.Version 9.11.2 of ANADDB 
.(MPI version, prepared for a x86_64_linux_gnu9.3 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 : Sat 15 Jul 2023.
- ( at 12h08 )
  

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

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

 Flags :
     dieflag         1
      nlflag         2
 Miscellaneous information :
       eivec         1
         asr         1
      chneut         2
 Frequency information :
       nfreq       100
       frmin         0.00000000E+00
       frmax         2.00000000E-03
 Non-linear response information :
      alphon         1
      prtmbm         1
     ramansr         1
 First list of wavevector (reduced coord.) :
       nph1l         1
       qph1l
                     0.00000000E+00  0.00000000E+00  0.00000000E+00    1.000E+00
 Second list of wavevector (cart. coord.) :
       nph2l         3
       qph2l
                     1.00000000E+00  0.00000000E+00  0.00000000E+00    0.000E+00
                     0.00000000E+00  1.00000000E+00  0.00000000E+00    0.000E+00
                     0.00000000E+00  0.00000000E+00  1.00000000E+00    0.000E+00

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

 read the DDB information and perform some checks


  ==== Info on the Cryst% object ====
 Real(R)+Recip(G) space primitive vectors, cartesian coordinates (Bohr,Bohr^-1):
 R(1)=  0.0000000  5.3082654  5.3082654  G(1)= -0.0941927  0.0941927  0.0941927
 R(2)=  5.3082654  0.0000000  5.3082654  G(2)=  0.0941927 -0.0941927  0.0941927
 R(3)=  5.3082654  5.3082654  0.0000000  G(3)=  0.0941927  0.0941927 -0.0941927
 Unit cell volume ucvol=  2.9914923E+02 bohr^3
 Angles (23,13,12)=  6.00000000E+01  6.00000000E+01  6.00000000E+01 degrees
 Time-reversal symmetry is present
 Reduced atomic positions [iatom, xred, symbol]:
    1)    0.0000000  0.0000000  0.0000000  Al
    2)    0.2500000  0.2500000  0.2500000  As

 DDB file with 2 blocks has been read.

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

 Dielectric Tensor and Effective Charges 


 anaddb : Zero the imaginary part of the Dynamical Matrix at Gamma,
   and impose the ASR on the effective charges 

 The violation of the charge neutrality conditions
 by the effective charges is as follows :
    atom        electric field
 displacement     direction
       1               1       -1.429236        0.000000
       1               2       -0.000000        0.000000
       1               3       -0.000000        0.000000
       2               1       -0.000000        0.000000
       2               2       -1.429236        0.000000
       2               3        0.000000        0.000000
       3               1        0.000000        0.000000
       3               2        0.000000        0.000000
       3               3       -1.429236        0.000000

 Effective charge tensors after 
 imposition of the charge neutrality (if requested by user),
 and eventual restriction to some part :
   atom    displacement
         1         1    1.992108E+00    2.282375E-17    2.293757E-17
         1         2    2.282375E-17    1.992108E+00   -2.270993E-17
         1         3   -2.282375E-17   -2.282375E-17    1.992108E+00
         2         1   -1.992108E+00   -2.282375E-17   -2.293757E-17
         2         2   -2.282375E-17   -1.992108E+00    2.270993E-17
         2         3    2.282375E-17    2.282375E-17   -1.992108E+00
 Now, the imaginary part of the dynamical matrix is zeroed
 

 Non-linear optical coefficients d (pm/V)
    0.000000    0.000000    0.000000   32.723426    0.000000    0.000000
    0.000000   -0.000000    0.000000    0.000000   32.723426    0.000000
    0.000000    0.000000    0.000000    0.000000    0.000000   32.723426
 

 The violation of the Raman sum rule
 by the first-order electronic dielectric tensors is as follows
     atom
  displacement
       1        0.000000000        0.000000000        0.000000000
                0.000000000        0.000000000       -0.005004057
                0.000000000       -0.005004057       -0.000000000

       2       -0.000000000        0.000000000       -0.005004057
                0.000000000        0.000000001        0.000000000
               -0.005004057        0.000000000        0.000000000

