<div class="gmail_quote"><blockquote class="gmail_quote" style="border-left: 1px solid rgb(204, 204, 204); margin: 0pt 0pt 0pt 0.8ex; padding-left: 1ex;">Dear Dr. Stefano and Dr. Mohr,</blockquote><div><br>Thank you for your  comments,
<br><br>Actually I had successfully  done  phonon dispersion and  EPC  for Al bulk structure with  good  results so from now I want to apply for the Al wires  structures. Firstly I calculate for 2 atom cell of Al with zigzag wires, and I got 6 phonon modes along q-points and appear some negative frequencies, so I tried to improve my calculation but always appear negative acoustic frequencies (optical branch is no problem) and then I did with 4, 6 atom cell and of course I got 3-n modes but my results still no good like I expect. :(
<br>To check my set up parameters I calculate the same procedure for Al 1D linear chain with 1 and 2 atom cell with hopefully the phonon curves will be the same as I studied theoretically in Solid States books, but it was not :(. So should my calculation be wrong with this system. Could you give me advice about my input parameters? Please keep your eyes my INPUT files (in case of 2 atoms in zigzag chain)
<br><br><a href="http://Al.scf.fit.in">Al.scf.fit.in</a><br><br> &SYSTEM                                               <br>                       ibrav = 6,                      <br>                 celldm(1) = 39.994
,                   <br>                   celldm(3) =  0.199762906,           <br>                         nat = 2,                      <br>                        ntyp = 1,                      <br>                     ecutwfc = 
25.D0 ,                 <br>                     ecutrho = 300,                    <br>                 occupations = 'smearing' ,            <br>                     degauss = 0.05 ,                  <br>                    smearing = 'methfessel-paxton' ,   
<br>                      la2F = .true.                    <br> /                                                     <br> &ELECTRONS                                            <br>                    conv_thr = 1.D-10
 ,                <br>                 mixing_beta = 0.7D0 ,                 <br> /                                                     <br>ATOMIC_SPECIES                                         <br>   Al   26.98000  Al.vbc.UPF
                           <br>ATOMIC_POSITIONS angstrom                              <br>Al       0.000000000   1.517315647   2.138739361       <br>Al       0.000000000   0.116702849   0.023699809       <br>K_POINTS automatic                                     
<br>  4 4 40   0 0 0       <br><br><a href="http://Al.scf.in">Al.scf.in</a><br><br> &SYSTEM                                           <br>                       ibrav = 6,                  <br>                 celldm(1) = 
39.994,               <br>                   celldm(3) =  0.199762906,       <br>                         nat = 2,                  <br>                        ntyp = 1,                  <br>                     ecutwfc = 
25.D0 ,             <br>                     ecutrho = 300,                <br>                 occupations = 'smearing' ,        <br>                     degauss = 0.05 ,              <br>                    smearing = 'methfessel-paxton' 
<br> /                                                 <br> &ELECTRONS                                        <br>                    conv_thr = 1.D-10 ,            <br>                 mixing_beta = 0.7D0 ,             
<br> /                                                 <br>ATOMIC_SPECIES                                     <br>   Al   26.98000  Al.vbc.UPF                       <br>ATOMIC_POSITIONS angstrom                          <br>
Al       0.000000000   1.517315647   2.138739361   <br>Al       0.000000000   0.116702849   0.023699809   <br>K_POINTS automatic                                 <br>  2 2 20   0 0 0     <br><br><a href="http://Al.elph.in">
Al.elph.in</a><br><br>Electron-phonon coefficients for Alwire_2         <br> &inputph                                         <br>  tr2_ph=1.0d-14,                                 <br>  prefix='al2_elph',                              
<br>  fildvscf='al2d',                                <br>  filelph='matrix'                                <br>  amass(1)=26.98,                                 <br>  outdir='/root/tmp/',                            
<br>  fildyn='al2m.dyn',                              <br>  elph=.true.,                                    <br>  trans=.true.,                                   <br>  ldisp=.true.                                    
