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    <div class="moz-cite-prefix">Dear Alex<br>
      if the band structure is the same, the results should be
      comparable.<br>
      <br>
      There are two possible sources of difference that come to my mind:<br>
      1. The Wannier-interpolated band structure is different (e.g.
      because the Wannierization is not converged). Did you check if WFs
      are real, and the interpolated band structure is the same as the
      one calculated with VASP?<br>
      <br>
      2. The interpolation procedure is different in the two codes. Did
      you check in both codes that the results do not depend on the
      density of k-points used for the interpolation/integration?<br>
      <br>
      Also, the value that you state is evaluated at which chemical
      potential and temperature?<br>
      <br>
      Giovanni<br>
      <br>
      <br>
      On 10/17/2016 03:27 PM, Alex Gal Aziz wrote:<br>
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    <blockquote
cite="mid:HE1PR0101MB2441BE4CAEC0BE66EDE3525AD1D00@HE1PR0101MB2441.eurprd01.prod.exchangelabs.com"
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        <p>Thanks for the message,</p>
        <p><br>
        </p>
        <p>I have done a check with one calculation with BoltzTRAP and
          Boltzwann using PBE+U. Although the trend seems to be the
          same, the values are not really the same. The BoltzTRAP
          calculation gives values about 100<span
            style="mso-bidi-font-family:"Times New Roman""> μ</span>V/K
          higher. Around 500<span
            style="mso-bidi-font-family:"Times New Roman""> μ</span>V/K
          for BoltzTRAP compared to 400<span
            style="mso-bidi-font-family:"Times New Roman""> μ</span>V/K
          for Boltzwann.
          <br>
        </p>
        <p><br>
        </p>
        <p>I believe the error must be on my part, but changing the
          number of WF doesn't change the result. I have kept the
          Bandstructure frozen till about 1 eV above the lowest
          conduction band.</p>
        <p><br>
        </p>
        <p>Any ideas would be welcome.</p>
        <p><br>
        </p>
        <p>Thanks</p>
        <p><br>
        </p>
        <p>Alex Aziz</p>
        <p>PhD Student</p>
        <p>University of Reading<br>
        </p>
        <br>
        <br>
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            <hr tabindex="-1" style="display:inline-block; width:98%">
            <div id="x_divRplyFwdMsg" dir="ltr"><font
                style="font-size:11pt" face="Calibri, sans-serif"
                color="#000000"><b>From:</b> Wannier
                <a class="moz-txt-link-rfc2396E" href="mailto:wannier-bounces@quantum-espresso.org"><wannier-bounces@quantum-espresso.org></a> on behalf
                of Nicki Frank Hinsche
                <a class="moz-txt-link-rfc2396E" href="mailto:nicki.hinsche@physik.uni-halle.de"><nicki.hinsche@physik.uni-halle.de></a><br>
                <b>Sent:</b> 01 September 2016 21:38<br>
                <b>To:</b> <a class="moz-txt-link-abbreviated" href="mailto:wannier@quantum-espresso.org">wannier@quantum-espresso.org</a><br>
                <b>Subject:</b> [Wannier] Cu2ZnSnSe and Cu2ZnSnS
                (Boltzwann Calculations)</font>
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          <font size="2"><span style="font-size:10pt;">
              <div class="PlainText">Hej Ali, <br>
                <br>
                this depends heavily on the charge carrier
                concentration. The difference due to bipolar effects
                will be way more pronounced at high temperatures and/or
                low charge carrier concentrations. The size of the gap
                merely plays a role in the degenerate limit.<br>
                <br>
                bests<br>
                Nicki<br>
                <br>
                --------------------------------------------------------<br>
                Nicki Frank Hinsche, Dr. rer. nat.<br>
                HC Ørsted Postdoc<br>
                CAMd, Technical University of Denmark<br>
                Fysikvej, Bld. 307, Room 208<br>
                2800 Kgs. Lyngby, Denmark <br>
                Tel.: ++45 45 25 31 84 <br>
                --------------------------------------------------------<br>
                <br>
                > Message: 1<br>
                > Date: Thu, 1 Sep 2016 10:03:04 +0000<br>
                > From: Alex Gal Aziz
                <a class="moz-txt-link-rfc2396E" href="mailto:A.G.Aziz@pgr.reading.ac.uk"><A.G.Aziz@pgr.reading.ac.uk></a><br>
                > To: <a class="moz-txt-link-rfc2396E" href="mailto:wannier@quantum-espresso.org">"wannier@quantum-espresso.org"</a>
                <a class="moz-txt-link-rfc2396E" href="mailto:wannier@quantum-espresso.org"><wannier@quantum-espresso.org></a><br>
                > Subject: [Wannier] Cu2ZnSnSe and Cu2ZnSnS
                (Boltzwann Calculations)<br>
                > Message-ID:<br>
                >       
<a class="moz-txt-link-rfc2396E" href="mailto:VI1PR0101MB2365665CF6E0025C9742F44AD1E20@VI1PR0101MB2365.eurprd01.prod.exchangelabs.com"><VI1PR0101MB2365665CF6E0025C9742F44AD1E20@VI1PR0101MB2365.eurprd01.prod.exchangelabs.com></a><br>
                >        <br>
                > Content-Type: text/plain; charset="iso-8859-1"<br>
                > <br>
                > I am investigating Cu2ZnSnSe4 and Cu2ZnSnS4.<br>
                > <br>
                > <br>
                > I have been using VASP compiled with Wannier
                functions to generate the initial projections and then
                generate the MLWF using the Disentanglement procedure. I
                have checked the band structures and they look correct
                with the appropriate band gaps (~1.5 for Cu2ZnSnS4 and
                0.9 Cu2ZnSnSe4).<br>
                > <br>
                > <br>
                > When I check the Seebeck using BoltzWann I seem to
                get similar results in both cases. I am trying to figure
                out if this seems plausible due to the difference in
                band gaps.<br>
                > <br>
                > <br>
                > Any suggestions would be welcomed<br>
                > <br>
                > <br>
                > Thanks<br>
                > <br>
                > Alex Aziz<br>
                > <br>
                > <br>
                > PhD Student<br>
                > <br>
                > Department of Chemistry, University of Reading<br>
                > Whiteknights, Reading RG6 6AD<br>
                <br>
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      <pre wrap="">_______________________________________________
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</pre>
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    <br>
    <p><br>
    </p>
    <pre class="moz-signature" cols="72">-- 
Giovanni Pizzi
EPFL STI IMX THEOS
MED2 1326
Station 9
CH-1015 Lausanne (Switzerland)
Phone: +41 21 69 31124</pre>
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