# Pt (fcc) with spin-orbit
  ndtset  3
  tolwfr  1.0d-10

# Dataset 1 : self-consistent ground state calculation
 kptopt1  1
  nband  24
  ngkpt  4 4 4
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

############################
# Dataset 2: 
# invoke ABINIT --> LOBSTER converter
# Read previous WFK in IBZ and use symmetries
# to produce new WFK in full BZ with istwfk == 1
############################
optdriver2 8
wfk_task2 "wfk_fullbz"
getwfk2   -1   # Read WKF in the IBZ

############################
# Dataset 3: read WFK of dataset 2
############################
#getden3    1
getwfk3   -1
#getwfk3    1
#istwfk3   *1
kptopt3    3

# common input data
   acell  3*7.41
    ecut  15.0
   natom  1
   nstep  50
 nspinor  2     
  #nspden  1     
  ntypat  1
  occopt  3
   rprim  0.0  0.5  0.5
          0.5  0.0  0.5
          0.5  0.5  0.0
  tsmear  0.01
   typat  1
    xred  0.0  0.0  0.0
  znucl   78

 pp_dirpath "$ABI_PSPDIR"
 pseudos "78_Pt_r.oncvpsp.psp8"

#%%<BEGIN TEST_INFO>
#%% [setup]
#%% executable = abinit
#%% [files]
#%% files_to_test = 
#%%   t12.out, tolnlines = 0, tolabs = 0.000e+00, tolrel = 0.000e+00, fld_options = -medium
#%% [paral_info]
#%% max_nprocs = 4
#%% [extra_info]
#%% authors = M. Giantomassi
#%% keywords = psp8, SOC
#%% description = 
#%%   Similar to v7[07]. Here we test optdriver 8 (WFK post-processing) with NC 
#%%   and SO. More specifically, we reconstruct the wavefunctions in the full BZ in
#%%   dataset 2 and we use this WFK to restart the calculation in dataset 3 with 
#%%   the full k-mesh (kptopt 3). The SCF cycle should exit at the first iteration
#%%   since the wavefunctions are already converged.
#%%<END TEST_INFO>