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- From: Igor Lukacevic <ilukacevic@fizika.unios.hr>
- To: forum@abinit.org
- Subject: [abinit-forum] phonon dispersion in ZrO2
- Date: Tue, 12 Jan 2010 10:21:05 +0100
Dear colleagues, I am having problems in reproducing the phonon dispersions in the rocksalt phase of ZrO2 wrt the results obtained in F. Detraux et al., prl 81, 3297 (1998): 1] I obtain many imaginary frequencies. 2] Acoustic mode(s) go imaginary, while the optical mode is the unstable one. They have been using ecut 30 Ha and ngkpt 3*4, while I used ecut 60 Ha and ngkpt 3*6. Both psuedos have the same number of valence electrons. I'm using abinit 5.8.4p, and I correct the output of mrgdbb (acell and rprim) to be able to use brav=2 option in anaddb. My calcs converge without warnings. I'm sending the inputs and the plot bellow. Could anyone give me a clue why this happens and how to improve my calcs? Thank you all in advance! Yours, Igor Lukacevic ================================== RF phonon input # Crystalline ZrO2 - fluorite - cubic fcc - Fm-3m #225 : computation of the phonon spectrum ndtset 18 #Set 1 : ground state self-consistency getwfk1 0 # Cancel default kptopt1 1 # Automatic generation of k points, taking # into account the symmetry nqpt1 0 # Cancel default tolvrs1 1.0d-18 # SCF stopping criterion (modify default) rfphon1 0 # Cancel default #Q vectors for all datasets #Complete set of symmetry-inequivalent qpt chosen to be commensurate # with kpt mesh so that only one set of GS wave functions is needed. #Generated automatically by running GS calculation with kptopt=1, # nshift=0, shiftk=0 0 0 (to include gamma) and taking output kpt set # file as qpt set. Set nstep=1 so only one iteration runs. nqpt 1 # One qpt for each dataset (only 0 or 1 allowed) # This is the default for all datasets and must # be explicitly turned off for dataset 1. qpt2 0.00000000E+00 0.00000000E+00 0.00000000E+00 qpt3 0.00000000E+00 0.00000000E+00 0.00000000E+00 qpt4 1.66666667E-01 0.00000000E+00 0.00000000E+00 qpt5 3.33333333E-01 0.00000000E+00 0.00000000E+00 qpt6 5.00000000E-01 0.00000000E+00 0.00000000E+00 qpt7 1.66666667E-01 1.66666667E-01 0.00000000E+00 qpt8 3.33333333E-01 1.66666667E-01 0.00000000E+00 qpt9 5.00000000E-01 1.66666667E-01 0.00000000E+00 qpt10 -3.33333333E-01 1.66666667E-01 0.00000000E+00 qpt11 -1.66666667E-01 1.66666667E-01 0.00000000E+00 qpt12 3.33333333E-01 3.33333333E-01 0.00000000E+00 qpt13 5.00000000E-01 3.33333333E-01 0.00000000E+00 qpt14 -3.33333333E-01 3.33333333E-01 0.00000000E+00 qpt15 5.00000000E-01 5.00000000E-01 0.00000000E+00 qpt16 5.00000000E-01 3.33333333E-01 1.66666667E-01 qpt17 -3.33333333E-01 3.33333333E-01 1.66666667E-01 qpt18 -3.33333333E-01 5.00000000E-01 1.66666667E-01 #Set 2 : Response function calculation of d/dk wave function iscf2 -3 # Need this non-self-consistent option for d/dk kptopt2 2 # Modify default to use time-reversal symmetry rfphon2 0 # Cancel default rfelfd2 2 # Calculate d/dk wave function only tolvrs2 0.0 # Cancel default for d/dk tolwfr2 1.0d-22 # Use wave function residual criterion instead #Set 3 : Response function calculation of Q=0 phonons and electric field pert. getddk3 2 # d/dk wave functions from last dataset kptopt3 2 # Modify default to use time-reversal symmetry rfelfd3 3 # Electric-field perturbation response only #Sets 4-17 : Finite-wave-vector phonon calculations (defaults for all datasets) getwfk 1 # Use GS wave functions from dataset1 kptopt 3 # Need full k-point set for finite-Q response rfphon 1 # Do phonon response rfatpol 1 3 # Treat displacements of all atoms rfdir 1 1 1 # Do all directions (symmetry will be used) tolvrs 1.0d-8 # This default is active for sets 3-10 ####################################################################### #Common input variables #Definition of the unit cell acell 3*9.46 angdeg 90 90 90 brvltt -1 spgroup 225 #Definition of the atom types ntypat 2 znucl 40 8 8 #Definition of the atoms natom 3 typat 1 2 2 xred 0.00 0.00 0.00 0.25 0.25 0.25 0.75 0.75 0.75 #Gives the number of band, explicitely (do not take the default) nband 14 #Exchange-correlation functional ixc 3 #Definition of the planewave basis set ecut 60 #Definition of the k-point grid nshiftk 4 shiftk 0.5 0.5 0.5 0.5 0.0 0.0 0.0 0.5 0.0 0.0 0.0 0.5 ngkpt 3*6 #Definition