<?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>2026-04-17T17:32:10Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/152915" metadataPrefix="qdc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/152915</identifier><datestamp>2025-12-05T11:00:12Z</datestamp><setSpec>com_2072_1057</setSpec><setSpec>col_2072_478907</setSpec><setSpec>col_2072_478917</setSpec><setSpec>col_2072_478933</setSpec></header><metadata><qdc:qualifieddc xmlns:qdc="http://dspace.org/qualifieddc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://purl.org/dc/elements/1.1/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dc.xsd http://purl.org/dc/terms/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dcterms.xsd http://dspace.org/qualifieddc/ http://www.ukoln.ac.uk/metadata/dcmi/xmlschema/qualifieddc.xsd">
   <dc:title>Newton Trajectories for the tilted Frenkel‐Kontorova model</dc:title>
   <dc:creator>Quapp, Wolfgang</dc:creator>
   <dc:creator>Bofill i Villà, Josep M.</dc:creator>
   <dc:subject>Química física</dc:subject>
   <dc:subject>Estructura electrònica</dc:subject>
   <dc:subject>Teories no lineals</dc:subject>
   <dc:subject>Physical and theoretical chemistry</dc:subject>
   <dc:subject>Electronic structure</dc:subject>
   <dc:subject>Nonlinear theories</dc:subject>
   <dcterms:abstract>Newton trajectories are used for the Frenkel-Kontorova model of a finite chain with free-end bound- ary conditions. We optimise stationary structures, as well as barrier breakdown points for a critical tilting force were depinning of the chain happens. These special points can be obtained straight for- wardly by the tool of Newton trajectories. We explain the theory and add examples for a finite-length chain of a fixed number of 2, 3, 4, 5 and 23 particles.</dcterms:abstract>
   <dcterms:issued>2020-03-18T10:05:22Z</dcterms:issued>
   <dcterms:issued>2020-03-18T10:05:22Z</dcterms:issued>
   <dcterms:issued>2019-02-06</dcterms:issued>
   <dcterms:issued>2020-03-18T10:05:22Z</dcterms:issued>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/acceptedVersion</dc:type>
   <dc:relation>Versió postprint del document publicat a: https://doi.org/10.1080/00268976.2019.1576930</dc:relation>
   <dc:relation>Molecular Physics, 2019, vol. 117, num. 9-12, p. 1541-1558</dc:relation>
   <dc:relation>https://doi.org/10.1080/00268976.2019.1576930</dc:relation>
   <dc:rights>(c) Taylor and Francis, 2019</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:publisher>Taylor and Francis</dc:publisher>
   <dc:source>Articles publicats en revistes (Química Inorgànica i Orgànica)</dc:source>
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