[QE-users] Acoustic Sum Rule Frequency Question

Tang, Weilun [M S E] weilunt at iastate.edu
Sat Nov 1 20:10:20 CET 2025


Dear. Dr. Giannozzi,

Thank you very much for your reply and your time.

I came across a post that you mentioned low frequency modes tend to have sizable admixture. Is 441.1 cm-1 considered in the low frequency range?

I have a question about structure relaxation for a charged system. Currently, I use A = B = 17.2 A and C = 10. I found that when I increase the size of the unit cell, such as A = B = 18 A and C = 10, the structure relaxation didn't converge, but I didn't have this issue with netural charge system. Is there anything I should be careful when deaing with charged system?

Additional, I checked my calculation for other molecules, and compare before and after acoustic sum rule. They all have the similar behavior: high frequency modes have very little changes. In the medium frequency region, one or two modes have a significant shift in frequency. Below is another example as a reference. I noticed that  510.0 cm-1 seems to be shifted up to 750.02 cm-1 after acoustic sum rule.

------------------------------------------------------ output from ph.x
     Mode symmetry, C_3h (-6)   point group:

         freq (   1-   1) =         49.3  [cm-1]   --> A'              R
         freq (   2-   2) =         61.2  [cm-1]   --> E''             R
         freq (   3-   3) =         61.2  [cm-1]   --> E''*            R
        freq (   4-   4) =        104.0  [cm-1]   --> A''             I
        freq (   5-   5) =        154.3  [cm-1]   --> E'              I+R
        freq (   6-   6) =        154.3  [cm-1]   --> E'*             I+R
        freq (   7-   7) =        176.8  [cm-1]   --> E''             R
        freq (   8-   8) =        176.8  [cm-1]   --> E''*            R
        freq (   9-   9) =        183.5  [cm-1]   --> E'              I+R
        freq (  10-  10) =        183.5  [cm-1]   --> E'*             I+R
        freq (  11-  11) =        311.8  [cm-1]   --> A''             I
        freq (  12-  12) =        376.2  [cm-1]   --> A'              R
        freq (  13-  13) =        386.9  [cm-1]   --> E''             R
        freq (  14-  14) =        386.9  [cm-1]   --> E''*            R
        freq (  15-  15) =        401.7  [cm-1]   --> A'              R
        freq (  16-  16) =        435.4  [cm-1]   --> E'              I+R
        freq (  17-  17) =        435.4  [cm-1]   --> E'*             I+R
        freq (  18-  18) =        510.0  [cm-1]   --> A''             I
        freq (  19-  19) =        638.5  [cm-1]   --> E''             R
        freq (  20-  20) =        638.5  [cm-1]   --> E''*            R
        freq (  21-  21) =        790.4  [cm-1]   --> A''             I
        freq (  22-  22) =        823.7  [cm-1]   --> E'              I+R
        freq (  23-  23) =        823.7  [cm-1]   --> E'*             I+R
        freq (  24-  24) =        883.8  [cm-1]   --> E'              I+R
        freq (  25-  25) =        883.8  [cm-1]   --> E'*             I+R
        freq (  26-  26) =        908.0  [cm-1]   --> A'              R
        freq (  27-  27) =        949.2  [cm-1]   --> A'              R
        freq (  28-  28) =       1208.3  [cm-1]   --> A'              R
        freq (  29-  29) =       1265.0  [cm-1]   --> E'              I+R
        freq (  30-  30) =       1265.0  [cm-1]   --> E'*             I+R
        freq (  31-  31) =       1277.9  [cm-1]   --> A'              R
        freq (  32-  32) =       1464.3  [cm-1]   --> E'              I+R
        freq (  33-  33) =       1464.3  [cm-1]   --> E'*             I+R
        freq (  34-  34) =       2581.4  [cm-1]   --> E'              I+R
        freq (  35-  35) =       2581.4  [cm-1]   --> E'*             I+R
        freq (  36-  36) =       2588.7  [cm-1]   --> A'              R
--------------------------------------------------------------------------------- output from dynmat.x
# mode   [cm-1]    [THz]      IR          Raman   depol.fact
    1     -0.00   -0.0000    0.0000         3.5089    0.7500
    2     -0.00   -0.0000    0.0000         3.7711    0.7500
    3     -0.00   -0.0000    0.0000         0.4088    0.7500
    4      0.00    0.0000    0.0000         0.5258    0.7500
    5      0.00    0.0000    0.0000         1.1191    0.7500
    6      0.00    0.0000    0.0000         1.8734    0.7500
    7    110.68    3.3181    0.0000         0.1475    0.7500
    8    110.68    3.3181    0.0000         0.1475    0.7500
    9    149.03    4.4677    0.0023         0.0000    0.7500
   10    173.76    5.2092    0.0212         3.3877    0.7500
   11    173.76    5.2092    0.0212         3.3877    0.7500
   12    376.21   11.2784    0.0000        12.7649    0.0354
   13    403.42   12.0943    0.0000         8.2338    0.0521
   14    435.39   13.0525    0.0029         0.8795    0.7500
   15    435.39   13.0525    0.0029         0.8795    0.7500
   16    467.53   14.0163    0.0000         0.8370    0.7500
   17    467.54   14.0164    0.0000         0.8370    0.7500
   18    638.52   19.1422    0.0000         0.0197    0.7500
   19    638.52   19.1422    0.0000         0.0197    0.7500
   20    750.02   22.4850    0.0288         0.0000    0.7500
   21    796.81   23.8877    0.0669         0.0000    0.7500
   22    833.63   24.9916    2.3490         1.3092    0.7500
   23    833.63   24.9916    2.3490         1.3092    0.7500
   24    892.72   26.7630    0.3425         2.8335    0.7500
   25    892.72   26.7630    0.3425         2.8335    0.7500
   26    910.03   27.2821    0.0000        10.4788    0.0820
   27    949.01   28.4507    0.0000        36.9935    0.1382
   28   1208.38   36.2262    0.0000         0.6504    0.1090
   29   1265.06   37.9256    7.4876         0.6427    0.7500
   30   1265.06   37.9256    7.4876         0.6427    0.7500
   31   1277.95   38.3118    0.0000        11.7798    0.3737
   32   1465.41   43.9318   16.7623        12.2264    0.7500
   33   1465.41   43.9318   16.7623        12.2264    0.7500
   34   2586.09   77.5290    0.0000       314.9596    0.0756
   35   2586.97   77.5555    0.0932        32.8023    0.7500
   36   2586.97   77.5555    0.0932        32.8412    0.7485
------------------------------------------------------------------------------