of the SCF procedure iscf 7 # Use Pulay mixing sheme for SCF cycle npulayit 10 # Number of Pulay iterations nnsclo 4 # Number of non-self consistent loops nline 8 # Number of line minimisations diemac 4 ================================== anaddb input !Input file for the anaddb code. Analysis of the SiO2 DDB !Flags ifcflag 1 ! Interatomic force constant flag !Wavevector grid number 1 (coarse grid, from DDB) brav 2 ! Bravais Lattice : 1-S.C., 2-F.C., 3-B.C., 4-Hex.) ngqpt 3*6 ! Monkhorst-Pack indices nqshft 1 ! number of q-points in repeated basic q-cell q1shft 3*0.0 !Effective charges asr 1 ! Acoustic Sum Rule. 1 => imposed asymetrically chneut 1 ! Charge neutrality requirement for effective charges. !Interatomic force constant info dipdip 1 ! Dipole-dipole interaction treatment !Phonon band structure output for band2eps - See note near end for ! dealing with gamma LO-TO splitting issue. eivec 4 !Wavevector list number 1 (Reduced coordinates and normalization factor) nph1l 71 ! number of phonons in list 1 qph1l 0.0000 0.0000 0.0000 1.0 !(gamma point) 0.0375 0.0375 0.0750 1.0 0.0750 0.0750 0.1500 1.0 0.1125 0.1125 0.2250 1.0 0.1500 0.1500 0.3000 1.0 0.1875 0.1875 0.3750 1.0 0.2250 0.2250 0.4500 1.0 0.2625 0.2625 0.5250 1.0 0.3000 0.3000 0.6000 1.0 0.3375 0.3375 0.6750 1.0 0.3750 0.3750 0.7500 1.0 !(K point) 0.3875 0.3875 0.7750 1.0 0.4000 0.4000 0.8000 1.0 0.4125 0.4125 0.8250 1.0 0.4250 0.4250 0.8500 1.0 0.4375 0.4375 0.8750 1.0 0.4500 0.4500 0.9000 1.0 0.4625 0.4625 0.9250 1.0 0.4750 0.4750 0.9500 1.0 0.4875 0.4875 0.9750 1.0 0.5000 0.5000 1.0000 1.0 !(X point) 0.5500 0.5500 1.0000 1.0 0.6000 0.6000 1.0000 1.0 0.6500 0.6500 1.0000 1.0 0.7000 0.7000 1.0000 1.0 0.7500 0.7500 1.0000 1.0 0.8000 0.8000 1.0000 1.0 0.8500 0.8500 1.0000 1.0 0.9000 0.9000 1.0000 1.0 0.9500 0.9500 1.0000 1.0 1.0000 1.0000 1.0000 1.0 !(gamma point) 0.9500 0.9500 0.9500 1.0 0.9000 0.9000 0.9000 1.0 0.8500 0.8500 0.8500 1.0 0.8000 0.8000 0.8000 1.0 0.7500 0.7500 0.7500 1.0 0.7000 0.7000 0.7000 1.0 0.6500 0.6500 0.6500 1.0 0.6000 0.6000 0.6000 1.0 0.5500 0.5500 0.5500 1.0 0.5000 0.5000 0.5000 1.0 !(L point) 0.5000 0.4500 0.5000 1.0 0.5000 0.4000 0.5000 1.0 0.5000 0.3500 0.5000 1.0 0.5000 0.3000 0.5000 1.0 0.5000 0.2500 0.5000 1.0 0.5000 0.2000 0.5000 1.0 0.5000 0.1500 0.5000 1.0 0.5000 0.1000 0.5000 1.0 0.5000 0.0500 0.5000 1.0 0.5000 0.0000 0.5000 1.0 !(X point) 0.5000 0.0250 0.5250 1.0 0.5000 0.0500 0.5500 1.0 0.5000 0.0750 0.5750 1.0 0.5000 0.1000 0.6000 1.0 0.5000 0.1250 0.6250 1.0 0.5000 0.1500 0.6500 1.0 0.5000 0.1750 0.6750 1.0 0.5000 0.2000 0.7000 1.0 0.5000 0.2250 0.7250 1.0 0.5000 0.2500 0.7500 1.0 !(W point) 0.5000 0.2750 0.7250 1.0 0.5000 0.3000 0.7000 1.0 0.5000 0.3250 0.6750 1.0 0.5000 0.3500 0.6500 1.0 0.5000 0.3750 0.6250 1.0 0.5000 0.4000 0.6000 1.0 0.5000 0.4250 0.5750 1.0 0.5000 0.4500 0.5500 1.0 0.5000 0.4750 0.5250 1.0 0.5000 0.5000 0.5000 1.0 !(L point) !Wavevector list number 2 (Cartesian directions for non-analytic gamma phonons) !The output for this calculation must be cut-and-pasted into the ! t59_out.freq file to be used as band2eps input to get proper LO-TO ! splitting at gamma. Note that gamma occurrs twice. nph2l 1 ! number of directions in list 2 qph2l 1.0 0.0 0.0 0.0 # This line added when defaults were changed (v5.3) to keep the previous, old behaviour symdynmat 0 |
- [abinit-forum] phonon dispersion in ZrO2, Igor Lukacevic, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, pascal boulet, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, Igor Lukacevic, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, pascal boulet, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, Igor Lukacevic, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, Igor Lukacevic, 01/16/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, pascal boulet, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, Igor Lukacevic, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, Xavier Gonze, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, Igor Lukacevic, 01/12/2010
- Re: Re: [abinit-forum] phonon dispersion in ZrO2, ilukacevic, 01/18/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, Igor Lukacevic, 01/12/2010
- Re: [abinit-forum] phonon dispersion in ZrO2, pascal boulet, 01/12/2010
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