<?xml version="1.0" encoding="UTF-8"?><rdf:RDF xmlns="http://purl.org/rss/1.0/" xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/">
<channel rdf:about="http://127.0.0.1/xmlui/handle/123456789/584">
<title>Structural, optical and electrical properties of nitrogen and lithium doped ZnO</title>
<link>http://127.0.0.1/xmlui/handle/123456789/584</link>
<description/>
<items>
<rdf:Seq>
<rdf:li rdf:resource="http://127.0.0.1/xmlui/handle/123456789/585"/>
</rdf:Seq>
</items>
<dc:date>2026-04-17T05:44:19Z</dc:date>
</channel>
<item rdf:about="http://127.0.0.1/xmlui/handle/123456789/585">
<title>Structural, optical and electrical properties of nitrogen and lithium doped ZnO</title>
<link>http://127.0.0.1/xmlui/handle/123456789/585</link>
<description>Structural, optical and electrical properties of nitrogen and lithium doped ZnO
Majumdar, Sayanee
Zinc oxide (ZnO) is a wide band gap (Eg = 3.3 eV at 300 K) semiconductor with large&#13;
exciton binding energy at room temperature (~ 60 meV). As-grown ZnO is always n-type&#13;
though p-type doping is indispensable to fabricate opto-electronic devices. This thesis&#13;
contains studies on p-type doping in ZnO by lithium (Li) and nitrogen (N). After&#13;
chemical synthesis of doped and as-prepared ZnO, the films were deposited by pulsed&#13;
laser deposition and characterized by structural, optical and electrical techniques. It was&#13;
observed from the x-ray diffraction (XRD) and Raman spectroscopy that Li had&#13;
substituted Zn in ZnO lattice. The change in a- and c-parameter with Li incorporation&#13;
was found to be due to lattice strain. It was also observed from photoluminescence (PL)&#13;
measurements that no deep level was formed prohibiting p-type conductivity.
</description>
<dc:date>2010-01-01T00:00:00Z</dc:date>
</item>
</rdf:RDF>