       3        0.000000000       -0.005004057        0.000000000
               -0.005004057        0.000000000        0.000000000
                0.000000000        0.000000000        0.000000000

 

  First-order change in the electronic dielectric 
  susceptibility tensor (Bohr^-1)
  induced by an atomic displacement
  (after imposing the sum over all atoms to vanish)
   atom  displacement
    1          1        0.000000000        0.000000000        0.000000000
                        0.000000000       -0.000000000       -0.192466932
                        0.000000000       -0.192466932       -0.000000000
    1          2       -0.000000000        0.000000000       -0.192466932
                        0.000000000        0.000000000        0.000000000
                       -0.192466932        0.000000000        0.000000000
    1          3        0.000000000       -0.192466932        0.000000000
                       -0.192466932       -0.000000000        0.000000000
                        0.000000000        0.000000000        0.000000000

    2          1       -0.000000000       -0.000000000       -0.000000000
                       -0.000000000       -0.000000000        0.192466932
                       -0.000000000        0.192466932        0.000000000
    2          2        0.000000000       -0.000000000        0.192466932
                       -0.000000000       -0.000000000       -0.000000000
                        0.192466932       -0.000000000       -0.000000000
    2          3       -0.000000000        0.192466932       -0.000000000
                        0.192466932       -0.000000000       -0.000000000
                       -0.000000000       -0.000000000       -0.000000000


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

 Treat the first list of vectors 


  Phonon wavevector (reduced coordinates) :  0.00000  0.00000  0.00000
 Phonon energies in Hartree :
   0.000000E+00  0.000000E+00  0.000000E+00  1.620427E-03  1.620427E-03
   1.620427E-03
 Phonon frequencies in cm-1    :
-  0.000000E+00  0.000000E+00  0.000000E+00  3.556426E+02  3.556426E+02
-  3.556426E+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 - absolute values smaller than 1.0d-7 are set to zero)
  Mode number    1   Energy    0.000000E+00
 Attention : low frequency mode.
   (Could be unstable or acoustic mode)
-  1  0.00000000E+00  0.00000000E+00 -2.32020398E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  0.00000000E+00 -2.32020414E-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 -2.32020398E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00 -2.32020414E-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  2.32020398E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  2.32020414E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    4   Energy    1.620427E-03
-  1  0.00000000E+00  0.00000000E+00 -3.86630696E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  0.00000000E+00  1.39237441E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    5   Energy    1.620427E-03
-  1  0.00000000E+00  3.86630696E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00 -1.39237441E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    6   Energy    1.620427E-03
-  1  3.86630696E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2 -1.39237441E-03  0.00000000E+00  0.00000000E+00
-     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 -1.0 -1.0 -1.0  1.0 -1.0  1.0 -1.0 -0.0 -0.0 -0.0  0.0  1.0 -1.0 -1.0  1.0
 -0.0 -0.0  0.0 -0.0  1.0  1.0 -1.0 -1.0
 Symmetry characters of vibration mode #   4
       degenerate with vibration modes #   5 to    6
  3.0 -1.0 -1.0 -1.0  1.0 -1.0  1.0 -1.0  0.0 -0.0  0.0 -0.0  1.0 -1.0 -1.0  1.0
  0.0  0.0 -0.0 -0.0  1.0  1.0 -1.0 -1.0

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

 The alphon input variable is non-zero, will mix the degenerate phonon modes
 in order to align the mode effective charges with the cartesian axes.
  
 Mode effective charges 
 Mode number.    x            y            z            length 
-     1          0.000000     0.000000     0.000000     0.000000
-     2         -0.000000     0.000000     0.000000     0.000000
-     3         -0.000000    -0.000000    -0.000000     0.000000
-     4         -0.000000    -0.000000    -2.549253     2.549253
-     5          0.000000     2.549253    -0.000000     2.549253
-     6          2.549253    -0.000000     0.000000     2.549253
  
