| ²é¿´: 3879 | »Ø¸´: 2 | |||
xunèÉË®²Ýгæ (³õÈëÎÄ̳)
|
[½»Á÷]
[VASP] ÇóÖú£ºDFPT·¨Ëã³öÀ´µÄÓÐLO-TOÅüÁѵÄÉù×ÓÆ×ÔÚGµã¶Ï¿ªÁË£¬ÒªÈçºÎ½â¾öÄØ ÒÑÓÐ2È˲ÎÓë
|
|
ÈçÌ⣬ϣÍûÄÜÓÐÉù×Ó¼ÆËã·½ÃæµÄ¸ßÈ˰ïÎÒ½â¾öÒ»ÏÂÕâ¸öÎÊÌ⣬ÎÒÕæµÄ¼¼ÇîÁË Ñ¹Ëõ°üÀïµÄSPOSCARÊÇ3*3*3À©°ûµÄ½á¹û£¬ÊÇÎÒ¼ÆËãËùʹÓõġ£ÔÚphonopy½øÐкó´¦ÀíµÄʱºò¶îÍ⿼ÂÇÁËLO-TOÅüÁÑ INCAR£º NELM=100 EDIFF = 1e-9 ! It is a recommended value. When calculating phonon, 1e-9 at least. AMIX=0.7 BMIX=0.01 #NBANDS = 96 ! Default = NELECT/2 + NIONS/2 #NPAR=8 #NCORE=6 KPAR=10 ! When irreducible k-points are large in amount, may increase KPAR, which will increase memory usage in most instances and sharply increase speed. ###Parallel settings are related to convergence, but have no certain relation. If electron step fail, change the above three may solve problem. ISTART = 0 ICHARG = 2 ! For band structures,with ISTART=0 and ICHARG=11. Copying WAVECAR and using ISTRAT=1 may lead to fault in high excited states and lower speed #LORBIT = 11 #LAMXMIX=4 ! system includes d-element, 4 ; system includes f-element, 6 LWAVE = .FALSE. LCHARG = .FALSE. ! Sometimes it should be commented #NWRITE=3 #LREAL=A ! When calculating phonon, do not change it. Default setting is .FALSE. #ISYM = -1 SYMPREC = 1e-6 ! Default 1e-5 #GGA = PE GGA_COMPAT = .FALSE. ! Apply spherical cutoff on gradient field. #ALGO = Fast ! When precision is high in many aspects, usually need to comment it. NEVER use Exact except some kinds of GW. Exact will decrease speed by thousands of times. When electron step goes wrong, see wiki or comment it to solve. ISMEAR = 0 ! Gaussian smearing usually, 1 for metal, -5 for DOS or accurate Etot SIGMA = 0.01 ! Default=0.2, for metals; other should be smaller. For phonon calculation, 0.03 at least PREC = Accurate ! Use it in phonon calculation ENCUT = 450 ! Please set it manually KSPACING=0.15 ADDGRID=.TRUE. #LSORBIT = .TRUE. #LNONCOLLINEAR = .TRUE. #ISPIN = 2 ! Default=1; 2 for spin-polarized calculations #MAGMOM = 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 #LDAU = .TRUE. #LDAUU = [real array] ! Coulomb interaction parameters #LDAUJ = [real array] ! Exchange interaction parameters #LHFCALC = .TRUE. ! Hartree-Fock Calculation. Recommended all bands simultaneous algorithm #HFSCREEN = [real] #SCISSOR= #LVEL = .TRUE. #LOPTICS = .TRUE. CSHIFT=0.05 NEDOS=4000 ! Number of grid points for the electronic density of states and dielectric function #OMEGAMAX=70 ! It can not change the frequency range of calculation for ionic dielectricfunction whatever IBRION=6 or 7 or 8, but can change range for electron dielectricfunction and cause little(or nothing) difference to dielectricfunction's values when the change of OMEGAMAX is not large, so in this case, OMEGAMAX can be used. #For ionic dielectricfunction, it is possible for VASP that whole range(highest frequency) can be calculated will be calculated, so to change range, should change accuracy to include higher frequency phonon modes, which means change supercell size. K density, ISYM, NBAND, parallel setting have very little effects on upper limit #OMEGATL ! do not effect electron and ion dielectricfunction in every aspect, should not use it. #DIPOL = [real array] ! center for cell in direct coordinates #LVTOT = .TRUE. ! Total local potential #LVHAR = .TRUE. ! Containing entire local potential #LELF = .TRUE. ! Electron localization function #LBERRY = .TRUE. ! #LCALCPOL = .TRUE. #LCALCEPS = .TRUE. #EFIELD_PEAD = 0 0 0 ! unit eV/Ang #LASPH=.TRUE. ! For Raman's latter half series calculations, use it and LEPSILON. IBRION=8 LEPSILON=.TRUE. ! Ionic dielectric function. DFPT need no more empty bands #use supercell that: 1three lattice constants have little difference, 2lattice constants > 10A, 3atom number > 90. Every result relying on IBRION=5-8 must use supercell. #When ISYM=2, do not support NCORE!=1, but support kpoints parallel. Kpoints parallel do not change dielectricfunction's values. When ISYM=-1, support band parallel. This role also applies to Raman. #LPHON_POLAR=.TRUE. ! Static dielectric tensor and Born charges that are needed for LO-TO splitting are also need supercell calculation. #PHON_DIELECTRIC= #PHON_BORN_CHARGES= |
» ²ÂÄãϲ»¶
279·ÖÇóµ÷¼Á Ò»Ö¾Ô¸211
ÒѾÓÐ16È˻ظ´
Çóµ÷¼ÁÒ»Ö¾Ô¸Î人Àí¹¤´óѧ²ÄÁϹ¤³Ì£¨085601£©
ÒѾÓÐ5È˻ظ´
ÉϺ£µçÁ¦´óѧ²ÄÁÏ·À»¤ÓëвÄÁÏÖØµãʵÑéÊÒÕÐÊÕµ÷¼ÁÑо¿Éú£¨²ÄÁÏ¡¢»¯Ñ§¡¢µç»¯Ñ§£¬»·¾³£©
ÒѾÓÐ3È˻ظ´
¼±·¢ºËÐÄÆÚ¿¯ÂÛÎÄ
ÒѾÓÐ5È˻ظ´
291 Çóµ÷¼Á
ÒѾÓÐ5È˻ظ´
298-Ò»Ö¾Ô¸Öйúũҵ´óѧ-Çóµ÷¼Á
ÒѾÓÐ11È˻ظ´
Ò»Ö¾Ô¸ÄϾ©Àí¹¤´óѧ085701×ÊÔ´Óë»·¾³302·ÖÇóµ÷¼Á
ÒѾÓÐ7È˻ظ´
316Çóµ÷¼Á
ÒѾÓÐ7È˻ظ´
²ÄÁÏÓ뻯¹¤¿¼Ñе÷¼Á
ÒѾÓÐ4È˻ظ´
Ò»Ö¾Ô¸ÖØÇì´óѧ085700×ÊÔ´Óë»·¾³£¬×Ü·Ö308Çóµ÷¼Á
ÒѾÓÐ7È˻ظ´

