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<DIV style="FONT: 10pt MS UI Gothic">----- Original Message ----- </DIV>
<DIV
style="BACKGROUND: #e4e4e4; FONT: 10pt MS UI Gothic; font-color: black"><B>From:</B>
<A title=arto@mail.nnz.ru href="mailto:arto@mail.nnz.ru">Oleg Artamonov</A>
</DIV>
<DIV style="FONT: 10pt MS UI Gothic"><B>To:</B> <A
title=wien@zeus.theochem.tuwien.ac.at
href="mailto:wien@zeus.theochem.tuwien.ac.at">A Mailing list for WIEN2k
users</A> </DIV>
<DIV style="FONT: 10pt MS UI Gothic"><B>Sent:</B> Thursday, October 09, 2008
6:06 PM</DIV>
<DIV style="FONT: 10pt MS UI Gothic"><B>Subject:</B> [Wien] Surface states
splitting</DIV>
<DIV><BR></DIV>
<DIV>
<P align=left><FONT face="Times New Roman">Dear Peter Blaha,</FONT></P>
<P align=left><FONT face="Times New Roman">In Your paper "PHYSICAL REVIEW B,
VOLUME 65, 033407" in Fig. 1 you present two surface state
dispersion curves for opposite spin projections. I am trying to
repeat this for the W(110) surface. May I ask you to list the key points of
your calculation? How is it possible to recognize the spin projection for
surface states?</FONT></P>
<P align=left><FONT face="Times New Roman">Sincerely yours,</FONT></P>
<P align=left><FONT face="Times New Roman">
Oleg Artamonov.</FONT></P></DIV>
<P>
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