Publication data of Eilam, Gad: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion1970198019902000201020200100020003000400050006000
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications197019801990200020102020040801201602000246810
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion19701980199020002010202001020304050
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestProbing the flavor changing tc vertex via tree level processes: e+ e- ---> t anti-c electron-neutrino anti-electron-neutrino, t anti-c e+ e- and t ---> c W+ W-Probing the flavor changing tc vertex via tree level processes: e+ e- ---> t an…B ---> phi pi and B0 ---> phi phi in the standard model and new bounds on R parity violationB ---> phi pi and B0 ---> phi phi in the standard model and new bounds on R…Pure leptonic radiative decays B+-, D(s) ---> lepton neutrino gamma and the annihilation graphPure leptonic radiative decays B+-, D(s) ---> lepton neutrino gamma and the…Experimental constraints on stop-scharm flavor mixing and implications in top-quark FCNC processesExperimental constraints on stop-scharm flavor mixing and implications in to…High-energy Collisions With Atomic Nuclei. Part 1Enhancement of CP violation in B+- ---> K(i)+- D0 by resonant effectsRadiative decay B ---> lepton neutrino gamma in the light cone QCD approachNumber of Neutrinos in the Standard Model and Its Extensions to SupersymmetryNumber of Neutrinos in the Standard Model and Its Extensions to Supersym…A Quark-parton Model of Nuclear ProductionOn the rate asymmetries in charged B decays$B o K ell^+ ell^-$ and Other Rare $B$ Meson DecaysFLAVOR CHANGING ELECTROMAGNETIC TRANSITIONSRadiative corrections to top quark decayTop quark rare decay t ---> ch in R-parity violating SUSYSUSY-induced FCNC top-quark processes at the large hadron colliderMultiparticle Production in Particle-Nucleus Collisions at High-EnergiesCP violation in top physicsB ---> K* gamma and the Top Quark MassRare decays of the top quark in the standard and two Higgs doublet models1970198019902000201020200100020003000400050006000
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)Probing the flavor changing tc vertex via tree level processes: e+ e- ---> t anti-c electron-neutrino anti-electron-neutrino, t anti-c e+ e- and t ---> c W+ W-Probing the flavor changing tc vertex via tree level processes: e+ e- ---> t an…B ---> phi pi and B0 ---> phi phi in the standard model and new bounds on R parity violationB ---> phi pi and B0 ---> phi phi in the standard model and new bounds on R…Pure leptonic radiative decays B+-, D(s) ---> lepton neutrino gamma and the annihilation graphPure leptonic radiative decays B+-, D(s) ---> lepton neutrino gamma and the…Experimental constraints on stop-scharm flavor mixing and implications in top-quark FCNC processesExperimental constraints on stop-scharm flavor mixing and implications in to…High-energy Collisions With Atomic Nuclei. Part 1Enhancement of CP violation in B+- ---> K(i)+- D0 by resonant effectsRadiative decay B ---> lepton neutrino gamma in the light cone QCD approachNumber of Neutrinos in the Standard Model and Its Extensions to SupersymmetryNumber of Neutrinos in the Standard Model and Its Extensions to Supersym…A Quark-parton Model of Nuclear ProductionOn the rate asymmetries in charged B decays$B o K ell^+ ell^-$ and Other Rare $B$ Meson DecaysFLAVOR CHANGING ELECTROMAGNETIC TRANSITIONSRadiative corrections to top quark decayTop quark rare decay t ---> ch in R-parity violating SUSYSUSY-induced FCNC top-quark processes at the large hadron colliderMultiparticle Production in Particle-Nucleus Collisions at High-EnergiesCP violation in top physicsB ---> K* gamma and the Top Quark MassRare decays of the top quark in the standard and two Higgs doublet models1970198019902000201020200255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average197019801990200020102020050100150200250