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<div>Dear QE users, <BR>
  I have calculated the density of states (DOS) of pure graphene.  The supercell used in my work  is a rectangular cell containing 60 carbon atoms.   But something has puzzled me greatly. There is always a little energy gap (~0.2 eV) in the DOS, which contracts with the fact that graphene is zero gap semiconductor. Although I have change many parameters. This problem has not been solved. Here I give the input file and I will be greatly appreciated if you can give me some suggestions. <BR>
For scf.in                                                                                      <BR>
&CONTROL <BR>
     title = 'graphene layer' , <BR>
     calculation = 'scf' , <BR>
     restart_mode = 'from_scratch' , <BR>
     outdir = './tmp' , <BR>
     pseudo_dir = '~pseudo' , <BR>
     prefix = 'graphene' , <BR>
 / <BR>
 &SYSTEM <BR>
     ibrav = 8 , <BR>
     a = 12.31 , b = 12.79312342 , c = 12.000 , <BR>
     nat = 60 , <BR>
     ntyp = 1 , <BR>
     occupations = 'smearing' , <BR>
     tot_charge = 0.0, <BR>
     degauss = 0.02 , <BR>
     smearing = 'mp' , <BR>
     nspin = 2 , <BR>
     starting_magnetization(1) = 0.5 , <BR>
     ecutwfc = 30.0 , <BR>
     ecutrho = 300.0 , <BR>
 / <BR>
 &ELECTRONS <BR>
     conv_thr = 1.0d-8 , <BR>
     mixing_mode = 'local-TF' , <BR>
     mixing_beta = 0.7 , <BR>
     diagonalization = 'david' , <BR>
 / <BR>
ATOMIC_SPECIES <BR>
  C   12.0107  C.pbe-rrkjus.UPF <BR>
ATOMIC_POSITIONS crystal <BR>
 C   0.0000000       0.0000000      0.50000000 <BR>
 C  0.10000000      5.55555671E-02  0.50000000 <BR>
 C  0.10000000      0.16666667      0.50000000 <BR>
 C   0.0000000      0.22222224      0.50000000 <BR>
 C   0.0000000      0.33333334      0.50000000 <BR>
 C  0.10000000      0.38888890      0.50000000 <BR>
 C  0.10000000      0.50000000      0.50000000 <BR>
 C   0.0000000      0.55555558      0.50000000 <BR>
 C   0.0000000      0.66666669      0.50000000 <BR>
 C  0.10000000      0.72222227      0.50000000 <BR>
 C  0.10000000      0.83333337      0.50000000 <BR>
 C   0.0000000      0.88888896      0.50000000 <BR>
 C  0.20000000       0.0000000      0.50000000 <BR>
 C  0.30000001      5.55555671E-02  0.50000000 <BR>
 C  0.30000001      0.16666667      0.50000000 <BR>
 C  0.20000000      0.22222224      0.50000000 <BR>
 C  0.20000000      0.33333334      0.50000000 <BR>
 C  0.30000001      0.38888890      0.50000000 <BR>
 C  0.30000001      0.50000000      0.50000000 <BR>
 C  0.20000000      0.55555558      0.50000000 <BR>
 C  0.20000000      0.66666669      0.50000000 <BR>
 C  0.30000001      0.72222227      0.50000000 <BR>
 C  0.30000001      0.83333337      0.50000000 <BR>
 C  0.20000000      0.88888896      0.50000000 <BR>
 C  0.40000001       0.0000000      0.50000000 <BR>
 C  0.50000000      5.55555671E-02  0.50000000 <BR>
 C  0.50000000      0.16666667      0.50000000 <BR>
 C  0.40000001      0.22222224      0.50000000 <BR>
 C  0.40000001      0.33333334      0.50000000 <BR>
 C  0.50000000      0.38888890      0.50000000 <BR>
 C  0.50000000      0.50000000      0.50000000 <BR>
 C  0.40000001      0.55555558      0.50000000 <BR>
 C  0.40000001      0.66666669      0.50000000 <BR>
 C  0.50000000      0.72222227      0.50000000 <BR>
 C  0.50000000      0.83333337      0.50000000 <BR>
 C  0.40000001      0.88888896      0.50000000 <BR>
