Thank you very much Andrei.
Actually the 4th frequency is as close to zero as the 2nd and 3rd, and it
is positive (as it should be)

  eigenvalue #           1  omega=  -40.738952961112830
  eigenvalue #           2  omega= -2.05736482791876937E-002
  eigenvalue #           3  omega= -1.32180970904245670E-002
  eigenvalue #           4  omega=  1.02952404945284657E-002
  eigenvalue #           5  omega=   13.407523547356076

Maybe the problem is not the meshcutoff but the fact that, in the
relaxation, I keep fixed the 1st layer positions, so there was big forces
on some atoms. Now I am trying to recalculate the phonons after relaxing
all the atoms.
By the way, is there a standard threshold value to judge the goodness of
atomic forces?

Best regards,

Carlo



2012/4/7 <[email protected]>

> > Andrei,
> >
> > thank you very much for your answer. I had already found in the ML
> > database
> > the nice phonon reference you indicated to me.
> > By negative frequencies, I mean:
> >
> >   eigenvalue #           1  omega=  -40.738952961112830
> >   eigenvalue #           2  omega= -2.05736482791876937E-002
> >   eigenvalue #           3  omega= -1.32180970904245670E-002
>
> Dear Carlo,
> Your frequencies 2 and 3 are zero, for all practical use.
> No special importance therefore that they are negative.
> If you have yet the third frequency (positive, in your case?)
> which is as close to zero as those two (your Nr4?)
> then likely you don't have a problem with MeshCutoff.
> However, your frequency Nr1 is an indication
> that your relaxation is not good enough.
> The negative frequency (if a stable one and not due to numerical noise)
> means: as you displace the atoms in some combination, the energy
> goes down. It shouldn't be like this at the equilibrium.
> Have a look into p.18 of
> http://www.home.uni-osnabrueck.de/apostnik/Lectures/APostnikov-Phonons.pdf
>
> > My system is a molecular junction. Just to explain you, at the beginning
> I
> > calculated the electrodes bulk lattice parameter, and then I built the
> > junction geometry. If I then relax by setting MD.variableCell=T the cell
> > dimensions increase by 1.5%... Do you think that I should necessarily use
> > a variable cell in the relaxation? (I am suspicious about it)
>
> Not necessarily at all; you can calculate phonons
> in a constrained system, under pressure etc. However,
> atom positions have to be optimized subject to this constraint
> (to be sure that trial atom displacements are around the equilibrium).
>
> > Finally, could you please give me some reference about the eggbox effect
> > test?
>
> It has been discussed many many times in the main list and in tutorials.
> E.g., you may have a look in
> http://www.home.uni-osnabrueck.de/apostnik/Lectures/SIESTA-tuto.pdf
> (pp.10-12)
>
> Good luck
>
> Andrei Postnikov
>
> >
> > Thank you very much!
> >
> > Carlo
> >
> >
> > 2012/4/7 <[email protected]>
> >
> >> Dear Carlo,
> >> as you don't specify how negative your negative frequencies are,
> >> it is not so easy to judge... Your sum of forces seems a bit too high...
> >> Even if not dramatically... And some individual forces as well -
> >> e.g., Fx on atom 2. So generally I'd recommend even higher MeshCutoff
> >> and further relaxation. A priori 350 Ry is not safely high,
> >> sometimes one needs to go to much higher.
> >>
> >> Before doing the phonons, I'd recommend the usual "eggbox test"
> >> to be sure that fluctuations of summary force as function of
> >> uniform displacement of all atoms remain within |0.1|.
> >>
> >> Concerning specifically the phonons, you may wish to check
> >>
> http://www.home.uni-osnabrueck.de/apostnik/Lectures/APostnikov-Phonons.pdf
> >> - especially p.18 of it.
> >>
> >> Best regards
> >>
> >> Andrei Postnikov
> >>
> >>
> >> > Dear Siesta users,
> >> >
> >> > I am trying to calculate phonon frequencies at Gamma for a molecular
