Publication data of Behring, Arnd: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion20122014201620182020202220240250500750100012501500
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications20122014201620182020202220240102030405001.534.567.5
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion20122014201620182020202220240510152025
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestThe polarized transition matrix element $A_{gq}(N)$ of the variable flavor number scheme at $O(alpha^3_s)$The polarized transition matrix element $A_{gq}(N)$ of the variable flavor n…Asymptotic 3-loop heavy flavor corrections to the charged current structure functions $F_L^{W^+-W^-}(x,Q^2)$ and $F_2^{W^+-W^-}(x,Q^2)$Asymptotic 3-loop heavy flavor corrections to the charged current structure …The three-loop single mass polarized pure singlet operator matrix elementSquark Flavor Implications from B --> K* l+ l-Higgs decay into massive b-quarks at NNLO QCD in the nested soft-collinear subtraction schemeHiggs decay into massive b-quarks at NNLO QCD in the nested soft-collinear …Quark beam function at next-to-next-to-next-to-leading order in perturbative QCD in the generalized large-$N_c$ approximationQuark beam function at next-to-next-to-next-to-leading order in perturbative …The Polarized Three-Loop Anomalous Dimensions from On-Shell Massive Operator Matrix ElementsThe Polarized Three-Loop Anomalous Dimensions from On-Shell Massive Oper…O($alpha_s^3$) heavy flavor contributions to the charged current structure function $xF_3(x,Q^2)$ at large momentum transferO($alpha_s^3$) heavy flavor contributions to the charged current structure …The unpolarized and polarized single-mass three-loop heavy flavor operator matrix elements A$_{gg,Q}$ and ∆A$_{gg,Q}$The unpolarized and polarized single-mass three-loop heavy flavor operator …The 3-Loop Non-Singlet Heavy Flavor Contributions to the Structure Function $g_{1}(x,Q^{2})$ at Large Momentum TransferThe 3-Loop Non-Singlet Heavy Flavor Contributions to the Structure Function…Heavy Flavor Wilson Coefficients in Deep-Inelastic Scattering: Recent ResultsHeavy quark form factors at two loopsMixed QCD-electroweak corrections to $W$-boson production in hadron collisionsMixed QCD-electroweak corrections to $W$-boson production in hadron collis…The three-loop splitting functions $P_{qg}^{(2)}$ and $P_{gg}^{(2, N_F)}$Higher order corrections to spin correlations in top quark pair production at the LHCHigher order corrections to spin correlations in top quark pair production at t…The logarithmic contributions to the $O(alpha^3_s)$ asymptotic massive Wilson coefficients and operator matrix elements in deeply inelastic scatteringThe logarithmic contributions to the $O(alpha^3_s)$ asymptotic massive Wil…Calculating Three Loop Ladder and V-Topologies for Massive Operator Matrix Elements by Computer AlgebraCalculating Three Loop Ladder and V-Topologies for Massive Operator Matrix E…The 3-Loop Non-Singlet Heavy Flavor Contributions and Anomalous Dimensions for the Structure Function $F_2(x,Q^2)$ and TransversityThe 3-Loop Non-Singlet Heavy Flavor Contributions and Anomalous Dimensio…The 3-loop pure singlet heavy flavor contributions to the structure function $F_2(x,Q^2)$ and the anomalous dimensionThe 3-loop pure singlet heavy flavor contributions to the structure function $…20122014201620182020202220240250500750100012501500
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)The polarized transition matrix element $A_{gq}(N)$ of the variable flavor number scheme at $O(alpha^3_s)$The polarized transition matrix element $A_{gq}(N)$ of the variable flavor n…Asymptotic 3-loop heavy flavor corrections to the charged current structure functions $F_L^{W^+-W^-}(x,Q^2)$ and $F_2^{W^+-W^-}(x,Q^2)$Asymptotic 3-loop heavy flavor corrections to the charged current structure …The three-loop single mass polarized pure singlet operator matrix elementSquark Flavor Implications from B --> K* l+ l-Higgs decay into massive b-quarks at NNLO QCD in the nested soft-collinear subtraction schemeHiggs decay into massive b-quarks at NNLO QCD in the nested soft-collinear …Quark beam function at next-to-next-to-next-to-leading order in perturbative QCD in the generalized large-$N_c$ approximationQuark beam function at next-to-next-to-next-to-leading order in perturbative …The Polarized Three-Loop Anomalous Dimensions from On-Shell Massive Operator Matrix ElementsThe Polarized Three-Loop Anomalous Dimensions from On-Shell Massive Oper…O($alpha_s^3$) heavy flavor contributions to the charged current structure function $xF_3(x,Q^2)$ at large momentum transferO($alpha_s^3$) heavy flavor contributions to the charged current structure …The unpolarized and polarized single-mass three-loop heavy flavor operator matrix elements A$_{gg,Q}$ and ∆A$_{gg,Q}$The unpolarized and polarized single-mass three-loop heavy flavor operator …The 3-Loop Non-Singlet Heavy Flavor Contributions to the Structure Function $g_{1}(x,Q^{2})$ at Large Momentum TransferThe 3-Loop Non-Singlet Heavy Flavor Contributions to the Structure Function…Heavy Flavor Wilson Coefficients in Deep-Inelastic Scattering: Recent ResultsHeavy quark form factors at two loopsMixed QCD-electroweak corrections to $W$-boson production in hadron collisionsMixed QCD-electroweak corrections to $W$-boson production in hadron collis…The three-loop splitting functions $P_{qg}^{(2)}$ and $P_{gg}^{(2, N_F)}$Higher order corrections to spin correlations in top quark pair production at the LHCHigher order corrections to spin correlations in top quark pair production at t…The logarithmic contributions to the $O(alpha^3_s)$ asymptotic massive Wilson coefficients and operator matrix elements in deeply inelastic scatteringThe logarithmic contributions to the $O(alpha^3_s)$ asymptotic massive Wil…Calculating Three Loop Ladder and V-Topologies for Massive Operator Matrix Elements by Computer AlgebraCalculating Three Loop Ladder and V-Topologies for Massive Operator Matrix E…The 3-Loop Non-Singlet Heavy Flavor Contributions and Anomalous Dimensions for the Structure Function $F_2(x,Q^2)$ and TransversityThe 3-Loop Non-Singlet Heavy Flavor Contributions and Anomalous Dimensio…The 3-loop pure singlet heavy flavor contributions to the structure function $F_2(x,Q^2)$ and the anomalous dimensionThe 3-loop pure singlet heavy flavor contributions to the structure function $…20122014201620182020202220240255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average2012201420162018202020222024050100150200250300