<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-21T11:13:12Z</responseDate><request verb="GetRecord" identifier="oai:dspace.mit.edu:1721.1/103713" metadataPrefix="dim">https://dspace.mit.edu/server/oai/request</request><GetRecord><record><header><identifier>oai:dspace.mit.edu:1721.1/103713</identifier><datestamp>2022-01-13T07:54:05Z</datestamp><setSpec>com_1721.1_7582</setSpec><setSpec>com_1721.1_7581</setSpec><setSpec>col_1721.1_131024</setSpec></header><metadata><dim:dim xmlns:dim="http://www.dspace.org/xmlns/dspace/dim" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.dspace.org/xmlns/dspace/dim http://www.dspace.org/schema/dim.xsd">
   <dim:field mdschema="dc" element="contributor" qualifier="advisor" lang="en_US">Bilge Yildiz.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="author" lang="en_US">Dinh, Minh A</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="other" lang="en_US">Massachusetts Institute of Technology. Department of Nuclear Science and Engineering.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="department">Massachusetts Institute of Technology. Department of Nuclear Science and Engineering</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="accessioned">2016-07-18T20:03:31Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="available">2016-07-18T20:03:31Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="copyright" lang="en_US">2015</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="issued" lang="en_US">2015</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="uri">http://hdl.handle.net/1721.1/103713</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="oclc" lang="en_US">953291090</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Thesis: S.B., Massachusetts Institute of Technology, Department of Nuclear Science and Engineering, 2015.</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Cataloged from PDF version of thesis.</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Includes bibliographical references (pages 31-33).</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="abstract" lang="en_US">The surfaces of zirconium during early stages of metal oxidation were examined by first-principles calculations using density functional theory. DFT calculations suggested that the interaction between the oxide and the substrate induced a slight vertical contraction of the oxide film and a slight buckling of the Zr layer in the oxide in which the latter effect was found to be more important. The total effect was significant. In fact, among the three examined configurations, the difference in heights across the oxide surface could reach 0.55 [angstroms] which should be visible under STM images. Therefore, the periodic relaxation patterns observed on the surface of zirconium at the initial stage in of its oxidation in previous study could be explained by the buckling of the zirconium layer in the oxide coupled with the fact that there was a mismatch between Zr metal and ZrO2 oxide lattice parameters. While some atomically-resolved STM images were also generated, more DFT results from different structure configurations are needed before a complete and useful large-scale STM image could be constructed.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="statementofresponsibility" lang="en_US">by Minh A. Dinh.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="degree" lang="en_US">S.B.</dim:field>
   <dim:field mdschema="dc" element="format" qualifier="extent" lang="en_US">33 pages</dim:field>
   <dim:field mdschema="dc" element="language" qualifier="iso" lang="en_US">eng</dim:field>
   <dim:field mdschema="dc" element="publisher" lang="en_US">Massachusetts Institute of Technology</dim:field>
   <dim:field mdschema="dc" element="rights" lang="en_US">M.I.T. theses are protected by copyright. They may be viewed from this source for any purpose, but reproduction or distribution in any format is prohibited without written permission. See provided URL for inquiries about permission.</dim:field>
   <dim:field mdschema="dc" element="rights" qualifier="uri" lang="en_US">http://dspace.mit.edu/handle/1721.1/7582</dim:field>
   <dim:field mdschema="dc" element="subject" lang="en_US">Nuclear Science and Engineering.</dim:field>
   <dim:field mdschema="dc" element="title" lang="en_US">First-principles study of the surfaces of zirconium during early stages of metal oxidation</dim:field>
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   	&lt;Title>First-principles study of the surfaces of zirconium during early stages of metal oxidation&lt;/Title>
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   	&lt;PublicationDate>2015&lt;/PublicationDate>
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        	&lt;DisplayName>Dinh, Minh A&lt;/DisplayName>
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    &lt;Keyword>Nuclear Science and Engineering.&lt;/Keyword>
   	&lt;Abstract>The surfaces of zirconium during early stages of metal oxidation were examined by first-principles calculations using density functional theory. DFT calculations suggested that the interaction between the oxide and the substrate induced a slight vertical contraction of the oxide film and a slight buckling of the Zr layer in the oxide in which the latter effect was found to be more important. The total effect was significant. In fact, among the three examined configurations, the difference in heights across the oxide surface could reach 0.55 [angstroms] which should be visible under STM images. Therefore, the periodic relaxation patterns observed on the surface of zirconium at the initial stage in of its oxidation in previous study could be explained by the buckling of the zirconium layer in the oxide coupled with the fact that there was a mismatch between Zr metal and ZrO2 oxide lattice parameters. While some atomically-resolved STM images were also generated, more DFT results from different structure configurations are needed before a complete and useful large-scale STM image could be constructed.&lt;/Abstract>
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