 Oscillator strengths (in a.u. ; 1 a.u.=253.2638413 m3/s2). Set to zero if abs()<tol14.
 Mode number.       xx          yy          zz          xy          xz          yz          trace
-   1     Real    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-         Imag    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-   2     Real    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-         Imag    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-   3     Real    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-         Imag    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-   4     Real    0.0000E+00  0.0000E+00  1.0974E-04  0.0000E+00  0.0000E+00  0.0000E+00  1.0974E-04
-         Imag    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-   5     Real    0.0000E+00  1.0974E-04  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  1.0974E-04
-         Imag    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00
-   6     Real    1.0974E-04  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  1.0974E-04
-         Imag    0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00  0.0000E+00

 Electronic dielectric tensor
     14.90775987      0.00000000      0.00000000
      0.00000000     14.90775987     -0.00000000
     -0.00000000     -0.00000000     14.90775987


 Relaxed ion dielectric tensor
     16.66342787      0.00000000      0.00000000
      0.00000000     16.66342787      0.00000000
      0.00000000      0.00000000     16.66342787


 Frequency dependent dielectric constant:

 ddb_diel : the number of frequencies is larger than 10 => I will consider only
 the three principal directions, assume that the tensor
 is diagonalized, and give dielectric constant and 
 reflectivities.
 Frequency(Hartree)    Dielectric constant                Reflectivity    
                     x           y          z          x        y        z
  0.0000E+00  1.6663E+01  1.6663E+01  1.6663E+01  3.6779E-01  3.6779E-01  3.6779E-01
  2.0202E-05  1.6664E+01  1.6664E+01  1.6664E+01  3.6780E-01  3.6780E-01  3.6780E-01
  4.0404E-05  1.6665E+01  1.6665E+01  1.6665E+01  3.6781E-01  3.6781E-01  3.6781E-01
  6.0606E-05  1.6666E+01  1.6666E+01  1.6666E+01  3.6782E-01  3.6782E-01  3.6782E-01
  8.0808E-05  1.6668E+01  1.6668E+01  1.6668E+01  3.6785E-01  3.6785E-01  3.6785E-01
  1.0101E-04  1.6670E+01  1.6670E+01  1.6670E+01  3.6787E-01  3.6787E-01  3.6787E-01
  1.2121E-04  1.6673E+01  1.6673E+01  1.6673E+01  3.6791E-01  3.6791E-01  3.6791E-01
  1.4141E-04  1.6677E+01  1.6677E+01  1.6677E+01  3.6795E-01  3.6795E-01  3.6795E-01
  1.6162E-04  1.6681E+01  1.6681E+01  1.6681E+01  3.6800E-01  3.6800E-01  3.6800E-01
  1.8182E-04  1.6686E+01  1.6686E+01  1.6686E+01  3.6805E-01  3.6805E-01  3.6805E-01
  2.0202E-04  1.6691E+01  1.6691E+01  1.6691E+01  3.6811E-01  3.6811E-01  3.6811E-01
  2.2222E-04  1.6697E+01  1.6697E+01  1.6697E+01  3.6818E-01  3.6818E-01  3.6818E-01
  2.4242E-04  1.6704E+01  1.6704E+01  1.6704E+01  3.6826E-01  3.6826E-01  3.6826E-01
  2.6263E-04  1.6711E+01  1.6711E+01  1.6711E+01  3.6834E-01  3.6834E-01  3.6834E-01
  2.8283E-04  1.6719E+01  1.6719E+01  1.6719E+01  3.6843E-01  3.6843E-01  3.6843E-01
  3.0303E-04  1.6727E+01  1.6727E+01  1.6727E+01  3.6853E-01  3.6853E-01  3.6853E-01
  3.2323E-04  1.6736E+01  1.6736E+01  1.6736E+01  3.6863E-01  3.6863E-01  3.6863E-01
  3.4343E-04  1.6746E+01  1.6746E+01  1.6746E+01  3.6874E-01  3.6874E-01  3.6874E-01
