<?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>2026-04-18T03:17:02Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/131796" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/131796</identifier><datestamp>2025-11-21T05:49:00Z</datestamp><setSpec>com_2072_1057</setSpec><setSpec>col_2072_478823</setSpec><setSpec>col_2072_478917</setSpec></header><metadata><oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
   <dc:title>K∗ vector and tensor couplings from Nf=2 twisted mass QCD</dc:title>
   <dc:creator>Dimopoulos, P.</dc:creator>
   <dc:creator>Mescia, Federico</dc:creator>
   <dc:creator>Vladikas, A.</dc:creator>
   <dc:subject>Física de partícules</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dc:subject>Particle physics</dc:subject>
   <dc:subject>Experiments</dc:subject>
   <dc:description>The mass m K ∗ and vector coupling f K ∗ of the K ∗ meson, as well as the ratio of the tensor to vector couplings f T f V | K ∗ , are computed in lattice QCD. Our simulations are performed in a partially quenched setup, with two dynamical (sea) Wilson quark flavors, having a maximally twisted mass term. Valence quarks are either of the standard or the Osterwalder-Seiler maximally twisted variety. Results obtained at three values of the lattice spacing are extrapolated to the continuum, giving m K ∗ = 981 ( 33 )     MeV , f K ∗ = 240 ( 18 )     MeV , and f T ( 2     GeV ) f V | K ∗ = 0.704 ( 41 ) .</dc:description>
   <dc:date>2019-04-08T12:12:21Z</dc:date>
   <dc:date>2019-04-08T12:12:21Z</dc:date>
   <dc:date>2011-07-19</dc:date>
   <dc:date>2019-04-08T12:12:21Z</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>1550-7998</dc:identifier>
   <dc:identifier>https://hdl.handle.net/2445/131796</dc:identifier>
   <dc:identifier>623814</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Reproducció del document publicat a: https://doi.org/10.1103/PhysRevD.84.014505</dc:relation>
   <dc:relation>Physical Review D, 2011, vol. 84, num. 1, p. 014505</dc:relation>
   <dc:relation>https://doi.org/10.1103/PhysRevD.84.014505</dc:relation>
   <dc:rights>(c) American Physical Society, 2011</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>7 p.</dc:format>
   <dc:format>application/pdf</dc:format>
   <dc:format>application/pdf</dc:format>
   <dc:publisher>American Physical Society</dc:publisher>
   <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
</oai_dc:dc></metadata></record></GetRecord></OAI-PMH>