<?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></authors></contributors><titles><title><style face="normal" font="default" size="100%">Not-step-like density of states and carrier distribution of conduction-band, narrow-to-wide 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%">2004</style></year></dates><urls><web-urls><url><style face="normal" font="default" size="100%">https://www.sciencedirect.com/science/article/pii/S138694770300732X?via%3Dihub</style></url></web-urls></urls><number><style face="normal" font="default" size="100%">2-4</style></number><volume><style face="normal" font="default" size="100%">21</style></volume><pages><style face="normal" font="default" size="100%">956-960</style></pages><language><style face="normal" font="default" size="100%">eng</style></language><abstract><style face="normal" font="default" size="100%">We analyze the important changes induced in the density of states of narrow-to-wide conduction-band dilute magnetic semiconductor quantum wells subjected to an in-plane magnetic field, &lt;em&gt;B&lt;/em&gt;. We show quantitatively that the DOS diverges significantly from the &lt;em&gt;famous&lt;/em&gt; step-like two-dimensional electron gas form, by providing results for many values of &lt;em&gt;B&lt;/em&gt; and grades of spatial localization. This introduces changes in the pertinent electronic properties. The self-consistent approach is indispensable and the eigenvalue problem has to be solved for each subband index &lt;em&gt;i&lt;/em&gt;, spin &lt;em&gt;σ&lt;/em&gt;, and in-plane wave vector, e.g. &lt;em&gt;k&lt;/em&gt;&lt;sub&gt;&lt;em&gt;x&lt;/em&gt;&lt;/sub&gt;. We can select the appropriate parameters so that the structure is populated by carriers of spin-down or exploit the effect of the &lt;em&gt;depopulation&lt;/em&gt; of the higher spin-subbands to eliminate carriers with spin-up.</style></abstract><notes><style face="normal" font="default" size="100%">cited By 7</style></notes></record></records></xml>