  3.6364E-04  1.6757E+01  1.6757E+01  1.6757E+01  3.6886E-01  3.6886E-01  3.6886E-01
  3.8384E-04  1.6768E+01  1.6768E+01  1.6768E+01  3.6899E-01  3.6899E-01  3.6899E-01
  4.0404E-04  1.6780E+01  1.6780E+01  1.6780E+01  3.6913E-01  3.6913E-01  3.6913E-01
  4.2424E-04  1.6793E+01  1.6793E+01  1.6793E+01  3.6928E-01  3.6928E-01  3.6928E-01
  4.4444E-04  1.6806E+01  1.6806E+01  1.6806E+01  3.6943E-01  3.6943E-01  3.6943E-01
  4.6465E-04  1.6821E+01  1.6821E+01  1.6821E+01  3.6960E-01  3.6960E-01  3.6960E-01
  4.8485E-04  1.6836E+01  1.6836E+01  1.6836E+01  3.6977E-01  3.6977E-01  3.6977E-01
  5.0505E-04  1.6852E+01  1.6852E+01  1.6852E+01  3.6996E-01  3.6996E-01  3.6996E-01
  5.2525E-04  1.6870E+01  1.6870E+01  1.6870E+01  3.7015E-01  3.7015E-01  3.7015E-01
  5.4545E-04  1.6888E+01  1.6888E+01  1.6888E+01  3.7036E-01  3.7036E-01  3.7036E-01
  5.6566E-04  1.6907E+01  1.6907E+01  1.6907E+01  3.7058E-01  3.7058E-01  3.7058E-01
  5.8586E-04  1.6927E+01  1.6927E+01  1.6927E+01  3.7081E-01  3.7081E-01  3.7081E-01
  6.0606E-04  1.6949E+01  1.6949E+01  1.6949E+01  3.7105E-01  3.7105E-01  3.7105E-01
  6.2626E-04  1.6972E+01  1.6972E+01  1.6972E+01  3.7131E-01  3.7131E-01  3.7131E-01
  6.4646E-04  1.6996E+01  1.6996E+01  1.6996E+01  3.7158E-01  3.7158E-01  3.7158E-01
  6.6667E-04  1.7021E+01  1.7021E+01  1.7021E+01  3.7186E-01  3.7186E-01  3.7186E-01
  6.8687E-04  1.7048E+01  1.7048E+01  1.7048E+01  3.7217E-01  3.7217E-01  3.7217E-01
  7.0707E-04  1.7076E+01  1.7076E+01  1.7076E+01  3.7248E-01  3.7248E-01  3.7248E-01
  7.2727E-04  1.7106E+01  1.7106E+01  1.7106E+01  3.7282E-01  3.7282E-01  3.7282E-01
  7.4747E-04  1.7138E+01  1.7138E+01  1.7138E+01  3.7317E-01  3.7317E-01  3.7317E-01
  7.6768E-04  1.7171E+01  1.7171E+01  1.7171E+01  3.7355E-01  3.7355E-01  3.7355E-01
  7.8788E-04  1.7207E+01  1.7207E+01  1.7207E+01  3.7394E-01  3.7394E-01  3.7394E-01
  8.0808E-04  1.7245E+01  1.7245E+01  1.7245E+01  3.7436E-01  3.7436E-01  3.7436E-01
  8.2828E-04  1.7284E+01  1.7284E+01  1.7284E+01  3.7480E-01  3.7480E-01  3.7480E-01
  8.4848E-04  1.7327E+01  1.7327E+01  1.7327E+01  3.7527E-01  3.7527E-01  3.7527E-01
  8.6869E-04  1.7371E+01  1.7371E+01  1.7371E+01  3.7576E-01  3.7576E-01  3.7576E-01
  8.8889E-04  1.7419E+01  1.7419E+01  1.7419E+01  3.7629E-01  3.7629E-01  3.7629E-01
  9.0909E-04  1.7470E+01  1.7470E+01  1.7470E+01  3.7684E-01  3.7684E-01  3.7684E-01
  9.2929E-04  1.7524E+01  1.7524E+01  1.7524E+01  3.7743E-01  3.7743E-01  3.7743E-01
  9.4949E-04  1.7581E+01  1.7581E+01  1.7581E+01  3.7806E-01  3.7806E-01  3.7806E-01
  9.6970E-04  1.7643E+01  1.7643E+01  1.7643E+01  3.7873E-01  3.7873E-01  3.7873E-01
  9.8990E-04  1.7709E+01  1.7709E+01  1.7709E+01  3.7944E-01  3.7944E-01  3.7944E-01
  1.0101E-03  1.7779E+01  1.7779E+01  1.7779E+01  3.8020E-01  3.8020E-01  3.8020E-01
  1.0303E-03  1.7855E+01  1.7855E+01  1.7855E+01  3.8101E-01  3.8101E-01  3.8101E-01
  1.0505E-03  1.7936E+01  1.7936E+01  1.7936E+01  3.8188E-01  3.8188E-01  3.8188E-01
  1.0707E-03  1.8024E+01  1.8024E+01  1.8024E+01  3.8281E-01  3.8281E-01  3.8281E-01
  1.0909E-03  1.8119E+01  1.8119E+01  1.8119E+01  3.8381E-01  3.8381E-01  3.8381E-01
  1.1111E-03  1.8221E+01  1.8221E+01  1.8221E+01  3.8489E-01  3.8489E-01  3.8489E-01
  1.1313E-03  1.8333E+01  1.8333E+01  1.8333E+01  3.8606E-01  3.8606E-01  3.8606E-01
  1.1515E-03  1.8454E+01  1.8454E+01  1.8454E+01  3.8732E-01  3.8732E-01  3.8732E-01
  1.1717E-03  1.8587E+01  1.8587E+01  1.8587E+01  3.8868E-01  3.8868E-01  3.8868E-01
