<?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>2026-04-18T02:15:36Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/131795" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/131795</identifier><datestamp>2025-12-05T16:48:59Z</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>BK-parameter from Nf = 2 twisted mass lattice QCD</dc:title>
   <dc:creator>Constantinou, M.</dc:creator>
   <dc:creator>Dimopoulos, P.</dc:creator>
   <dc:creator>Frezzotti, R.</dc:creator>
   <dc:creator>Jansen, K.</dc:creator>
   <dc:creator>Gimenez, V.</dc:creator>
   <dc:creator>Lubicz, V.</dc:creator>
   <dc:creator>Mescia, Federico</dc:creator>
   <dc:creator>Panagopoulos, H.</dc:creator>
   <dc:creator>Papinutto, M.</dc:creator>
   <dc:creator>Rossi, G. C.</dc:creator>
   <dc:creator>Simula, S.</dc:creator>
   <dc:creator>Skouroupathis, A.</dc:creator>
   <dc:creator>Stylianou, F.</dc:creator>
   <dc:creator>Vladikas, A.</dc:creator>
   <dc:creator>ETM Collaboration</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>We present an unquenched N f = 2 lattice computation of the B K parameter which controls K 0 − ¯¯¯¯ K 0 oscillations. A partially quenched setup is employed with two maximally twisted dynamical (sea) light Wilson quarks, and valence quarks of both the maximally twisted and the Osterwalder-Seiler variety. Suitable combinations of these two kinds of valence quarks lead to a lattice definition of the B K parameter which is both multiplicatively renormalizable and O ( a ) improved. Employing the nonperturbative RI-MOM scheme, in the continuum limit and at the physical value of the pion mass we get B RGI K = 0.729 ± 0.030 , a number well in line with the existing quenched and unquenched determinations.</dc:description>
   <dc:date>2019-04-08T12:11:20Z</dc:date>
   <dc:date>2019-04-08T12:11:20Z</dc:date>
   <dc:date>2011-01-01</dc:date>
   <dc:date>2019-04-08T12:11:20Z</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/2445/131795</dc:identifier>
   <dc:identifier>623813</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Reproducció del document publicat a: https://doi.org/10.1103/PhysRevD.83.014505</dc:relation>
   <dc:relation>Physical Review D, 2011, vol. 83, num. 1, p. 014505</dc:relation>
   <dc:relation>https://doi.org/10.1103/PhysRevD.83.014505</dc:relation>
   <dc:relation>info:eu-repo/grantAgreement/EC/FP7/249309/EU//HPLQCD</dc:relation>
   <dc:rights>(c) American Physical Society, 2011</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>20 p.</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>
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