[QE-users] Phonons on a flat potential energy surface
Tamas Karpati
tkarpati at gmail.com
Fri Oct 29 19:58:41 CEST 2021
Dear Antoine Jay,
I think that in case of multiple imaginary eigenvalues the lower
energy of a conformer
may be less indicative. On the other hand, frozen phonons might be
both needed and to be avoided,
unless you consider a sufficient number of surrounding atoms. Have you
checked if inclusion
of more atoms helps the imaginaries fade away? Did you try to toss O where the
imaginary eigenvectors suggest? This way imaginaries can be sorted out
one after the other
(lucky ones get rid of them at once :)
Hope this helps,
t
On Fri, Oct 29, 2021 at 10:10 AM Antoine Jay <ajay at laas.fr> wrote:
>
> Dear users,
> I would like to perform a phonon calculation at Gamma on a 216-atoms crystalline silicon supercell in which has been added 1 single oxygen (PBE functional).
> This interstitial O is located 'nearly' in the middle of two Si, and unfortunately, many local minima are possible for its position: C2, C1, C1h, D3d, each of them being separated by a very small energy barrier and a small distance as already shown in Countinho-2000:
> https://sci-hub.mksa.top/10.1103/physrevb.62.10824
>
> When I calculate phonons of the C1h (that has the smallest energy) within DFPT, I obtain imaginary eigenvalues in the dynamical matrix.
> Of course, when I look at the corresponding eigenvectors, I see that they are exactly located on the O.
> Then I manually do a frozen phonon calculation using a displacement equal to the eigenvector and I see a positive curvature of the parabola meaning that the system is well at a minimum.
> Increasing the size of the displacement in my Frozen phonon permits me to see the double minima switching between C2 and C1h.
> I suppose that the size of the perturbation in DFPT is too high...? Where can I change it is the code?
>
> Best regards,
>
> Antoine Jay
>
>
> Inputs in attachment
> Results:
> Forces are over converged: Total force = 0.00049 Ry/au
> Frequencies after DFPT are these
> freq ( 1- 1) = -118.6 [cm-1] --> ?
> freq ( 2- 2) = -114.5 [cm-1] --> ?
> freq ( 3- 3) = -99.2 [cm-1] --> ?
> freq ( 4- 4) = -38.0 [cm-1] --> ?
> freq ( 5- 5) = -37.7 [cm-1] --> ?
> freq ( 6- 6) = -37.7 [cm-1] --> ?
> freq ( 7- 7) = 87.7 [cm-1] --> A' I+R
> freq ( 8- 8) = 91.5 [cm-1] --> A' I+R
> freq ( 9- 9) = 91.8 [cm-1] --> A'' I+R
>
> and after simple ASR:
> # mode [cm-1] [THz] IR
> 1 -107.94 -3.2359 0.0000
> 2 -38.83 -1.1640 0.0000
> 3 -10.69 -0.3206 0.0000
> 4 -2.67 -0.0801 0.0000
> 5 8.82 0.2643 0.0000
> 6 29.09 0.8720 0.0000
> 7 97.81 2.9324 0.0000
> 8 98.94 2.9661 0.0000
> 9 98.97 2.9670 0.0000 _______________________________________________
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