  1.1919E-03  1.8733E+01  1.8733E+01  1.8733E+01  3.9017E-01  3.9017E-01  3.9017E-01
  1.2121E-03  1.8894E+01  1.8894E+01  1.8894E+01  3.9180E-01  3.9180E-01  3.9180E-01
  1.2323E-03  1.9072E+01  1.9072E+01  1.9072E+01  3.9358E-01  3.9358E-01  3.9358E-01
  1.2525E-03  1.9269E+01  1.9269E+01  1.9269E+01  3.9554E-01  3.9554E-01  3.9554E-01
  1.2727E-03  1.9491E+01  1.9491E+01  1.9491E+01  3.9771E-01  3.9771E-01  3.9771E-01
  1.2929E-03  1.9739E+01  1.9739E+01  1.9739E+01  4.0012E-01  4.0012E-01  4.0012E-01
  1.3131E-03  2.0022E+01  2.0022E+01  2.0022E+01  4.0281E-01  4.0281E-01  4.0281E-01
  1.3333E-03  2.0344E+01  2.0344E+01  2.0344E+01  4.0584E-01  4.0584E-01  4.0584E-01
  1.3535E-03  2.0716E+01  2.0716E+01  2.0716E+01  4.0926E-01  4.0926E-01  4.0926E-01
  1.3737E-03  2.1149E+01  2.1149E+01  2.1149E+01  4.1317E-01  4.1317E-01  4.1317E-01
  1.3939E-03  2.1660E+01  2.1660E+01  2.1660E+01  4.1767E-01  4.1767E-01  4.1767E-01
  1.4141E-03  2.2272E+01  2.2272E+01  2.2272E+01  4.2290E-01  4.2290E-01  4.2290E-01
  1.4343E-03  2.3018E+01  2.3018E+01  2.3018E+01  4.2907E-01  4.2907E-01  4.2907E-01
  1.4545E-03  2.3946E+01  2.3946E+01  2.3946E+01  4.3644E-01  4.3644E-01  4.3644E-01
  1.4747E-03  2.5132E+01  2.5132E+01  2.5132E+01  4.4542E-01  4.4542E-01  4.4542E-01
  1.4949E-03  2.6701E+01  2.6701E+01  2.6701E+01  4.5658E-01  4.5658E-01  4.5658E-01
  1.5152E-03  2.8873E+01  2.8873E+01  2.8873E+01  4.7086E-01  4.7086E-01  4.7086E-01
  1.5354E-03  3.2079E+01  3.2079E+01  3.2079E+01  4.8982E-01  4.8982E-01  4.8982E-01
  1.5556E-03  3.7283E+01  3.7283E+01  3.7283E+01  5.1631E-01  5.1631E-01  5.1631E-01
  1.5758E-03  4.7197E+01  4.7197E+01  4.7197E+01  5.5632E-01  5.5632E-01  5.5632E-01
  1.5960E-03  7.3487E+01  7.3487E+01  7.3487E+01  6.2579E-01  6.2579E-01  6.2579E-01
  1.6162E-03  3.4883E+02  3.4883E+02  3.4883E+02  8.0705E-01  8.0705E-01  8.0705E-01
  1.6364E-03 -7.3914E+01 -7.3914E+01 -7.3914E+01  1.0000E+00  1.0000E+00  1.0000E+00
  1.6566E-03 -2.4020E+01 -2.4020E+01 -2.4020E+01  1.0000E+00  1.0000E+00  1.0000E+00
  1.6768E-03 -9.9084E+00 -9.9084E+00 -9.9084E+00  1.0000E+00  1.0000E+00  1.0000E+00
  1.6970E-03 -3.2474E+00 -3.2474E+00 -3.2474E+00  1.0000E+00  1.0000E+00  1.0000E+00
  1.7172E-03  6.3065E-01  6.3065E-01  6.3065E-01  1.3166E-02  1.3166E-02  1.3166E-02
  1.7374E-03  3.1680E+00  3.1680E+00  3.1680E+00  7.8707E-02  7.8707E-02  7.8707E-02
  1.7576E-03  4.9571E+00  4.9571E+00  4.9571E+00  1.4450E-01  1.4450E-01  1.4450E-01
  1.7778E-03  6.2863E+00  6.2863E+00  6.2863E+00  1.8469E-01  1.8469E-01  1.8469E-01
  1.7980E-03  7.3124E+00  7.3124E+00  7.3124E+00  2.1166E-01  2.1166E-01  2.1166E-01
  1.8182E-03  8.1284E+00  8.1284E+00  8.1284E+00  2.3103E-01  2.3103E-01  2.3103E-01
  1.8384E-03  8.7927E+00  8.7927E+00  8.7927E+00  2.4564E-01  2.4564E-01  2.4564E-01
  1.8586E-03  9.3439E+00  9.3439E+00  9.3439E+00  2.5705E-01  2.5705E-01  2.5705E-01
  1.8788E-03  9.8085E+00  9.8085E+00  9.8085E+00  2.6621E-01  2.6621E-01  2.6621E-01
  1.8990E-03  1.0205E+01  1.0205E+01  1.0205E+01  2.7373E-01  2.7373E-01  2.7373E-01
  1.9192E-03  1.0548E+01  1.0548E+01  1.0548E+01  2.8002E-01  2.8002E-01  2.8002E-01
  1.9394E-03  1.0848E+01  1.0848E+01  1.0848E+01  2.8536E-01  2.8536E-01  2.8536E-01
  1.9596E-03  1.1111E+01  1.1111E+01  1.1111E+01  2.8994E-01  2.8994E-01  2.8994E-01
  1.9798E-03  1.1345E+01  1.1345E+01  1.1345E+01  2.9392E-01  2.9392E-01  2.9392E-01
  2.0000E-03  1.1553E+01  1.1553E+01  1.1553E+01  2.9741E-01  2.9741E-01  2.9741E-01

