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    <div class="moz-cite-prefix">On 17/03/20 15:46, Paolo Giannozzi
      wrote:<br>
    </div>
    <blockquote type="cite"
cite="mid:CAPMgbCva_mOvL_1jWbc9P6gRbVhX_sNDSjCps7t0+2JpbFE4rQ@mail.gmail.com">
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        <div dir="ltr">On Mon, Mar 16, 2020 at 1:53 AM Shen, Ziheng <<a
            href="mailto:zshen83@gatech.edu" moz-do-not-send="true">zshen83@gatech.edu</a>>
          wrote:<br>
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                <div>1) May I ask is there any literature that can prove
                  it’s feasible to neglect the small frequencies? </div>
              </div>
            </div>
          </blockquote>
          <div><br>
          </div>
          <div>no idea, but you can easily verify whether the neglect of
            almost-zero frequencies has any effect: if you impose the
            ASR on dynamical matrices, only frequencies of translational
            modes (and of rotational ones for a molecule) should change,
            while all other frequencies should stay almost the same.<br>
          </div>
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                <div>2) I saw you also replied to others that “nat_todo”
                  does not make any sense, but there were still people
                  claimed that they got some useful results. I read from
                  some books (like the one written by D.Sholl) saying
                  that it’s possible to calculate only frequencies of
                  adsorbates which could save computational resources.
                  Some other ab initial calculation software (like VASP)
                  also have similar functions to calculate adsorbates
                  only. Why is “nat_todo” not working here? 
                </div>
              </div>
            </div>
          </blockquote>
          <div><br>
          </div>
          <div>Presumably it doesn't work because it is not sufficient
            to just ignore all surface atoms and compute the dynamical
            matrix restricted to adsorbate atoms only. I guess there are
            tricks to approximated phonons for an adsorbate on a surface
            by computing a  "reduced" dynamical matrix for the adsorbate
            only, in which the information on the adsorbate-surface
            interactions is "refolded",  but I don't know any. This same
            question has been asked over and over again in the list and
            nobody (that I remember) ever gave an answer. <br>
          </div>
          <div><br>
            <div>Paolo<br>
            </div>
            <div><br>
            </div>
          </div>
        </div>
      </div>
    </blockquote>
    <p>I think that if you have light atoms adsorbed on some heavier
      material and are looking for the adsorbate related frequencies
      then you can diagonalize the reduced matrix and the frequencies
      that you obtain should be variational upper bounds to the real
      ones....<br>
    </p>
    <p>just pretend you computed the whole matrix but restrict the
      atomic motion to a subset of atoms... so to the extent the modes
      are localized on the adsorbate with little involvement of the
      substrate you should be ok...</p>
    <p>but the low lying frequencies (the ones resonant with the
      substrate modes) will be completely wrong. </p>
    <p><br>
    </p>
    <p>one could start with nat_todo equal to just the adsorbate and
      then the first shell, then the second one ... and see  how things
      converge ...</p>
    <p>another option (better, but would need some ad hoc coding) would
      be to build the dynmat of the nat_todo atoms with interatomic
      force constants for the rest of the cell borrowed from some model
      (the bulk, or the clean surface) ... and again monitor the
      convergence as you include more and more shells  of atoms in the
      nat_todo.</p>
    <p><br>
    </p>
    <p>stefano<br>
    </p>
    <p><br>
    </p>
    <p><br>
    </p>
    <blockquote type="cite"
cite="mid:CAPMgbCva_mOvL_1jWbc9P6gRbVhX_sNDSjCps7t0+2JpbFE4rQ@mail.gmail.com">
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                  <div
                    style="margin:0px;font-stretch:normal;line-height:normal">Best
                    regards</div>
                  <div
                    style="margin:0px;font-stretch:normal;line-height:normal">Ziheng
                    Shen</div>
                  <div
                    style="margin:0px;font-stretch:normal;line-height:normal">PhD
                    student @ Georgia Institute of Technology</div>
                  <div
                    style="margin:0px;font-stretch:normal;line-height:normal"><br>
                  </div>
                  <blockquote type="cite">
                    <div>On Mar 15, 2020, at 7:00 AM, <a
                        href="mailto:users-request@lists.quantum-espresso.org"
                        target="_blank" moz-do-not-send="true">
                        users-request@lists.quantum-espresso.org</a>
                      wrote:</div>
                    <br>
                    <div><span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">On
                        Fri, Mar 13, 2020 at 4:22 AM Shen, Ziheng <</span><a
                        href="mailto:zshen83@gatech.edu"
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px"
                        target="_blank" moz-do-not-send="true">zshen83@gatech.edu</a><span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">>
                        wrote:</span><br
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                      <br
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                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">1)
                        When doing frequency analysis for molecules, I
                        expected to get zero or</span><br
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none">
                      <blockquote type="cite"
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none">extremely
                        small value for the first six frequencies (i.e.
