
.Version 6.13.2 of ANADDB 
.(MPI version, prepared for a x86_64_linux_gnu4.4 computer) 

.Copyright (C) 1998-2024 ABINIT group . 
 ANADDB comes with ABSOLUTELY NO WARRANTY.
 It is free software, and you are welcome to redistribute it
 under certain conditions (GNU General Public License,
 see ~abinit/COPYING or http://www.gnu.org/copyleft/gpl.txt).

 ABINIT is a project of the Universite Catholique de Louvain,
 Corning Inc. and other collaborators, see ~abinit/doc/developers/contributors.txt .
 Please read https://docs.abinit.org/theory/acknowledgments for suggested
 acknowledgments of the ABINIT effort.
 For more information, see https://www.abinit.org .

.Starting date : Wed 21 Mar 2012.
- ( at 23h 1 )
  

================================================================================

 -outvars_anaddb: echo values of input variables ----------------------

 Flags :
     ifcflag         1
    elphflag         1
 Miscellaneous information :
       eivec         1
         asr         2
      chneut         0
 Interatomic Force Constants Inputs :
      dipdip         0
      ifcana         1
      ifcout         0
 Description of grid 1 :
        brav         1
       ngqpt         2         2         2
      nqshft         1
      q1shft
                     0.00000000E+00  0.00000000E+00  0.00000000E+00
 Elphon calculation will be carried out
   elphsmear    0.100000E-01
    a2fsmear    0.200000E-04
      mustar    0.100000E-01
      nqpath        12
       qpath
                0.333333E+00     0.333333E+00     0.000000E+00
                0.000000E+00     0.000000E+00     0.000000E+00
                0.500000E+00     0.000000E+00     0.000000E+00
                0.333333E+00     0.333333E+00     0.000000E+00
                0.333333E+00     0.333333E+00     0.500000E+00
                0.000000E+00     0.000000E+00     0.500000E+00
                0.500000E+00     0.000000E+00     0.500000E+00
                0.333333E+00     0.333333E+00     0.500000E+00
                0.500000E+00     0.000000E+00     0.500000E+00
                0.500000E+00     0.000000E+00     0.000000E+00
                0.000000E+00     0.000000E+00     0.000000E+00
                0.000000E+00     0.000000E+00     0.500000E+00
    telphint         1
 Smeared weight integration for elphon
    kptrlatt  2   0   0     0   2   0     0   0   2
kptrlatt_fin  2   0   0     0   2   0     0   0   2
 Will keep band dependency in gkk in memory.
 WARNING: the memory requirements will be multiplied by nbands**2 !!!
 scalar product will be performed when assembling the gamma matrices.
 WARNING: with this option you can not distinguish which 
    linewidth comes from which phonon mode !!!
 Will perform transport calculation in elphon to get
 resistivity and thermal conductivity as a function of T

 Minimum temperature for transport outputs:     0.000000E+00 K
 Maximum temperature for transport outputs:     1.000000E+03 K
 Number of temperature points for transport outputs:   1000

 First list of wavevector (reduced coord.) :
       nph1l         1
       qph1l
                     0.00000000E+00  0.00000000E+00  0.00000000E+00    1.000E+00

================================================================================

 read the DDB information and perform some checks

-begin at tcpu      0.021  and twall      0.022 sec

 Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
 R(1)=  5.5762039  0.0000000  0.0000000  G(1)=  0.1793335  0.1035382  0.0000000
 R(2)= -2.7881019  4.8291342  0.0000000  G(2)=  0.0000000  0.2070765  0.0000000
 R(3)=  0.0000000  0.0000000  8.8543118  G(3)=  0.0000000  0.0000000  0.1129393
 Unit cell volume ucvol=  2.3843101E+02 bohr^3
 Angles (23,13,12)=  9.00000000E+01  9.00000000E+01  1.20000000E+02 degrees
 Now the whole DDB is in central memory

