<?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>2026-06-08T10:43:29Z</responseDate><request verb="GetRecord" identifier="oai:docta.ucm.es:20.500.14352/33623" metadataPrefix="qdc">https://docta.ucm.es/rest/oai/request</request><GetRecord><record><header><identifier>oai:docta.ucm.es:20.500.14352/33623</identifier><datestamp>2024-09-04T18:00:01Z</datestamp><setSpec>com_20.500.14352_14</setSpec><setSpec>col_20.500.14352_15</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>Feshbach-type resonances for two-particle scattering in graphene</dc:title>
   <dc:creator>Gaul, Christopher</dc:creator>
   <dc:creator>Domínguez-Adame Acosta, Francisco</dc:creator>
   <dc:creator>Sols Lucía, Fernando</dc:creator>
   <dc:creator>Zapata, I.</dc:creator>
   <dcterms:abstract>Two-particle scattering in graphene is a multichannel problem, where the energies of the identical or opposite-helicity channels lie in disjoint energy segments. Due to the absence of Galilean invariance, these segments depend on the total momentum Q. The dispersion relations for the two opposite-helicity scattering channels are analogous to those of two one-dimensional tight-binding lattices with opposite dispersion relations, which are known to easily bind states at their edges. When an s-wave separable interaction potential is assumed, those bound states reveal themselves as three Feshbach resonances in the identical-helicity channel. In the limit Q -> 0, one of the resonances survives and the opposite-helicity scattering amplitudes vanish.</dcterms:abstract>
   <dcterms:dateAccepted>2023-06-19T13:25:11Z</dcterms:dateAccepted>
   <dcterms:available>2023-06-19T13:25:11Z</dcterms:available>
   <dcterms:created>2023-06-19T13:25:11Z</dcterms:created>
   <dcterms:issued>2014-01-21</dcterms:issued>
   <dc:type>journal article</dc:type>
   <dc:identifier>https://hdl.handle.net/20.500.14352/33623</dc:identifier>
   <dc:identifier>0163-1829</dc:identifier>
   <dc:identifier>10.1103/PhysRevB.89.045420</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>MICROSERES-CM (S2009/TIC-1476)</dc:relation>
   <dc:relation>(FIS2010-21372)</dc:relation>
   <dc:relation>(MAT2010-17180)</dc:relation>
   <dc:relation>Marie Curie ITN NanoCTM</dc:relation>
   <dc:relation>PICATA</dc:relation>
   <dc:rights>open access</dc:rights>
   <dc:publisher>American Physical Society</dc:publisher>
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