Thank you very much again for your time,

Weilun Tang
________________________________
From: Paolo Giannozzi <paolo.giannozzi at uniud.it>
Sent: Saturday, November 1, 2025 10:34 AM
To: Quantum ESPRESSO users Forum <users at lists.quantum-espresso.org>
Cc: Tang, Weilun [M S E] <weilunt at iastate.edu>
Subject: Re: [QE-users] Acoustic Sum Rule Frequency Question

Maybe your 441 cm-1 mode has a large admixture of a rotational mode?
This may happen if the supercell is not large enough

Paolo

On 11/1/2025 12:55 AM, Tang, Weilun [M S E] via users wrote:
> Dear Quantum Espresso users,
>
> I made a phonon calculation for an isolated molecule using acoustic sum
> rule *asr='zero-dim'. *Then, I compared the phonon modes before and
> after applying the acoustic sum rule. I noticed that there is a mode
> that has a huge change in frequency, as shown below. More specifically,
> the *441.1 cm-1* mode seems to be shifted to *115.30 cm-1 *after
> applying the acoustic sum rule. Is this normal?
>
> For this calculation, I used lower threshold: forc_conv_thr = 1.0D-6,
> etot_conv_thr = 1.0D-6, conv_thr = 1.D-14 for pw.x. And for phx, I use
> tr2_ph=1.0d-18.
> -------------------------------------------------------------
> Below is phonon modes from ph.x:
>
>        Mode symmetry, D_3h (-62m) point group:
>          freq (   1-   1) =        -27.8  [cm-1]   --> A'_2
>          freq (   2-   3) =         65.6  [cm-1]   --> E''             R
>          freq (   4-   4) =        103.9  [cm-1]   --> A''2            I
>          freq (   5-   6) =        120.4  [cm-1]   --> E''             R
>          freq (   7-   8) =        146.2  [cm-1]   --> E'              I+R
>          freq (   9-  10) =        188.8  [cm-1]   --> E'              I+R
>          freq (  11-  11) =        367.1  [cm-1]   --> A'_1            R
>          freq (  12-  13) =        430.7  [cm-1]   --> E'              I+R
>          freq (  14-  14) =        441.1  [cm-1]   --> A''2            I
>          freq (  15-  15) =        461.4  [cm-1]   --> A'_2
>          freq (  16-  17) =        631.9  [cm-1]   --> E''             R
>          freq (  18-  18) =        776.4  [cm-1]   --> A''2            I
>          freq (  19-  20) =        801.0  [cm-1]   --> E'              I+R
>          freq (  21-  21) =        907.1  [cm-1]   --> A'_1            R
>          freq (  22-  22) =       1101.1  [cm-1]   --> A'_2
>          freq (  23-  24) =       1150.0  [cm-1]   --> E'              I+R
>          freq (  25-  25) =       1189.0  [cm-1]   --> A'_1            R
>          freq (  26-  27) =       1337.2  [cm-1]   --> E'              I+R
> ----------------------------------------------------------------
> Below is output from dynmat.x
>
>       Reading Dynamical Matrix from file dmat.ttc
>       ...Force constants read
>       ...epsilon and Z* read
>       ...Raman cross sections read
>       Acoustic Sum Rule: || Z*(ASR) - Z*(orig)|| =    1.029894E+00
>       Acoustic Sum Rule: ||dyn(ASR) - dyn(orig)||=    2.701556E-01
>       A direction for q was not specified:TO-LO splitting will be absent
>
>       Polarizability (A^3 units)
>       multiply by 0.759092 for Clausius-Mossotti correction
>         262.517180   -0.000000   -0.000000
>          -0.000000  262.517180   -0.000000
>           0.000000    0.000000   57.305445
>
>       IR activities are in (D/A)^2/amu units
>       Raman activities are in A^4/amu units
>       multiply Raman by 0.576221 for Clausius-Mossotti correction
>
> # mode   [cm-1]    [THz]      IR          Raman   depol.fact
>      1     -0.00   -0.0000    0.0000        16.3234    0.7500
>      2     -0.00   -0.0000    0.0000      3355.0146    0.7500
>      3     -0.00   -0.0000    0.0000      1478.4689    0.7500