================================================================================

 Calculation of the interatomic forces 

-begin at tcpu      0.023  and twall      0.123 sec
       Homogeneous q point set in the B.Z.
 Grid q points  :        8
  1)   0.00000000E+00  0.00000000E+00  0.00000000E+00
  2)   5.00000000E-01  0.00000000E+00  0.00000000E+00
  3)   0.00000000E+00  5.00000000E-01  0.00000000E+00
  4)   5.00000000E-01  5.00000000E-01  0.00000000E+00
  5)   0.00000000E+00  0.00000000E+00  5.00000000E-01
  6)   5.00000000E-01  0.00000000E+00  5.00000000E-01
  7)   0.00000000E+00  5.00000000E-01  5.00000000E-01
  8)   5.00000000E-01  5.00000000E-01  5.00000000E-01

 The interatomic forces have been obtained

================================================================================

 Properties based on electron-phonon coupling 

 Found     2 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     6 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     6 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 Found     2 symmetries that leave the perturbation invariant.
 The set of symmetries contains only one element for this perturbation.
 The set of symmetries contains only one element for this perturbation.
 Found     6 symmetries that leave the perturbation invariant.
 The set of symmetries contains only one element for this perturbation.
 The set of symmetries contains only one element for this perturbation.
 Found     6 symmetries that leave the perturbation invariant.
 The set of symmetries contains only one element for this perturbation.
 The set of symmetries contains only one element for this perturbation.
 Found     2 symmetries that leave the perturbation invariant.
 The set of symmetries contains only one element for this perturbation.
 The set of symmetries contains only one element for this perturbation.
 Found     2 symmetries that leave the perturbation invariant.

 Output of the linewidths for the first point of each segment. Linewidths are given in Hartree.

 Q point =    3.333333E-01    3.333333E-01    0.000000E+00   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.466783E-03    2.442410E-06    1.827676E-02
       2        1.866560E-03    1.353819E-06    6.255890E-03
       3        1.896760E-03    1.446832E-06    6.474497E-03
       4        1.963809E-03    7.318684E-07    3.055254E-03
       5        2.016459E-03    2.579450E-06    1.021318E-02
       6        2.464674E-03    3.006910E-06    7.969191E-03

 Q point =    0.000000E+00    0.000000E+00    0.000000E+00   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        0.000000E+00    9.457125E-08    0.000000E+00
       2        0.000000E+00    6.605891E-09    0.000000E+00
       3        0.000000E+00    4.435474E-09    0.000000E+00
       4        1.260508E-03    1.515479E-06    1.535577E-02
       5        1.260508E-03    1.068307E-06    1.082474E-02
       6        3.065941E-03    3.137361E-09    5.373406E-06

 Q point =    5.000000E-01    0.000000E+00    0.000000E+00   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.086292E-03    0.000000E+00    0.000000E+00
       2        1.506042E-03    0.000000E+00    0.000000E+00
       3        1.800205E-03    0.000000E+00    0.000000E+00
       4        2.213736E-03    0.000000E+00    0.000000E+00
       5        2.248636E-03    0.000000E+00    0.000000E+00
       6        2.700875E-03    0.000000E+00    0.000000E+00

 Q point =    3.333333E-01    3.333333E-01    0.000000E+00   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.466783E-03    2.442410E-06    1.827676E-02
       2        1.866560E-03    1.353819E-06    6.255890E-03
       3        1.896760E-03    1.446832E-06    6.474497E-03
       4        1.963809E-03    7.318684E-07    3.055254E-03
       5        2.016459E-03    2.579450E-06    1.021318E-02
       6        2.464674E-03    3.006910E-06    7.969191E-03

 Q point =    3.333333E-01    3.333333E-01    5.000000E-01   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.262017E-03    3.758416E-06    3.799156E-02
       2        1.262017E-03    2.890225E-06    2.921554E-02
       3        1.956643E-03    4.140327E-06    1.741102E-02
       4        1.956643E-03    3.672866E-06    1.544524E-02
       5        2.447783E-03    3.137786E-06    8.431218E-03
       6        2.447783E-03    2.738559E-06    7.358497E-03