> >> > junction.
> >> > I relaxed the system by keeping fixed the Lattice Vectors (not a
> >> variable
> >> > cell). When I compute the frequencies (with MeshCutoff = 200 Ry), I
> >> obtain
> >> > that the first three frequencies are negative, which indicates that
> >> the
> >> > results are not correct.
> >> > Then, if I increase the MeshCutoff to 350 Ry (which seems a high value
> >> to
> >> > me) I obtain again negative frequencies.
> >> > Could you suggest me how to fix the problem?
> >> > The following are the forces of the system...do you think that they
> >> are
> >> > too
> >> > high? Which is a good criteria to say that the forces are low enough?
> >> >
> >> > Thank you very much,
> >> >
> >> > Carlo
> >> >
> >> > siesta:      1    0.106233   -0.096180    0.047641
> >> > siesta:      2   -0.655838    0.034936   -0.004086
> >> > siesta:      3    0.364736   -0.100368    0.166114
> >> > siesta:      4    0.130690    0.010500   -0.101584
> >> > siesta:      5   -0.122410    0.420815   -0.012044
> >> > siesta:      6    0.120625   -0.031292    0.152270
> >> > siesta:      7    0.003319    0.004051   -0.012274
> >> > siesta:      8    0.004951   -0.015719    0.001451
> >> > siesta:      9   -0.009523    0.004610    0.013162
> >> > siesta:     10    0.019411   -0.008606   -0.009840
> >> > siesta:     11    0.002485   -0.010131    0.005577
> >> > siesta:     12    0.001815   -0.012882   -0.010601
> >> > siesta:     13    0.002293   -0.027828    0.004317
> >> > siesta:     14    0.003541   -0.004099   -0.003595
> >> > siesta:     15   -0.004545   -0.005597    0.018501
> >> > siesta:     16   -0.002375    0.005693   -0.016887
> >> > siesta:     17    0.007410   -0.017539   -0.001118
> >> > siesta:     18    0.015827   -0.012960   -0.005705
> >> > siesta:     19   -0.010629   -0.007460   -0.001509
> >> > siesta:     20    0.008748    0.000683   -0.004698
> >> > siesta:     21   -0.004943    0.029703   -0.008064
> >> > siesta:     22   -0.003202    0.004500    0.030359
> >> > siesta:     23   -0.009982   -0.003884   -0.044988
> >> > siesta:     24    0.012110   -0.008463   -0.054600
> >> > siesta:     25    0.014891    0.000114    0.030375
> >> > siesta:     26    0.011714    0.007854   -0.002981
> >> > siesta:     27   -0.006905   -0.024651    0.005841
> >> > siesta:     28    0.002399   -0.019318    0.013282
> >> > siesta:     29   -0.019852    0.006114   -0.030653
> >> > siesta:     30   -0.023687    0.004007   -0.028044
> >> > siesta:     31    0.023195   -0.022556   -0.014991
> >> > siesta:     32    0.024333   -0.033430   -0.028258
> >> > siesta:     33   -0.014937    0.006378    0.009843
> >> > siesta:     34    0.004912   -0.019004   -0.008074
> >> > siesta:     35    0.006259   -0.012323    0.009612
> >> > siesta:     36   -0.010453    0.017222    0.013853
> >> > siesta:     37    0.001281    0.001284   -0.002971
> >> > siesta:     38    0.009564    0.017869   -0.013170
> >> > siesta:     39    0.004626   -0.016715   -0.008634
> >> > siesta:     40    0.008447   -0.028871   -0.007756
> >> > siesta:     41   -0.020042   -0.027721   -0.021694
> >> > siesta:     42    0.020027   -0.019833   -0.095505
> >> > siesta: ----------------------------------------
> >> > siesta:    Tot    0.016519   -0.011098   -0.032128
> >> >
> >> >
> >> > --
> >> >
> >> > Carlo Motta
> >> > * Ph.D. Student in Materials Science*
> >> > University Office Phone : +39 02 6448-5183
> >> > Department of Materials Science
> >> > University of Milano-Bicocca
> >> > Via R. Cozzi 53, 20125  Milano,  Italy
> >> >
> >>
> >>
> >
>
>


-- 

Carlo Motta
* Ph.D. Student in Materials Science*
Email: [email protected]
University Office Phone : +39 02 6448-5183
Department of Materials Science
University of Milano-Bicocca
Via R. Cozzi 53, 20125  Milano,  Italy

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