<br>  nq1=1, nq2=1, nq3=10,<br><br>And hereafter 6 modes I got<br><br> &plot nbnd=   6, nks=  27 /                                 <br>            0.000000  0.000000  0.000000                     <br>   -0.0855   -0.0450
    0.0000   20.7938  196.2309  372.4942 <br>            0.000000  0.000000  0.100000                     <br>  -13.1432    5.6657    5.7114   20.3098  196.7060  372.0899 <br>            0.000000  0.000000  0.200000                     
<br>  -25.6753   10.2550   10.5805   18.8468  198.1533  371.0008 <br>            0.000000  0.000000  0.300000                     <br>  -37.6999   14.0728   14.1858   16.2544  200.5950  369.4869 <br>            0.000000  
0.000000  0.400000                     <br>  -48.8295   11.6034   16.4265   16.4576  203.9728  367.7201 <br>            0.000000  0.000000  0.500000                     <br>  -58.7192   -5.6944   16.7453   17.6129  208.1190
  365.6663 <br>            0.000000  0.000000  0.600000                     <br>  -67.0895  -15.3952   14.9673   18.4203  212.8051  363.1793 <br>            0.000000  0.000000  0.700000                     <br>  -73.7443  -
21.7038   11.9605   19.3942  217.8126  360.1938 <br>            0.000000  0.000000  0.800000                     <br>  -78.6120  -26.9948    9.8326   20.4642  222.9635  356.8134 <br>            0.000000  0.000000  0.900000
                     <br>  -81.7857  -31.7595   10.1665   21.2176  228.1041  353.2106 <br>            0.000000  0.000000  1.000000                     <br>  -83.4878  -36.1149   10.5785   21.4924  233.0809  349.4591 <br>            
0.000000  0.000000  1.100000                     <br>  -83.9637  -39.9380    6.4409   21.5912  237.7521  345.4939 <br>            0.000000  0.000000  1.200000                     <br>  -83.3549  -43.0700  -11.8614   21.8643
  242.0400  341.2345 <br>            0.000000  0.000000  1.300000                     <br>  -81.7148  -45.5109  -19.5363   22.1233  245.9755  336.7214 <br>            0.000000  0.000000  1.400000                     <br>  -
79.2450  -47.4002  -24.2602   21.7049  249.6731  332.1110 <br>            0.000000  0.000000  1.500000                     <br>  -76.4698  -48.7989  -26.8527   20.1426  253.2412  327.5276 <br>            0.000000  0.000000
  1.600000                     <br>  -74.0708  -49.5494  -28.8342   17.6459  256.7020  322.9460 <br>            0.000000  0.000000  1.700000                     <br>  -72.4259  -49.4368  -31.6947   14.8469  259.9856  318.2672
 <br>            0.000000  0.000000  1.800000                     <br>  -71.2114  -48.4948  -35.6608   11.6256  263.0044  313.5063 <br>            0.000000  0.000000  1.900000                     <br>  -69.6799  -47.0750  -
39.7963    4.2536  265.7429  308.8670 <br>            0.000000  0.000000  2.000000                     <br>  -67.4586  -45.5010  -43.2503  -12.7026  268.2849  304.5960 <br>            0.000000  0.000000  2.100000                     
<br>  -64.9647  -46.1360  -43.6300  -19.3793  270.7903  300.7406 <br>            0.000000  0.000000  2.200000                     <br>  -63.0506  -49.2247  -40.9136  -23.4729  273.4711  297.0578 <br>            0.000000  
0.000000  2.300000                     <br>  -62.1609  -52.8376  -37.0315  -25.3558  276.5514  293.2015 <br>            0.000000  0.000000  2.400000                     <br>  -61.8563  -56.2311  -32.5370  -26.2996  280.1674
  289.0264 <br>            0.000000  0.000000  2.500000                     <br>  -61.6387  -57.8617  -29.3445  -27.6304  283.8161  285.1565 <br>            0.000000  0.000000  2.503000                     <br>  -61.6384  -
57.8633  -29.3391  -27.6341  283.8284  285.1440 <br><br><br>   Bac, <br><br><pre>------------------------------<br>Phung Viet Bac<br>Division of Mathematical and Physical Science,<br>Graduate School of Natural Science and Technology,
<br>Kanazawa University,<br>Kakuma, Kanazawa 920-1192, JAPAN</pre><br>                              <br>                                <br><br><br><br></div><blockquote class="gmail_quote" style="border-left: 1px solid rgb(204, 204, 204); margin: 0pt 0pt 0pt 0.8ex; padding-left: 1ex;">
<br><br>your phonon branches are really strange...<br>with two atoms I would expect 6 modes per each q-point<br><br>stefano<br><br><br><br>6 branches for 2 atom are what one expects (in general 3n branches and 3<br>acoustical and 3n-3 optical ones).
<br><br>However negative values indicate some error in your calculation, dependent<br>on the magnitude and system.<br>You can impose some sum-rules for the acoustic ones, to force them to be<br>0 at the Gamma point.<br><br>
Acoustic forces are harder to calculate (smaller forces). In your case I<br>would guess up to 15 cm^1 should be ok for the acoustic ones.<br>Negative optical ones should not occur.<br><br>Best<br>Marcel Mohr<br><br><br></blockquote>
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