<div dir="ltr">Dear Prof. Blaha,<div><br></div><div>                         I am sending a cif file of diatomic N2 herewith this email. Kindly suggest to me if it is right.</div><div><br></div><div>with regards,</div></div><br><div class="gmail_quote"><div dir="ltr" class="gmail_attr">On Wed, 7 Jun 2023 at 17:43, Peter Blaha <<a href="mailto:peter.blaha@tuwien.ac.at">peter.blaha@tuwien.ac.at</a>> wrote:<br></div><blockquote class="gmail_quote" style="margin:0px 0px 0px 0.8ex;border-left:1px solid rgb(204,204,204);padding-left:1ex">You have to simulate a N2 molecule.<br>
<br>
Choose a box of about 205 bohr and put 2 N atoms at +/-z, such that <br>
their distance is about the experimental distance.<br>
<br>
Use identical RMT and RKMAX values when you simulate   N2, C5N and graphite.<br>
<br>
<br>
<br>
Am 6/7/23 um 13:24 schrieb shamik chakrabarti:<br>
> I think I need to simulate the energy of diatomic nitrogen..but how to <br>
> do it?<br>
> <br>
> On Wed, 7 Jun 2023 at 16:17, shamik chakrabarti <br>
> <<a href="mailto:shamik15041981@gmail.com" target="_blank">shamik15041981@gmail.com</a> <mailto:<a href="mailto:shamik15041981@gmail.com" target="_blank">shamik15041981@gmail.com</a>>> wrote:<br>
> <br>
>     Dear Prof. Blaha,<br>
> <br>
>                    I want to simulate the formation energy of C5N<br>
>     (nitrogen doped monolayer graphene) with respect to the phase<br>
>     separation between C6 & N. Which struct file of nitrogen then we<br>
>     should choose?<br>
> <br>
>     with regards,<br>
> <br>
>     On Wed, 7 Jun 2023 at 16:00, Peter Blaha <<a href="mailto:peter.blaha@tuwien.ac.at" target="_blank">peter.blaha@tuwien.ac.at</a><br>
>     <mailto:<a href="mailto:peter.blaha@tuwien.ac.at" target="_blank">peter.blaha@tuwien.ac.at</a>>> wrote:<br>
> <br>
>         Besides what Fabien answered:<br>
> <br>
>         The magnetic moment is fortunately   6 uB, not 0.6.   Each N<br>
>         atom contributes obviously 3 electrons.<br>
> <br>
>         If I interpret the website correctly, these are r2scan data, not<br>
>         PBE anymore ???<br>
> <br>
> <br>
>         Anyway, N in hcp close packed structure ???<br>
> <br>
>         In databases you can do everything ....<br>
> <br>
>         Am 07.06.2023 um 11:08 schrieb shamik chakrabarti:<br>
>>         Dear Wien2k users,<br>
>><br>
>>                          I have tried to optimize the crystal<br>
>>         structure of Alpha-N2 by using data from "<br>
>>         <a href="https://materialsproject.org/materials/mp-12103/#electronic_Structure" rel="noreferrer" target="_blank">https://materialsproject.org/materials/mp-12103/#electronic_Structure</a> <<a href="https://materialsproject.org/materials/mp-12103/#electronic_Structure" rel="noreferrer" target="_blank">https://materialsproject.org/materials/mp-12103/#electronic_Structure</a>>"<br>
>>         However, after optimization (or even with the unoptimized<br>
>>         cell) we are getting vast different electronic band gap.<br>
>>         The structure on <br>
>>          "<a href="https://materialsproject.org/materials/mp-12103/#electronic_Structure" rel="noreferrer" target="_blank">https://materialsproject.org/materials/mp-12103/#electronic_Structure</a> <<a href="https://materialsproject.org/materials/mp-12103/#electronic_Structure" rel="noreferrer" target="_blank">https://materialsproject.org/materials/mp-12103/#electronic_Structure</a>>" tells band gap as *0.96 eV* while our optimized structure ( or even with the unoptimized structure) is giving the band gap as *~ 10.553 eV*. However the magnetic moment is coming the same (~0.6 muB) for both the cases. I am attaching the optimized struct file herewith this mail.<br>
>><br>
>>         Looking forward to your response in this regards.<br>
>><br>
>>         with regards,<br>
>><br>
>>         -- <br>
>>         Dr. Shamik Chakrabarti<br>
>>         Research Fellow<br>
>>         Department of Physics<br>
>>         Indian Institute of Technology Patna<br>
>>         Bihta-801103<br>
>>         Patna<br>
>>         Bihar, India<br>
>><br>
>>         _______________________________________________<br>
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> <br>
>         -- <br>
>         -----------------------------------------------------------------------<br>
>         Peter Blaha,  Inst. f. Materials Chemistry, TU Vienna, A-1060 Vienna<br>
>         Phone: +43-158801165300<br>
>         <a href="mailto:Email%3Apeter.blaha@tuwien.ac.at" target="_blank">Email:peter.blaha@tuwien.ac.at</a>  <mailto:<a href="mailto:peter.blaha@tuwien.ac.at" target="_blank">peter.blaha@tuwien.ac.at</a>>           <br>
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> <br>
> <br>
> <br>
>     -- <br>
>     Dr. Shamik Chakrabarti<br>
>     Research Fellow<br>
>     Department of Physics<br>
>     Indian Institute of Technology Patna<br>
>     Bihta-801103<br>
>     Patna<br>
>     Bihar, India<br>
> <br>
> <br>
> <br>
> -- <br>
> Dr. Shamik Chakrabarti<br>
> Research Fellow<br>
> Department of Physics<br>
> Indian Institute of Technology Patna<br>
> Bihta-801103<br>
> Patna<br>
> Bihar, India<br>
> <br>
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<br>
-- <br>
Peter Blaha, Inst.f. Materials Chemistry, TU Vienna, A-1060 Vienna<br>
Phone: +43-1-58801-165300          Email: <a href="mailto:peter.blaha@tuwien.ac.at" target="_blank">peter.blaha@tuwien.ac.at</a><br>
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</blockquote></div><br clear="all"><div><br></div><span class="gmail_signature_prefix">-- </span><br><div dir="ltr" class="gmail_signature"><div dir="ltr"><div><div dir="ltr"><div dir="ltr"><div dir="ltr"><div dir="ltr"><div style="font-size:small">Dr. Shamik Chakrabarti</div><div style="font-size:small">Research Fellow </div><div style="font-size:small">Department of Physics</div><div style="font-size:small">Indian Institute of Technology Patna</div><div style="font-size:small">Bihta-801103</div><div style="font-size:small">Patna</div><div style="font-size:small">Bihar, India</div></div></div></div></div></div></div></div>