 C  0.60000002       0.0000000      0.50000000 <BR>
 C  0.70000005      5.55555671E-02  0.50000000 <BR>
 C  0.70000005      0.16666667      0.50000000 <BR>
 C  0.60000002      0.22222224      0.50000000 <BR>
 C  0.60000002      0.33333334      0.50000000 <BR>
 C  0.70000005      0.38888890      0.50000000 <BR>
 C  0.70000005      0.50000000      0.50000000 <BR>
 C  0.60000002      0.55555558      0.50000000 <BR>
 C  0.60000002      0.66666669      0.50000000 <BR>
   C  0.70000005      0.72222227      0.50000000 <BR>
 C  0.70000005      0.83333337      0.50000000 <BR>
 C  0.60000002      0.88888896      0.50000000 <BR>
 C  0.80000001       0.0000000      0.50000000 <BR>
 C  0.90000004      5.55555671E-02  0.50000000 <BR>
 C  0.90000004      0.16666667      0.50000000 <BR>
 C  0.80000001      0.22222224      0.50000000 <BR>
 C  0.80000001      0.33333334      0.50000000 <BR>
 C  0.90000004      0.38888890      0.50000000 <BR>
 C  0.90000004      0.50000000      0.50000000 <BR>
 C  0.80000001      0.55555558      0.50000000 <BR>
 C  0.80000001      0.66666669      0.50000000 <BR>
 C  0.90000004      0.72222227      0.50000000 <BR>
 C  0.90000004      0.83333337      0.50000000 <BR>
 C  0.80000001      0.88888896      0.50000000 <BR>
 K_POINTS automatic <BR>
 8 8 1 0 0 0 <BR>
For  nscf.in   <BR>
&CONTROL <BR>
     title = 'graphene layer' , <BR>
     calculation = 'nscf' , <BR>
     restart_mode = 'from_scratch' , <BR>
     outdir = './tmp' , <BR>
     pseudo_dir = '/lustre/ISSP2/tfcao/pseudo' , <BR>
     prefix = 'graphene' , <BR>
 / <BR>
 &SYSTEM <BR>
     ibrav = 8 , <BR>
     a = 12.31 , b = 12.79312342 , c = 12.000 , <BR>
     nat = 60 , <BR>
     ntyp = 1 , <BR>
     occupations = 'tetrahedra' , <BR>
     tot_charge = 0.0, <BR>
     nspin = 2 , <BR>
     starting_magnetization(1) = 0.5 , <BR>
     ecutwfc = 30.0 , <BR>
     ecutrho = 300.0 , <BR>
 / <BR>
 &ELECTRONS <BR>
     conv_thr = 1.0d-8 , <BR>
     mixing_mode = 'local-TF' , <BR>
     mixing_beta = 0.7 , <BR>
     diagonalization = 'david' , <BR>
 / <BR>
ATOMIC_SPECIES <BR>
  C   12.0107  C.pbe-rrkjus.UPF <BR>
For dos.in  <BR>
 &inputpp <BR>
  prefix = 'graphene' , <BR>
  outdir = './tmp' , <BR>
  Emin = -4.0 , <BR>
  Emax = 4.0 , <BR>
  DeltaE = 0.01 , <BR>
  fildos = graphene.dos , <BR>
/ <BR>
The accessory is the DOS I have got.                                                             <BR>
I  am sorry for such a long file. I hope that you can give some suggestions.   <BR>
====================================================================== <BR>
Tengfei Cao,   Research Laboratory for Computational Materials Sciences, <BR>
Instutue of Solid State Physics,the Chinese Academy of Sciences, <BR>
<BR>
====================================================================== <BR>
<BR>
<BR>
<BR>
<BR>
<BR>
<BR>
                                                                                                                                                                                                                                                                          93,2         底端 <BR>
                                                                                                                                                                                                                                                                       1,2          顶端 <BR>
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