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

 Treat the second list of vectors 


  Phonon at Gamma, with non-analyticity in the
  direction (cartesian coordinates)  1.00000  0.00000  0.00000
 Phonon energies in Hartree :
   0.000000E+00  0.000000E+00  0.000000E+00  1.620427E-03  1.620427E-03
   1.713190E-03
 Phonon frequencies in cm-1    :
-  0.000000E+00  0.000000E+00  0.000000E+00  3.556426E+02  3.556426E+02
-  3.760017E+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 - absolute values smaller than 1.0d-7 are set to zero)
  Mode number    1   Energy    0.000000E+00
 Attention : low frequency mode.
   (Could be unstable or acoustic mode)
-  1  0.00000000E+00  0.00000000E+00 -2.32020398E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  0.00000000E+00 -2.32020414E-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 -2.32020398E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00 -2.32020414E-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  2.32020400E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  2.32020414E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    4   Energy    1.620427E-03
-  1  0.00000000E+00  0.00000000E+00  3.86630696E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  0.00000000E+00 -1.39237441E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    5   Energy    1.620427E-03
-  1  0.00000000E+00  3.86630696E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00 -1.39237441E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    6   Energy    1.713190E-03
;  1  3.86630695E-03  0.00000000E+00  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2 -1.39237442E-03  0.00000000E+00  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00