 Q point =    0.000000E+00    0.000000E+00    5.000000E-01   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        8.725339E-04    4.880146E-06    1.032003E-01
       2        8.725339E-04    6.824749E-06    1.443227E-01
       3        8.725339E-04    3.743369E-05    7.916090E-01
       4        8.725339E-04    1.629525E-05    3.445951E-01
       5        2.132418E-03    5.650123E-06    2.000442E-02
       6        2.132418E-03    1.060058E-05    3.753163E-02

 Q point =    5.000000E-01    0.000000E+00    5.000000E-01   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.490334E-03    0.000000E+00    0.000000E+00
       2        1.490334E-03    0.000000E+00    0.000000E+00
       3        1.587850E-03    0.000000E+00    0.000000E+00
       4        1.587850E-03    0.000000E+00    0.000000E+00
       5        2.650776E-03    0.000000E+00    0.000000E+00
       6        2.650776E-03    0.000000E+00    0.000000E+00

 Q point =    3.333333E-01    3.333333E-01    5.000000E-01   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.262017E-03    3.758416E-06    3.799156E-02
       2        1.262017E-03    2.890225E-06    2.921554E-02
       3        1.956643E-03    4.140327E-06    1.741102E-02
       4        1.956643E-03    3.672866E-06    1.544524E-02
       5        2.447783E-03    3.137786E-06    8.431218E-03
       6        2.447783E-03    2.738559E-06    7.358497E-03

 Q point =    5.000000E-01    0.000000E+00    5.000000E-01   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.490334E-03    0.000000E+00    0.000000E+00
       2        1.490334E-03    0.000000E+00    0.000000E+00
       3        1.587850E-03    0.000000E+00    0.000000E+00
       4        1.587850E-03    0.000000E+00    0.000000E+00
       5        2.650776E-03    0.000000E+00    0.000000E+00
       6        2.650776E-03    0.000000E+00    0.000000E+00

 Q point =    5.000000E-01    0.000000E+00    0.000000E+00   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        1.086292E-03    0.000000E+00    0.000000E+00
       2        1.506042E-03    0.000000E+00    0.000000E+00
       3        1.800205E-03    0.000000E+00    0.000000E+00
       4        2.213736E-03    0.000000E+00    0.000000E+00
       5        2.248636E-03    0.000000E+00    0.000000E+00
       6        2.700875E-03    0.000000E+00    0.000000E+00

 Q point =    0.000000E+00    0.000000E+00    0.000000E+00   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        0.000000E+00    9.457125E-08    0.000000E+00
       2        0.000000E+00    6.605891E-09    0.000000E+00
       3        0.000000E+00    4.435474E-09    0.000000E+00
       4        1.260508E-03    1.515479E-06    1.535577E-02
       5        1.260508E-03    1.068307E-06    1.082474E-02
       6        3.065941E-03    3.137361E-09    5.373406E-06

 Q point =    0.000000E+00    0.000000E+00    5.000000E-01   isppol =    1
 Mode number    Frequency (Ha)  Linewidth (Ha)  Lambda(q,n)
       1        8.725339E-04    4.880146E-06    1.032003E-01
       2        8.725339E-04    6.824749E-06    1.443227E-01
       3        8.725339E-04    3.743369E-05    7.916090E-01
       4        8.725339E-04    1.629525E-05    3.445951E-01
       5        2.132418E-03    5.650123E-06    2.000442E-02
       6        2.132418E-03    1.060058E-05    3.753163E-02


 Superconductivity : isotropic evaluation of parameters from electron-phonon coupling.

