<?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>2026-04-18T05:58:00Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:2445/12418" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:2445/12418</identifier><datestamp>2025-12-05T16:41:57Z</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>Heavy quark hadronic Lagrangian for s-wave quarkonium</dc:title>
   <dc:creator>Pineda, Antonio (Pineda Ruiz)</dc:creator>
   <dc:creator>Soto Riera, Joan</dc:creator>
   <dc:subject>Pertorbació (Dinàmica quàntica)</dc:subject>
   <dc:subject>Quarks</dc:subject>
   <dc:subject>Perturbation (Quantum dynamics)</dc:subject>
   <dc:subject>Quarks</dc:subject>
   <dc:description>We use Heavy Quark Effective Theory (HQET) techniques to parametrize certain non-perturbative effects related to quantum fluctuations that put both heavy quark and antiquark in quarkonium almost on shell. The large off-shell momentum contributions are calculated using Coulomb type states. The almost on-shell momentum contributions are evaluated using an effective 'chiral' lagrangian which incorporates the relevant symmetries of the HQET for quarks and antiquarks. The cut-off dependence of both contributions matches perfectly. The decay constants and the matrix elements of bilinear currents at zero recoil are calculated. The new non-perturbative contributions from the on-shell region are parametrized by a single constant. They turn out to be $O(\alpha^2/\Lambda_{QCD} a_{n})$, $a_{n}$ being the Bohr radius and $\alpha$ the strong coupling constant, times the non-perturbative contribution coming from the multipole expansion (gluon condensate). We discuss the physical applications to $\Upsilon$, $J/\Psi$ and $B_{c}$ systems.</dc:description>
   <dc:date>2010-05-06T10:46:42Z</dc:date>
   <dc:date>2010-05-06T10:46:42Z</dc:date>
   <dc:date>1996</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>0556-2821</dc:identifier>
   <dc:identifier>https://hdl.handle.net/2445/12418</dc:identifier>
   <dc:identifier>112033</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Reproducció digital del document publicat en format paper, proporcionada per PROLA i http://dx.doi.org/10.1103/PhysRevD.53.3983</dc:relation>
   <dc:relation>Physical Review D, 1996, vol. 53, núm. 7, p. 3983-3997</dc:relation>
   <dc:relation>http://dx.doi.org/10.1103/PhysRevD.53.3983</dc:relation>
   <dc:rights>(c) The American Physical Society, 1996</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>15 p.</dc:format>
   <dc:format>application/pdf</dc:format>
   <dc:publisher>The American Physical Society</dc:publisher>
   <dc:source>Articles publicats en revistes (Física Quàntica i Astrofísica)</dc:source>
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