<?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>2026-06-27T10:32:13Z</responseDate><request verb="GetRecord" identifier="oai:docta.ucm.es:20.500.14352/43951" metadataPrefix="mods">https://docta.ucm.es/rest/oai/request</request><GetRecord><record><header><identifier>oai:docta.ucm.es:20.500.14352/43951</identifier><datestamp>2023-08-25T14:40:47Z</datestamp><setSpec>com_20.500.14352_14</setSpec><setSpec>col_20.500.14352_15</setSpec></header><metadata><mods:mods xmlns:mods="http://www.loc.gov/mods/v3" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.loc.gov/mods/v3 http://www.loc.gov/standards/mods/v3/mods-3-1.xsd">
   <mods:name>
      <mods:namePart>Llanes Estrada, Felipe José</mods:namePart>
   </mods:name>
   <mods:name>
      <mods:namePart>Bicudo, Pedro</mods:namePart>
   </mods:name>
   <mods:name>
      <mods:namePart>Cardoso, M</mods:namePart>
   </mods:name>
   <mods:extension>
      <mods:dateAvailable encoding="iso8601">2023-06-20T03:34:57Z</mods:dateAvailable>
   </mods:extension>
   <mods:extension>
      <mods:dateAccessioned encoding="iso8601">2023-06-20T03:34:57Z</mods:dateAccessioned>
   </mods:extension>
   <mods:originInfo>
      <mods:dateIssued encoding="iso8601">2009-08-28</mods:dateIssued>
   </mods:originInfo>
   <mods:identifier type="issn">0031-9007</mods:identifier>
   <mods:identifier type="doi">10.1103/PhysRevLett.103.092003</mods:identifier>
   <mods:identifier type="uri">https://hdl.handle.net/20.500.14352/43951</mods:identifier>
   <mods:identifier type="officialurl">http://dx.doi.org/10.1103/PhysRevLett.103.092003</mods:identifier>
   <mods:identifier type="relatedurl">http://prl.aps.org</mods:identifier>
   <mods:abstract>We argue that three-quark excited states naturally group into quartets, split into two parity doublets, and that the mass splittings between these parity partners decrease higher up in the baryon spectrum. This decreasing mass difference can be used to probe the running quark mass in the midinfrared power-law regime. A measurement of masses of high-partial-wave  resonances should be sufficient to unambiguously establish the approximate degeneracy. We test this concept with the first computation of excited high-j baryon masses in a chirally invariant quark model.</mods:abstract>
   <mods:language>
      <mods:languageTerm>eng</mods:languageTerm>
   </mods:language>
   <mods:accessCondition type="useAndReproduction">open access</mods:accessCondition>
   <mods:titleInfo>
      <mods:title>Probing the infrared quark mass from highly excited baryons</mods:title>
   </mods:titleInfo>
   <mods:genre>journal article</mods:genre>
</mods:mods></metadata></record></GetRecord></OAI-PMH>