                        translational &<br>
                        rotational modes). According to suggestions from
                        those previously posted<br>
                        problems, I tried to apply more restrict
                        convergence thresholds and ASR. It<br>
                        seems that ASR help a lot to reduce the number.
                        But I still got frequencies<br>
                        at ~50 level. Is it possible to completely
                        remove those small values? Or<br>
                        are those values small enough to be neglected?<br>
                        <br>
                      </blockquote>
                      <br
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none">
                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">They
                        are small enough to be neglected. They can be
                        removed by applying the</span><br
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none">
                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">ASR
                        to the computed dynamical matrix. See the
                        various kinds of ASR in codes</span><br
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                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">"dynmat"
                        and "matdyn", in particular the "zero-dim" one.
                        Note that  more</span><br
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                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">sophisticated
                        ASR than "simple" can be surprising slow.</span><br
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                      <br
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none">
                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">2)
                        My ultimate goal is to perform frequency
                        analysis for adsorbate so that</span><br
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                      <blockquote type="cite"
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none">I
                        can both determine transition state structures
                        and apply ZPE corrections.<br>
                        I tried to use ?nat_todo? to fix the surface
                        atoms and only did calculation<br>
                        for adsorbate (CH in my case). I got crazy
                        result (~10000 cm-1) when using<br>
                        large tr2_ph, and got improved results when I
                        decrease the threshold. But I<br>
                        still got fairly large translational &
                        rotational frequencies like below<br>
                        <br>
                      </blockquote>
                      <br
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                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">I
                        don't think you will obtain anything sensible by
                        fixing the surface atoms</span><br
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                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">and
                        making the calculation for the adsorbate atoms
                         only</span><br
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                      <br
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none">
                      <span
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none;float:none;display:inline">Paolo</span><br
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                      <br
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                      <br
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                      <blockquote type="cite"
style="font-family:Helvetica;font-size:12px;font-style:normal;font-variant-caps:normal;font-weight:normal;letter-spacing:normal;text-align:start;text-indent:0px;text-transform:none;white-space:normal;word-spacing:0px;text-decoration:none"><br>
                         freq (    1) =     -25.618746 [THz] =
                           -854.549399 [cm-1]<br>
                            freq (    2) =      -7.333895 [THz] =
                           -244.632409 [cm-1]<br>
                            freq (    3) =      -6.696884 [THz] =
                           -223.383991 [cm-1]<br>
                            freq (    4) =      -6.248674 [THz] =
                           -208.433322 [cm-1]<br>
                            freq (    5) =      -4.947831 [THz] =
                           -165.041892 [cm-1]<br>
                            freq (    6) =      -2.014699 [THz] =
                            -67.203109 [cm-1]<br>
                            freq (   37) =       0.571458 [THz] =
                             19.061786 [cm-1]<br>
                            freq (   38) =       5.754719 [THz] =
                            191.956759 [cm-1]<br>
                            freq (   39) =      16.488930 [THz] =
                            550.011494 [cm-1]<br>
                            freq (   40) =      16.563150 [THz] =
                            552.487199 [cm-1]<br>
                            freq (   41) =      18.255969 [THz] =
                            608.953585 [cm-1]<br>
                            freq (   42) =      56.121326 [THz] =
                           1872.005923 [cm-1]<br>
                        <br>
                        What does negative translational frequencies
                        indicate, is it possible to<br>
                        eliminate these imaginary numbers (like using
                        more restrict threshold)?<br>
                        And does my result indicate that my structure is
                        most probably not a<br>
                        transition state since all the other frequencies
                        are positive?<br>
                        <br>
                        I?m attaching the input file of pw.x &ph.x
                        below:<br>
