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    <div class="moz-cite-prefix">Dear Vikan,<br>
      I dont have direct experience on this problem. here a few things i
      would look into:<br>
      <br>
      from your NEB calculation around the TS you should be able to see
      what the unstable mode is expected to look like and how many atoms
      are involved.<br>
      If you compute interatomic force constants (IFC) only around a
      subset of the atoms there is the problem of how you impose the
      acoustic sum rule. <br>
      One way would be to complete your DynMat using the IFC of the bulk
      material (that you could compute separately), and impose ASR on
      this model. <br>
      To stay on the safe side you could set the mass of the atoms that
      you did not compute to a very large number so they do not move. <br>
      <br>
      stefano<br>
      <br>
      <br>
      On 21/10/2016 17:38, Vikan Manmathan wrote:<br>
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    <blockquote
cite="mid:CADCvCZmAJigqb2S66PZKCCJGKRDZKQFjucUp89VVpXg6J6GX=Q@mail.gmail.com"
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          <div>Dear Developers and Experts,<br>
            <br>
          </div>
          <div>I am interested in studying diffusion of metal clusters
            on oxide support. As a first step, I took a simplest case (<span
              class="" style="" id=":1cs.1" tabindex="-1">adatom</span>
            hopping) and obtained the transition state using CI-NEB
            method.  I want to find the rate constant for the above, I
            need to know the normal mode vibrational frequencies at
            initial and transition states. <br>
             <br>
          </div>
          So I calculated the phonon frequencies using frozen atomic
          coordinate (<span class="" style="" id=":1cs.2" tabindex="-1">nat</span>_<span
            class="" style="" id=":1cs.3" tabindex="-1">todo</span>
          option only on metal <span class="" style="" id=":1cs.4"
            tabindex="-1">adatom</span>) since the system size is very
          large.  I expected the transition state to have one less real
          frequencies (3N-1) relative to initial state (3N). However, I
          am getting 3N real frequencies for the transition state
          (correct me if I am wrong).<br>
          <br>
           I have also checked it by including more atoms in the linear
          response (up to 33 atoms) but still I got 3N real frequencies
          for the TS.<br>
          <br>
        </div>
        <div>I have attached the input files and the output file
          generated by <span class="" style="" id=":1cs.5"
            tabindex="-1">dynmat</span>.x<br>
        </div>
        <div><br>
        </div>
        <div>Any suggestion will be highly appreciated.<br>
          <br>
        </div>
        <div>Thanks in advance.<br>
          <br>
        </div>
        <div>regards,<br>
        </div>
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                          <div><span
                              style="background-color:rgb(255,255,255)"><b><font
                                  size="2"><span class="" style=""
                                    id=":1cs.7" tabindex="-1">NANDHA</span>
                                  <span class="" style="" id=":1cs.8"
                                    tabindex="-1">KUMAR</span> V.</font></b></span><br>
                          </div>
                          <span
                            style="background-color:rgb(238,238,238)"><span></span></span><font
                            color="#0b5394"><font
                              face="tahoma,sans-serif">Research scholar,<br>
                            </font></font>
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                                  <div><span style="color:rgb(32,18,77)"><span
                                        class="" style="" id=":1cs.9"
                                        tabindex="-1">IISER</span>, <span
                                        class="" style="" id=":1cs.10"
                                        tabindex="-1">PUNE</span>.<span
style="background-color:rgb(0,0,0)"><span></span></span><span
                                        style="background-color:rgb(243,243,243)"><span></span></span></span><br>
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