 mka2f: isotropic lambda =     1.679635E-01
 mka2f: lambda <omega^2> =     3.735701E-07
 mka2f: lambda <omega^3> =     6.788315E-10
 mka2f: lambda <omega^4> =     1.385978E-12
 mka2f: lambda <omega^5> =     3.081777E-15
 mka2f: omegalog  =     1.326317E-03 (Ha)     4.188172E+02 (Kelvin)
 mka2f: input mustar =     1.000000E-02
-mka2f: MacMillan Tc =     4.805473E-07 (Ha)     1.517447E-01 (Kelvin)
 mka2f_tr: 1/3 trace of TRANSPORT lambda for isppol   1 =      2.004060E-01

================================================================================

 Treat the first list of vectors 

-begin at tcpu      1.246  and twall      2.046 sec
 
  Phonon wavevector (reduced coordinates) :  0.00000  0.00000  0.00000
 Phonon energies in Hartree :
   0.000000E+00  0.000000E+00  0.000000E+00  1.260508E-03  1.260508E-03
   3.065941E-03
 Phonon frequencies in cm-1    :
-  0.000000E+00  0.000000E+00  0.000000E+00  2.766494E+02  2.766494E+02
-  6.728962E+02

 Eigendisplacements 
 (will be given, for each mode : in cartesian coordinates
   for each atom the real part of the displacement vector,
   then the imaginary part of the displacement vector)
  Mode number    1   Energy    0.000000E+00
 Attention : low frequency mode.
   (Could be unstable or acoustic mode)
;  1  0.00000000E+00  0.00000000E+00  2.39346937E-03
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2  0.00000000E+00  0.00000000E+00  2.39346937E-03
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    2   Energy    0.000000E+00
 Attention : low frequency mode.
   (Could be unstable or acoustic mode)
;  1  0.00000000E+00 -2.39346937E-03  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2  0.00000000E+00 -2.39346937E-03  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    3   Energy    0.000000E+00
 Attention : low frequency mode.
   (Could be unstable or acoustic mode)
;  1  2.39346940E-03  0.00000000E+00  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2  2.39346941E-03  0.00000000E+00  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    4   Energy    1.260508E-03
;  1  1.26482544E-04  2.39012509E-03  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2 -1.26482545E-04 -2.39012509E-03  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    5   Energy    1.260508E-03
;  1  2.39012510E-03 -1.26482551E-04  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2 -2.39012509E-03  1.26482538E-04  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    6   Energy    3.065941E-03
;  1  0.00000000E+00  0.00000000E+00  2.39346940E-03
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2  0.00000000E+00  0.00000000E+00 -2.39346941E-03
;     0.00000000E+00  0.00000000E+00  0.00000000E+00

 Analysis of degeneracies and characters (maximum tolerance=1.00E-06 a.u.)
 For each vibration mode, or group of modes if degenerate,
 the characters are given for each symmetry operation (see the list in the log file).
 Symmetry characters of vibration mode #   1
       degenerate with vibration modes #   2 to    3
  3.0 -3.0  1.0 -1.0  2.0 -2.0  1.0 -1.0  0.0  0.0  1.0 -1.0 -1.0  1.0  1.0 -1.0
  0.0  0.0  1.0 -1.0  2.0 -2.0  1.0 -1.0
 Symmetry characters of vibration mode #   4
        degenerate with vibration mode #   5
  2.0  2.0  0.0  0.0 -1.0 -1.0 -0.0 -0.0 -1.0 -1.0  0.0  0.0  2.0  2.0  0.0  0.0
 -1.0 -1.0 -0.0 -0.0 -1.0 -1.0  0.0  0.0
 Symmetry characters of vibration mode #   6
  1.0  1.0 -1.0 -1.0 -1.0 -1.0  1.0  1.0  1.0  1.0 -1.0 -1.0 -1.0 -1.0  1.0  1.0
  1.0  1.0 -1.0 -1.0 -1.0 -1.0  1.0  1.0

================================================================================

+Total cpu time      1.246  and wall time      2.047 sec

 anaddb : the run completed succesfully.
