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# Ni fcc structure with two atoms per unit cell

#Ni is a ferromagnatic material
#spin definition
nsppol  2
nspden  2
spinat   0.0 0.0   4.0

prtdos   1  
prtden   1


#Structure optimize
optcell  1
ionmov   2
ntime    15
dilatmx  1.05
tolmxf   1.0e-6
ecutsm   0.5

#######################################################
#Common data
acell    3*6.65184
rprim    0.0   0.5  0.5
         0.5   0.0  0.5
         0.5   0.5  0.0

ntypat   1
znucl    28

   
natom    1
typat    1

xred     0.0  0.0  0.0
        

ixc      11

occopt   3  
tsmear   0.01
nband    10

kptopt   1
ngkpt    8 8 8
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
   
ecut     60.0
tolvrs   1.0d-18
iscf     5
nstep    70


diemac   12
¼ÆËãµÃµ½µÄ½á¹ûÊÇ£ºacell=6.73,²éÔÄÎÄÏ׵Ľá¹ûÊÇ£º6.65.
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# Ni fcc structure with two atoms per unit cell

#Ni is a ferromagnatic material
#spin definition
nsppol  2
nspden  2
spinat   0.0 0.0   4.0

prtdos   1  
prtden   1


#Structure optimize
#optcell  1
#ionmov   2
#ntime    15
#dilatmx  1.05
#tolmxf   1.0e-6
ecutsm    0.5

#######################################################
#Common data
acell    3*6.65
rprim    0.0   0.5  0.5
         0.5   0.0  0.5
         0.5   0.5  0.0

ntypat   1
znucl    28

   
natom    1
typat    1

xred     0.0  0.0  0.0
        

ixc      11

occopt   3  
tsmear   0.01
nband    10

kptopt   1
ngkpt    8 8 8
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
   
ecut     50
tolvrs   1.0d-18
iscf     5
nstep    70


diemac   12
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# Crystalline Ni : computation of the second drivative of the total energy
#

#Ni is a ferromagnatic material
#spin definition
  nsppol   2
  nspden   2
  spinat   0.0  0.0  4.0



#Response-function calculatio, with q=0
  rfphon   1            # Will consider phonon-type perturbation
rfatpol   1 1          # all the  atoms wiil be displaced
   rfdir   1 1 1        # Along the first reduced coordinate axis
    nqpt   1            # One wavevector is to be considered
     qpt   0 0 0        # This wavevector is q=0 (Gamma)
  kptopt   2            # Automatic generation of k points, taking
                        # into account the time-reversal symmetry only
  tolvrs   1.0d-8       # SCF stopping criterion
    iscf   5            # Self-consistent calculation, using algorithm 5
  irdwfk   1            # Read the ground-state wavefunctions

#########################################################################
#common input variables

#Definition of the unit cell
acell 3*6.65   
rprim  0.0  0.5  0.5   # In lessons 1 and 2, these primitive vectors
       0.5  0.0  0.5   # (to be scaled by acell) were 1 0 0  0 1 0  0 0 1
       0.5  0.5  0.0   # that is, the default.

#Definition of the atom types
ntypat 1          # There is only one type of atom
znucl  28         # The keyword "znucl" refers to the atomic number of the
                  # possible type(s) of atom. The pseudopotential(s)
                  # mentioned in the "files" file must correspond
                  # to the type(s) of atom. Here, the only type is Silicon.
                        

#Definition of the atoms
natom 1           # There are two atoms
typat 1           # They both are of type 1, that is, Silicon.
xred              # This keyword indicate that the location of the atoms
                  # will follow, one triplet of number for each atom
   0.0  0.0  0.0  # Triplet giving the REDUCED coordinate of atom 1.
                  # Triplet giving the REDUCED coordinate of atom 2.
                  # Note the use of fractions (remember the limited
                  # interpreter capabilities of ABINIT)

#Definition of the planewave basis set
ecut  50.0         # Maximal kinetic energy cut-off, in Hartree

#Definition of the k-point grid

ngkpt 8 8 8        # This is a 8x8x8 grid based on the primitive vectors
nshiftk 4          # of the reciprocal space (that form a BCC lattice !),
                   # repeated four times, with different shifts :
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
                  # In cartesian coordinates, this grid is simple cubic, and
                  # actually corresponds to the
                  # so-called 4x4x4 Monkhorst-Pack grid

ixc    11
  

occopt 3
tsmear 0.05
nband  10
#Definition of the SCF procedure
nstep  80          # Maximal number of SCF cycles

                  
diemac 12.0        # Although this is not mandatory, it is worth to
                   # precondition the SCF cycle. The model dielectric
                   # function used as the standard preconditioner
                   # is described in the "dielng" input variable section.
                   # Here, we follow the prescription for bulk silicon.
ÎÊÌâ¾ÍÀ´ÁË£¬µÃ²»µ½ºÏÀíµÄ½á¹û£¬
¶øÇÒlogÖÐÓÐÒ»´ó¶ÑÕâÑùµÄWARNING:
cgwf3.F90:701:WARNING
New trial energy at line 4 = -8.174248E+02
is higher than former: -8.174248E+02
µÃµ½GammaµãÉù×Ó¾¹È»Îª£º
Phonon wavevector (reduced coordinates) : 0.00000 0.00000 0.00000
Phonon energies in Hartree :
-3.212615E-03 -3.212615E-03 -3.212615E-03
Phonon frequencies in cm-1 :
- -7.050876E+02 -7.050876E+02 -7.050876E+02
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