Publication data of Bell, Guido: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion20062008201020122014201620182020202220240500100015002000
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications20062008201020122014201620182020202220240102030405001.534.567.5
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion2006200820102012201420162018202020222024051015202530
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestTwo-loop anomalous dimensions of generic dijet soft functionsHeavy-to-light currents at NNLO in SCET and semi-inclusive $ar{B} o X_s l^+ l^-$ decayHeavy-to-light currents at NNLO in SCET and semi-inclusive $ar{B} o X_s …Generic dijet soft functions at two-loop order: correlated emissionsMaster integrals for the two-loop penguin contribution in non-leptonic B-decaysMaster integrals for the two-loop penguin contribution in non-leptonic B-deca…Enhanced nonperturbative effects through the collinear anomalyElectroweak Sudakov Logarithms and Real Gauge-Boson Radiation in the TeV RegionElectroweak Sudakov Logarithms and Real Gauge-Boson Radiation in the TeV …B- ---> pi- pi0/rho- rho0 to NNLO in QCD factorizationTwo-loop current–current operator contribution to the non-leptonic QCD penguin amplitudeTwo-loop current–current operator contribution to the non-leptonic QCD pen…Higher order QCD corrections in exclusive charmless B decays$e^+ e^-$ angularity distributions at NNLL$^prime$ accuracyNNLO corrections to inclusive semileptonic B decays in the shape-function regionNNLO corrections to inclusive semileptonic B decays in the shape-function re…Factorization and Resummation for Jet BroadeningNNLO vertex corrections in charmless hadronic B decays: Real partModelling light-cone distribution amplitudes from non-relativistic bound statesNNLO vertex corrections in charmless hadronic B decays: Imaginary partNNLL Resummation for Jet BroadeningThe gluon jet function at two-loop orderLight-Cone Distribution Amplitudes for Heavy-Quark HadronsAnalytic Regularization in Soft-Collinear Effective Theory20062008201020122014201620182020202220240500100015002000
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)Two-loop anomalous dimensions of generic dijet soft functionsHeavy-to-light currents at NNLO in SCET and semi-inclusive $ar{B} o X_s l^+ l^-$ decayHeavy-to-light currents at NNLO in SCET and semi-inclusive $ar{B} o X_s …Generic dijet soft functions at two-loop order: correlated emissionsMaster integrals for the two-loop penguin contribution in non-leptonic B-decaysMaster integrals for the two-loop penguin contribution in non-leptonic B-deca…Enhanced nonperturbative effects through the collinear anomalyElectroweak Sudakov Logarithms and Real Gauge-Boson Radiation in the TeV RegionElectroweak Sudakov Logarithms and Real Gauge-Boson Radiation in the TeV …B- ---> pi- pi0/rho- rho0 to NNLO in QCD factorizationTwo-loop current–current operator contribution to the non-leptonic QCD penguin amplitudeTwo-loop current–current operator contribution to the non-leptonic QCD pen…Higher order QCD corrections in exclusive charmless B decays$e^+ e^-$ angularity distributions at NNLL$^prime$ accuracyNNLO corrections to inclusive semileptonic B decays in the shape-function regionNNLO corrections to inclusive semileptonic B decays in the shape-function re…Factorization and Resummation for Jet BroadeningNNLO vertex corrections in charmless hadronic B decays: Real partModelling light-cone distribution amplitudes from non-relativistic bound statesNNLO vertex corrections in charmless hadronic B decays: Imaginary partNNLL Resummation for Jet BroadeningThe gluon jet function at two-loop orderLight-Cone Distribution Amplitudes for Heavy-Quark HadronsAnalytic Regularization in Soft-Collinear Effective Theory20062008201020122014201620182020202220240255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average2006200820102012201420162018202020222024050100150200250