forum] negative phonon frequencies at gamma point
  • Date: Wed, 9 Sep 2009 07:59:58 -0500 (CDT)
  • Importance: Normal

Dear Sanjeev

what are the stresses?.. this will indicate how well converged
you are.. but just looking at your acell, with only two digits,
probably is not.
I see it is a Zb structure, read about how to choose K points
for those.. just in case... we have done many different Zb and Rs
structures and never encounter a problem as the one you mention

regards

-aldo.


-> Dear ABINIT users,
-> Greetings...
->
-> I want to calculate phonon frequencies of GaP system (semiconductor), the
-> input file, for that i got from abinit/tutorial.
-> when i run this file (input file is given below), i got negative phonon
-> frequencies at gamma point and no LO-TO separation.
->
-> I have also given here, the output after running this input file. please
-> suggest me, where i am wrong? I have seen all earlier posting related with
-> this subject, but i can not resolve this problem.
->
-> kind regards
-> sanjeev
->
->
->
->
-> # Crystalline GaP : computation of the response to homogeneous
->
-> # electric field and atomic displacements, at q=0
->
->
->
->
->
->
->
-> ndtset 3
->
->
->
->
->
-> #Ground state calculation
->
-> kptopt1 1 # Automatic generation of k points, taking
->
-> # into account the symmetry
->
-> tolvrs1 1.0d-20 # SCF stopping criterion
->
-> iscf1 7 # Self-consistent calculation, using algorithm 7
->
->
->
->
->
-> #Response Function calculation : d/dk
->
-> rfelfd2 2 # Activate the calculation of the d/dk
-> perturbation
->
-> rfdir2 1 1 1 # Need to consider the perturbation in the all
-> direction
->
->
->
-> nqpt2 1
->
-> qpt2 0.0 0.0 0.0 # This is a calculation at the Gamma point
->
->
->
->
->
-> getwfk2 -1 # Uses as input the output wf of the previous
-> dataset
->
->
->
->
->
-> kptopt2 2 # Automatic generation of k points,
->
-> # using only the time-reversal symmetry to
-> decrease
->
-> # the size of the k point set.
->
->
->
->
->
-> iscf2 -3 # The d/dk perturbation must be treated
->
-> # in a non-self-consistent way
->
-> tolwfr2 1.0d-22 # Must use tolwfr for non-self-consistent
-> calculations
->
->
->
-> #Response Function calculation : electric field perturbation and phonons
->
-> rfphon3 1 # Activate the calculation of the atomic
-> dispacement perturbations
->
-> rfatpol3 1 2 # All the atoms will be displaced
->
-> rfelfd3 3 # Activate the calculation of the electric
-> field
-> perturbation
->
-> rfdir3 1 1 1 # All directions are selected. However,
-> symmetries
-> will be used to decrease
->
-> # the number of perturbations
->
-> nqpt3 1
->
-> qpt3 0.0 0.0 0.0 # This is a calculation at the Gamma point
->
->
->
->
->
-> getwfk3 -2 # Uses as input wfs the output wfs of the
-> dataset
-> 1
->
-> getddk3 -1 # Uses as input ddk wfs the output of the
-> dataset
-> 2
->
->
->
->
->
-> kptopt3 2 # Automatic generation of k points,
->
-> # using only the time-reversal symmetry to
-> decrease
->
-> # the size of the k point set.
->
-> tolvrs3 1.0d-9
->
-> iscf3 7 # Self-consistent calculation, using algorithm 7
->
->
->
->
->
->
->
->
->
-> #######################################################################
->
-> #Common input variables
->
->
->
->
->
-> #Definition of the unit cell
->
-> acell 3*10.45 # This is equivalent to 10.61 10.61 10.61
->
-> rprim 0.0 0.5 0.5
->
-> 0.5 0.0 0.5
->
-> 0.5 0.5 0.0
->
->
->
->
->
-> #Definition of the atom types
->
-> ntypat 2 # There are two types of atom
->
-> znucl 31 15
->
->
->
->
->
-> #Definition of the atoms
->
-> natom 2 # There are two atoms
->
-> typat 1 2
->
-> xred
->
-> 0.0 0.0 0.0
->
-> 0.25 0.25 0.25
->
->
->
->
->
-> #Gives the number of band, explicitely
->
-> nband 16
->
->
->
->
->
-> #Exchange-correlation functional
->
-> ixc 11
->
-> #Definition of the planewave basis set
->
-> ecut 50.0 # Maximal kinetic energy cut-off, in Hartree
->
->
->
->
->
-> #Definition of the k-point grid
->
-> kptrlatt -4 4 4 # In cartesian coordinates, this grid is simple
-> cubic, and
->
-> 4 -4 4 # actually corresponds to the so-called 8x8x8
-> Monkhorst-Pack grid.
->
-> 4 4 -4
->
-> tsmear 0.04
->
-> occopt 4
->
->
->
->
->
->
->
-> #Definition of the SCF procedure
->
-> nstep 100 # Maximal number of SCF cycles
->
-> diemac 10.0
->
->
............................................................................................
->
-> ouput
->
->
-> Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
->
-> Phonon energies in Hartree :
->
-> -1.028821E-04 -1.028819E-04 -1.028810E-04 1.468314E-03 1.468314E-03
->
-> 1.468314E-03
->
-> Phonon frequencies in cm-1 :
->
-> - -2.258001E+01 -2.257997E+01 -2.257978E+01 3.222577E+02 3.222577E+02
->
-> - 3.222577E+02
->


--

Prof. Aldo Humberto Romero
CINVESTAV-Unidad Queretaro
Libramiento Norponiente 2000
CP 76230, Queretaro, QRO, Mexico
tel: 442 211 9909
fax: 442 211 9938

email: aromero@qro.cinvestav.mx
aldorome@gmail.com
www: qro.cinvestav.mx/~aromero




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