  Phonon at Gamma, with non-analyticity in the
  direction (cartesian coordinates)  0.00000  1.00000  0.00000
 Phonon energies in Hartree :
   0.000000E+00  0.000000E+00  0.000000E+00  1.620427E-03  1.620427E-03
   1.713190E-03
 Phonon frequencies in cm-1    :
-  0.000000E+00  0.000000E+00  0.000000E+00  3.556426E+02  3.556426E+02
-  3.760017E+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 - absolute values smaller than 1.0d-7 are set to zero)
  Mode number    1   Energy    0.000000E+00
 Attention : low frequency mode.
   (Could be unstable or acoustic mode)
-  1  0.00000000E+00  0.00000000E+00 -2.32020398E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  0.00000000E+00 -2.32020414E-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 -2.32020399E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00 -2.32020413E-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  2.32020398E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  2.32020414E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    4   Energy    1.620427E-03
-  1  0.00000000E+00  0.00000000E+00 -3.86630696E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  0.00000000E+00  1.39237441E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    5   Energy    1.620427E-03
-  1  3.86630696E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2 -1.39237441E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    6   Energy    1.713190E-03
;  1  0.00000000E+00  3.86630695E-03  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2  0.00000000E+00 -1.39237442E-03  0.00000000E+00
;     0.00000000E+00  0.00000000E+00  0.00000000E+00

  Phonon at Gamma, with non-analyticity in the
  direction (cartesian coordinates)  0.00000  0.00000  1.00000
 Phonon energies in Hartree :
   0.000000E+00  0.000000E+00  0.000000E+00  1.620427E-03  1.620427E-03
   1.713190E-03
 Phonon frequencies in cm-1    :
-  0.000000E+00  0.000000E+00  0.000000E+00  3.556426E+02  3.556426E+02
-  3.760017E+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 - absolute values smaller than 1.0d-7 are set to zero)
  Mode number    1   Energy    0.000000E+00
 Attention : low frequency mode.
   (Could be unstable or acoustic mode)
-  1  0.00000000E+00  0.00000000E+00 -2.32020399E-03
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  0.00000000E+00 -2.32020413E-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  2.32020398E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  0.00000000E+00  2.32020414E-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  2.32020398E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2  2.32020414E-03  0.00000000E+00  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    4   Energy    1.620427E-03
-  1  4.27070346E-07 -3.86630694E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2 -1.53800986E-07  1.39237441E-03  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    5   Energy    1.620427E-03
-  1  3.86630694E-03  4.27070346E-07  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
-  2 -1.39237441E-03 -1.53800986E-07  0.00000000E+00
-     0.00000000E+00  0.00000000E+00  0.00000000E+00
  Mode number    6   Energy    1.713190E-03
;  1  0.00000000E+00  0.00000000E+00  3.86630695E-03
;     0.00000000E+00  0.00000000E+00  0.00000000E+00
;  2  0.00000000E+00  0.00000000E+00 -1.39237442E-03
;     0.00000000E+00  0.00000000E+00  0.00000000E+00

 Generalized Lyddane-Sachs-Teller relation at zero frequency :
 Direction                     Dielectric constant
   1.00000   0.00000   0.00000     16.66342787
   0.00000   1.00000   0.00000     16.66342787
   0.00000   0.00000   1.00000     16.66342787
-
- Proc.   0 individual time (sec): cpu=          0.2  wall=          0.2

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

+Total cpu time      0.162  and wall time      0.179 sec

 anaddb : the run completed succesfully.