>      4      0.00    0.0000    0.0000       285.5435    0.7500
>      5      0.00    0.0000    0.0000       873.4000    0.7500
>      6      0.00    0.0000    0.0000      1623.8289    0.7500
>      7     73.38    2.1998    0.0000       696.8190    0.7500
>      8     73.38    2.1998    0.0000       696.8152    0.7500
>      9    115.30    3.4567    0.2787         0.0000    0.7500
>     10    177.24    5.3134    1.7092     44473.2909    0.7500
>     11    177.24    5.3134    1.7092     44473.2914    0.7500
>     12    367.09   11.0050    0.0000  11288132.4685    0.1106
>     13    436.75   13.0934    0.2992      3721.4221    0.7500
>     14    436.75   13.0934    0.2992      3721.4231    0.7500
>     15    462.38   13.8617    0.0000         0.0004    0.7500
>     16    631.59   18.9347    0.0000     13677.2759    0.7500
>     17    631.59   18.9347    0.0000     13677.2842    0.7500
>     18    778.46   23.3377    0.0792         0.0000    0.7500
>     19    802.57   24.0605   12.9665   1800840.5786    0.7500
>     20    802.57   24.0605   12.9665   1800840.5109    0.7500
>     21    907.11   27.1945    0.0000   8355726.6168    0.1191
>     22   1101.10   33.0101    0.0000         0.0000    0.7500
>     23   1150.13   34.4801   26.2055  16251271.1703    0.7500
>     24   1150.13   34.4801   26.2055  16251270.4526    0.7500
>     25   1189.02   35.6458    0.0000     16979.5440    0.2674
>     26   1337.59   40.1000   27.2231  16068754.7864    0.7500
>     27   1337.59   40.1000   27.2231  16068754.1344    0.7500
>
> --------------------------------------------------------------------------------------------------------
> Below is my input file for pw.x
>
> &CONTROL
>    calculation  = "scf",
>    prefix       = "ttc",
>    pseudo_dir   = "/home/weilunt/pseudopotential/norm_conserving/pz",
>    outdir       = "./tmp",
>    forc_conv_thr = 1.0D-6,
>    etot_conv_thr = 1.0D-6,
>
> /
> &SYSTEM
>    assume_isolated = 'martyna-tuckerman',
>    ibrav     = 4,
>    A = 17.2,
>    C = 10,
>    nat       = 9,
>    ntyp      = 3,
>    ecutwfc   = 80.D0, !better 120
>    tot_charge = -3,
>    occupations = 'fixed',
> /
> &ELECTRONS
>    conv_thr    = 1.D-14,
>    mixing_beta = 0.7,
>    electron_maxstep = 200,
> /
> &IONS
> /
> ATOMIC_SPECIES
>    S 32.070  S.pz-hgh.UPF
>    N 14.007  N.pz-hgh.UPF
>    C 12.010  C.pz-hgh.UPF
> ATOMIC_POSITIONS (angstrom)
> S                0.0000000000       -3.0749791762       -0.0000000000
> S               -2.6627598154        1.5374395881       -0.0000000000
> S                2.6627598154        1.5374395881        0.0000000000
> N                1.1913527585       -0.6879250817       -0.0000000000
> N               -1.1913527585       -0.6879250817        0.0000000000
> N                0.0000000000        1.3757501635        0.0000000000
> C                0.0000000000       -1.3240902237       -0.0000000000
> C               -1.1466139383        0.6620951119        0.0000000000
> C                1.1466139383        0.6620951119        0.0000000000
> K_POINTS (automatic)
> 1 1 1 0 0 0
> -----------------------------------------------------------------------------------------
>
> Thank you for your time and your help in advance,
>
> Weilun Tang
>
>
>
> _______________________________________________________________________________
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> --------------------------------------------------------------------------------
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--
Paolo Giannozzi, Dip. Scienze Matematiche Informatiche e Fisiche,
Univ. Udine, via delle Scienze 206, 33100 Udine Italy, +39-0432-558216

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