<?xml version="1.0" encoding='utf-8'?>
<!DOCTYPE wml PUBLIC "-//WAPFORUM//DTD WML 1.1//EN" "http://www.wapforum.org/DTD/wml_1.1.xml">
<wml>
<card id="card1" title="Ferromagnetism - Page 17 - Wikipedia">
<p>
<a accesskey="1" href="page.php?w=Ferromagnetism&amp;p=16">1.Previous</a><br />
<a accesskey="3" href="page.php?w=Ferromagnetism&amp;p=18">3.Next</a>
</p>
<p>but which undergoes a structural transition into a <a href="page.php?w=Tetragonal_crystal_system">tetragonal</a> state with ferromagnetic order when cooled below its 1=''T''<sub>C</sub> = 125 K. In its ferromagnetic state, PuP's <a href="page.php?w=easy_axis">easy axis</a> is in the <100> direction.</100></p>

<p>In NpFe<sub>2</sub> the easy axis is <111>. Above ''T''<sub>C</sub> ? 500&nbsp;K, NpFe<sub>2</sub> is also paramagnetic and cubic. Cooling below the Curie temperature produces a <a href="page.php?w=rhombohedral">rhombohedral</a> distortion wherein the rhombohedral angle changes from 60° (cubic phase) to 60.53°. An alternate description of this distortion is to consider the length  along the unique trigonal axis (after the distortion has begun) and  as the distance in the plane perpendicular to . In the cubic phase this reduces to {{Mvar/Mvar|a}} =}} 1.00}}. Below the Curie temperature, the lattice acquires a distortion</111></p><p>
<a accesskey="1" href="page.php?w=Ferromagnetism&amp;p=16">1.Previous</a><br />
<a accesskey="3" href="page.php?w=Ferromagnetism&amp;p=18">3.Next</a>
</p>

<do type="prev" label="Search">
        <go href="search.wml"/>
</do>

</card>
</wml>
