<?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>2026-09-21T00:10:18Z</responseDate><request verb="GetRecord" identifier="oai:dspace.mit.edu:1721.1/120215" metadataPrefix="dim">https://dspace.mit.edu/server/oai/request</request><GetRecord><record><header><identifier>oai:dspace.mit.edu:1721.1/120215</identifier><datestamp>2022-01-13T07:54:07Z</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">Nevin Weinberg and Joshua N. Winn.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="author" lang="en_US">Patra, Kishore Chandra</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="other" lang="en_US">Massachusetts Institute of Technology. Department of Physics.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="department">Massachusetts Institute of Technology. Department of Physics</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="accessioned">2019-02-05T15:58:27Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="available">2019-02-05T15:58:27Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="copyright" lang="en_US">2018</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="issued" lang="en_US">2018</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="uri">http://hdl.handle.net/1721.1/120215</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="oclc" lang="en_US">1082863704</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Thesis: S.B., Massachusetts Institute of Technology, Department of Physics, 2018.</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 87-93).</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="abstract" lang="en_US">We summarize our results, so far, in the search for orbital decay in exoplanets. Orbital decay is the gradual shrinkage of the planetary orbit due to tidal dissipation. We ranked currently known exoplanetary systems according to the theoretical orbital decay rate and trimmed the list down to 12 best targets. We collected new transit light curves for the targets visible in the northern hemisphere using the 1.2 m telescope at the Fred L. Whipple Observatory, Arizona. For the southern targets, we are currently collaborating with the Las Cumbres Observatory Telescope Network to obtain new transits. We analyzed the timing residuals for each target, seeking evidence for any change in the orbital period. Currently, the best candidate for orbital decay is WASP-12 b with an observed period derivative ... . However, we find that a few other possible models, including apsidal precession, nodal precession and color-dependent transit times, cannot be ruled out completely. Continous monitoring of WASP-12 b is necessary in the future to resolve the current conundrum. The search for orbital decay is still in its infancy for most other targets. However, we aim to produce a few transit times for each target to serve as an "anchor" for when TESS relays back more high quality light curves.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="statementofresponsibility" lang="en_US">by Kishore Chandra Patra.</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">93 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">MIT theses are protected by copyright. They may be viewed, downloaded, or printed from this source but further reproduction or distribution in any format is prohibited without written 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">Physics.</dim:field>
   <dim:field mdschema="dc" element="title" lang="en_US">The search for orbital decay in hot Jupiters</dim:field>
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   	&lt;Title>The search for orbital decay in hot Jupiters&lt;/Title>
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   	&lt;PublicationDate>2018&lt;/PublicationDate>
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        	&lt;DisplayName>Patra, Kishore Chandra&lt;/DisplayName>
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    &lt;Keyword>Physics.&lt;/Keyword>
   	&lt;Abstract>We summarize our results, so far, in the search for orbital decay in exoplanets. Orbital decay is the gradual shrinkage of the planetary orbit due to tidal dissipation. We ranked currently known exoplanetary systems according to the theoretical orbital decay rate and trimmed the list down to 12 best targets. We collected new transit light curves for the targets visible in the northern hemisphere using the 1.2 m telescope at the Fred L. Whipple Observatory, Arizona. For the southern targets, we are currently collaborating with the Las Cumbres Observatory Telescope Network to obtain new transits. We analyzed the timing residuals for each target, seeking evidence for any change in the orbital period. Currently, the best candidate for orbital decay is WASP-12 b with an observed period derivative ... . However, we find that a few other possible models, including apsidal precession, nodal precession and color-dependent transit times, cannot be ruled out completely. Continous monitoring of WASP-12 b is necessary in the future to resolve the current conundrum. The search for orbital decay is still in its infancy for most other targets. However, we aim to produce a few transit times for each target to serve as an &amp;quot;anchor&amp;quot; for when TESS relays back more high quality light curves.&lt;/Abstract>
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