<div dir="ltr">Dear Wien2k and Prof Blaha<div><br></div><div>According to Prof Blaha (<a href="https://www.mail-archive.com/wien@zeus.theochem.tuwien.ac.at/msg01133.html">https://www.mail-archive.com/wien@zeus.theochem.tuwien.ac.at/msg01133.html</a> ) , in the paramagnetic state, the local magnetic moments still exists bur oriented in arbitrary directions. And according to this approach , there are infinite configurations for the paramagnetic state.</div><div><br></div><div>On the hand, there are many articles where their authors simulate the paramagnetic state differently.</div><div><br></div><div>Example 01:</div><div><br></div><div>... The paramagnetic states are also treated using spin-polarized calculation with <b>the magnetic moments of all Ni atoms equal to zero</b>.</div><div><br></div><div>Example 02:</div><div><br></div><div>Hexagonal NiS is a pamagnetic metal with high conductivity above the temperature Tt. At Tt, the system undergoes a first-order phase transition, where the resistivity abruptly increases and<b> magnetic moments appear at the Ni sites.</b></div><div><br></div><div>I need comments for this discrepancy from wien2k users and especially from Prof Blaha.</div><div><br></div><div>Best regards<br clear="all"><div><br></div>-- <br><div class="gmail_signature" data-smartmail="gmail_signature"><div dir="ltr"><div><div dir="ltr"><div><div dir="ltr"><div><div dir="ltr"><div><div dir="ltr"><div><div dir="ltr"><div><div dir="ltr"><div style="font-family:monospace"><div><font size="2"><span style="color:rgb(0,0,255)">Mr: A.Reggad</span> <br><span style="background-color:rgb(238,238,238)"><span style="color:blue">Laboratoire de Génie Physique</span></span><br></font></div><font size="2"><span style="color:rgb(0,0,255)">Université Ibn Khaldoun - Tiaret</span><br></font></div><div><font size="2"><span style="font-family:monospace"><span style="color:rgb(0,0,255)">Algerie</span></span></font><br></div><div><div><br><span style="font-family:times new roman,serif"><span style="color:blue"></span></span><br></div></div></div></div></div></div></div></div></div></div></div></div></div></div></div></div>
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