dxcharlary
ר¼Ò¹ËÎÊ (Ö°Òµ×÷¼Ò)
-

ר¼Ò¾Ñé: +83 - 1STÇ¿Ìû: 2
- Ó¦Öú: 251 (´óѧÉú)
- ½ð±Ò: 10420.1
- É¢½ð: 155
- ºì»¨: 65
- Ìû×Ó: 3137
- ÔÚÏß: 757.6Сʱ
- ³æºÅ: 936718
- ×¢²á: 2010-01-04
- רҵ: Äý¾Û̬ÎïÐÔI:½á¹¹¡¢Á¦Ñ§ºÍ
- ¹ÜϽ: µÚÒ»ÐÔÔÀí
2Â¥2025-05-03 20:34:29
С³æ³æLG
ľ³æ (ÕýʽдÊÖ)
- Ó¦Öú: 114 (¸ßÖÐÉú)
- ½ð±Ò: 1775.9
- É¢½ð: 1871
- ºì»¨: 25
- Ìû×Ó: 975
- ÔÚÏß: 678.5Сʱ
- ³æºÅ: 2128430
- ×¢²á: 2012-11-15
- ÐÔ±ð: GG
- רҵ: Äý¾Û̬ÎïÐÔ II £ºµç×ӽṹ
3Â¥2025-05-16 16:53:23













»Ø¸´´ËÂ¥