<?xml version="1.0" encoding="UTF-8"?><xml><records><record><source-app name="Biblio" version="7.x">Drupal-Biblio</source-app><ref-type>17</ref-type><contributors><authors><author><style face="normal" font="default" size="100%">Simserides, C.</style></author><author><style face="normal" font="default" size="100%">Galanakis, I.</style></author></authors></contributors><titles><title><style face="normal" font="default" size="100%">Quasi-two-dimensional carriers in dilute-magnetic-semiconductor quantum wells under in-plane magnetic field</style></title><secondary-title><style face="normal" font="default" size="100%">Physica E: Low-Dimensional Systems and Nanostructures</style></secondary-title></titles><dates><year><style  face="normal" font="default" size="100%">2008</style></year></dates><urls><web-urls><url><style face="normal" font="default" size="100%">https://www.sciencedirect.com/science/article/pii/S1386947707003232?via%3Dihub</style></url></web-urls></urls><number><style face="normal" font="default" size="100%">5</style></number><volume><style face="normal" font="default" size="100%">40</style></volume><pages><style face="normal" font="default" size="100%">1214-1216</style></pages><language><style face="normal" font="default" size="100%">eng</style></language><abstract><style face="normal" font="default" size="100%">Due to the competition between spatial and magnetic confinement, the density of states (DOS) of a quasi-two-dimensional system deviates from the ideal step-like form both quantitatively and qualitatively. We study how this affects the spin-subband populations and the spin polarization as functions of the temperature, &lt;em&gt;T&lt;/em&gt;, and the in-plane magnetic field, &lt;em&gt;B&lt;/em&gt;, for narrow to wide dilute-magnetic-semiconductor quantum wells (QWs). We focus on the QW width, the magnitude of the spin–spin exchange interaction, and the sheet carrier concentration dependence. We look for ranges where the system is completely spin polarized. Increasing &lt;em&gt;T&lt;/em&gt;, the carrier spin splitting, &lt;em&gt;U&lt;/em&gt;&lt;sub&gt;0σ&lt;/sub&gt;&lt;span class=&quot;math&quot;&gt;&lt;span class=&quot;MathJax_Preview&quot;&gt;&lt;/span&gt;&lt;span id=&quot;MathJax-Element-1-Frame&quot; style=&quot;font-size: 90%; display: inline-block; position: relative;&quot; class=&quot;MathJax_SVG&quot; data-mathml=&quot;&lt;math xmlns=&amp;quot;http://www.w3.org/1998/Math/MathML&amp;quot;&gt;&lt;msub is=&amp;quot;true&amp;quot;&gt;&lt;mrow is=&amp;quot;true&amp;quot;&gt;&lt;mi is=&amp;quot;true&amp;quot;&gt;U&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=&amp;quot;true&amp;quot;&gt;&lt;mn is=&amp;quot;true&amp;quot;&gt;0&lt;/mn&gt;&lt;mi is=&amp;quot;true&amp;quot;&gt;&amp;amp;#x3C3;&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&quot;&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class=&quot;math&quot;&gt;&lt;/span&gt;, decreases, while on increasing &lt;em&gt;B&lt;/em&gt;, &lt;span class=&quot;math&quot;&gt;&lt;span class=&quot;MathJax_Preview&quot;&gt;&lt;/span&gt;&lt;span id=&quot;MathJax-Element-2-Frame&quot; style=&quot;font-size: 90%; display: inline-block; position: relative;&quot; class=&quot;MathJax_SVG&quot; data-mathml=&quot;&lt;math xmlns=&amp;quot;http://www.w3.org/1998/Math/MathML&amp;quot;&gt;&lt;msub is=&amp;quot;true&amp;quot;&gt;&lt;mrow is=&amp;quot;true&amp;quot;&gt;&lt;mi is=&amp;quot;true&amp;quot;&gt;U&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow is=&amp;quot;true&amp;quot;&gt;&lt;mn is=&amp;quot;true&amp;quot;&gt;0&lt;/mn&gt;&lt;mi is=&amp;quot;true&amp;quot;&gt;&amp;amp;#x3C3;&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&quot;&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class=&quot;math&quot;&gt;&lt;/span&gt; &lt;em&gt;U&lt;/em&gt;&lt;sub&gt;0σ &lt;/sub&gt;increases. Moreover, due to the DOS modification, all energetically higher subbands become gradually depopulated.</style></abstract><notes><style face="normal" font="default" size="100%">cited By 7</style></notes></record></records></xml>