<?xml version="1.0" encoding="UTF-8"?><feed xmlns="http://www.w3.org/2005/Atom" xmlns:dc="http://purl.org/dc/elements/1.1/">
<title>Structural, optical and electrical properties of nitrogen and lithium doped ZnO</title>
<link href="http://127.0.0.1/xmlui/handle/123456789/584" rel="alternate"/>
<subtitle/>
<id>http://127.0.0.1/xmlui/handle/123456789/584</id>
<updated>2026-04-17T12:17:38Z</updated>
<dc:date>2026-04-17T12:17:38Z</dc:date>
<entry>
<title>Structural, optical and electrical properties of nitrogen and lithium doped ZnO</title>
<link href="http://127.0.0.1/xmlui/handle/123456789/585" rel="alternate"/>
<author>
<name>Majumdar, Sayanee</name>
</author>
<id>http://127.0.0.1/xmlui/handle/123456789/585</id>
<updated>2015-05-29T11:16:30Z</updated>
<published>2010-01-01T00:00:00Z</published>
<summary type="text">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.
</summary>
<dc:date>2010-01-01T00:00:00Z</dc:date>
</entry>
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