Publication data of Portoles, Jorge: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion199520002005201020152020202501000200030004000
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications199520002005201020152020202502040608010001.22.43.64.86
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion199520002005201020152020202505101520253035
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestHadron structure in tau ---> KK pi nu (tau) decaysThe Chiral Lagrangian parameters, l1, l2, are determined by the rho resonanceThe Chiral Lagrangian parameters, l1, l2, are determined by the rho resonan…Vector meson exchange contributions to K ---> pi gamma gamma and K(L) ---> gamma lepton+ lepton-Vector meson exchange contributions to K ---> pi gamma gamma and K(L) --…tau ---> pi pi pi nu(tau) decays in the resonance effective theorySpectral distribution for the decay tau ---> nu(tau) K piUnitarity and vector meson contributions to K+ ---> pi+ gamma gammaThe Vector form-factor of the pion from unitarity and analyticity: A Model independent approachThe Vector form-factor of the pion from unitarity and analyticity: A Model ind…Lepton flavour violating semileptonic tau decays in constrained MSSM-seesaw scenariosLepton flavour violating semileptonic tau decays in constrained MSSM-seesa…Form-factors in radiative pion decaytau ---> pi pi pi nu(tau) decays and the a(1)(1260) off-shell width revisitedIntegrating out heavy particles with functional methods: a simplified frameworkIntegrating out heavy particles with functional methods: a simplified framew…The Hadronic off-shell width of meson resonancesThe < VAP > Green function in the resonance regionCan we extract short distance information from B(K(L) ---> mu+ mu-)?Odd intrinsic parity processes within the resonance effective theory of QCDThe < SPP > Green function and SU(3) breaking in K(l3) decaysTowards a consistent estimate of the chiral low-energy constantsThe Decays K ---> pi l+ l- beyond leading order in the chiral expansionKaon Decays in the Standard Model199520002005201020152020202501000200030004000
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)Hadron structure in tau ---> KK pi nu (tau) decaysThe Chiral Lagrangian parameters, l1, l2, are determined by the rho resonanceThe Chiral Lagrangian parameters, l1, l2, are determined by the rho resonan…Vector meson exchange contributions to K ---> pi gamma gamma and K(L) ---> gamma lepton+ lepton-Vector meson exchange contributions to K ---> pi gamma gamma and K(L) --…tau ---> pi pi pi nu(tau) decays in the resonance effective theorySpectral distribution for the decay tau ---> nu(tau) K piUnitarity and vector meson contributions to K+ ---> pi+ gamma gammaThe Vector form-factor of the pion from unitarity and analyticity: A Model independent approachThe Vector form-factor of the pion from unitarity and analyticity: A Model ind…Lepton flavour violating semileptonic tau decays in constrained MSSM-seesaw scenariosLepton flavour violating semileptonic tau decays in constrained MSSM-seesa…Form-factors in radiative pion decaytau ---> pi pi pi nu(tau) decays and the a(1)(1260) off-shell width revisitedIntegrating out heavy particles with functional methods: a simplified frameworkIntegrating out heavy particles with functional methods: a simplified framew…The Hadronic off-shell width of meson resonancesThe < VAP > Green function in the resonance regionCan we extract short distance information from B(K(L) ---> mu+ mu-)?Odd intrinsic parity processes within the resonance effective theory of QCDThe < SPP > Green function and SU(3) breaking in K(l3) decaysTowards a consistent estimate of the chiral low-energy constantsThe Decays K ---> pi l+ l- beyond leading order in the chiral expansionKaon Decays in the Standard Model19952000200520102015202020250255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average1995200020052010201520202025050100150200250300