                        =========================scf input, structure
                        obtained from<br>
                        neb.x========================<br>
                        &CONTROL<br>
                         Calculation='scf',<br>
                         restart_mode='from_scratch',<br>
                         prefix         = "Ni_ch_ts"<br>
                         outdir         = "./ts/tmp",<br>
                         pseudo_dir     = "./pseudo",<br>
                         tstress        = .true.<br>
                         verbosity      = 'high'<br>
                         tefield      = .true.<br>
                         dipfield     = .true.<br>
                        /<br>
                        &SYSTEM<br>
                         ibrav                  = 0,<br>
                         nat                    = 14,<br>
                         ntyp                   = 3,<br>
                         ecutwfc                = 65,<br>
                         ecutrho                = 650,<br>
                         Occupations='smearing',<br>
                         smearing='mp',<br>
                         degauss=0.01,<br>
                         nspin=2,<br>
                         starting_magnetization(1)=0.2,<br>
                         eamp        = 0.0<br>
                         edir        = 3<br>
                         emaxpos     = 0.95<br>
                         eopreg      = 0.05<br>
                        /<br>
                        &ELECTRONS<br>
                         electron_maxstep=250,<br>
                         conv_thr    = 1.D-10,<br>
                         mixing_beta = 0.1,<br>
                        /<br>
                        <br>
                        ATOMIC_SPECIES<br>
                        Ni 58.69 ni_pbe_v1.4.uspp.F.UPF<br>
                        C  12    C.pbe-n-kjpaw_psl.1.0.0.UPF<br>
                        H  1     H.pbe-kjpaw_psl.1.0.0.UPF<br>
                        CELL_PARAMETERS { angstrom }<br>
                        <br>
                               4.9667177200         0.0000000000
                                0.0000000000<br>
                               2.4833588600         4.3013037190
                                0.0000000000<br>
                               0.0000000000         0.0000000000
                                20.000000000<br>
                        <br>
                        ATOMIC_POSITIONS { angstrom }<br>
                        Ni    0.0000000000    0.0000000000
                           7.9723500000<br>
                        Ni    1.2416800000    2.1506500000
                           7.9723500000<br>
                        Ni    2.4833600000    0.0000000000
                           7.9723500000<br>
                        Ni    3.7250400000    2.1506500000
                           7.9723500000<br>
                        Ni    2.4833600000    1.4337700000
                          10.0000000000<br>
                        Ni    3.7250400000    3.5844200000
                          10.0000000000<br>
                        Ni    4.9667200000    1.4337700000
                          10.0000000000<br>
                        Ni    6.2084000000    3.5844200000
                          10.0000000000<br>
                        Ni    1.2281125212    0.7413038538
                          12.1124602290<br>
                        Ni    2.4833613443    2.9495126082
                          12.0722664849<br>
                        Ni    3.7386101535    0.7413040204
                          12.1124604793<br>
                        Ni    4.9667205066    2.8946406480
                          11.9560276983<br>
                        C    2.4833610952    1.4972020489
                          13.1166864267<br>
                        H    2.4833559794    3.1940064219
                          13.5465576823<br>
                        <br>
                        K_POINTS { automatic }<br>
                        6 6 1 0 0 0<br>
                        <br>
                        =======================================ph.x<br>
                        input=======================================<br>
                        phonons of CH on metal Ni at Gamma<br>
                        &inputph<br>
                        tr2_ph=1.0d-16,<br>
                        prefix='Ni_ch_ts',<br>
                        epsil=.false.,<br>
                        amass(1)=58.69,<br>
                        amass(2)=12.011,<br>
                        amass(3)=1.0,<br>
                        alpha_mix(1)=0.1,<br>
                        outdir='./tmp/',<br>
                        fildyn='CH.dynG',<br>
                        nat_todo= 2,<br>
                        /<br>
                        0.0 0.0 0.0<br>
                        13 14<br>
                        <br>
                        <br>
                        Thanks in advance for anyone that could give
                        suggestions to me!<br>
                        <br>
                        Best regards<br>
                        Ziheng Shen<br>
                        PhD student @ Georgia Institute of Technology</blockquote>
                    </div>
                  </blockquote>
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                <div>Paolo Giannozzi, Dip. Scienze Matematiche
                  Informatiche e Fisiche,<br>
                  Univ. Udine, via delle Scienze 208, 33100 Udine, Italy<br>
                  Phone +39-0432-558216, fax +39-0432-558222<br>
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      <pre class="moz-quote-pre" wrap="">_______________________________________________
Quantum ESPRESSO is supported by MaX (<a class="moz-txt-link-abbreviated" href="http://www.max-centre.eu/quantum-espresso">www.max-centre.eu/quantum-espresso</a>)
users mailing list <a class="moz-txt-link-abbreviated" href="mailto:users@lists.quantum-espresso.org">users@lists.quantum-espresso.org</a>
<a class="moz-txt-link-freetext" href="https://lists.quantum-espresso.org/mailman/listinfo/users">https://lists.quantum-espresso.org/mailman/listinfo/users</a></pre>
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