Publication data of Ligeti, Zoltan: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion199520002005201020152020202502500500075001000012500
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications199520002005201020152020202503060901201500246810
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion1995200020052010201520202025010203040506070
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestNew limit on inclusive $B o X_{s}$ anti-neutrino neutrino decay and constraints on new physicsNew limit on inclusive $B o X_{s}$ anti-neutrino neutrino decay and constra…|V(ub)| from exclusive B and D decaysOn dark matter models with uniquely spin-dependent detection possibilitiesImplications of the LHCb Evidence for Charm CP ViolationImplications of the B --> X lepton anti-lepton-neutrino lepton spectrum for heavy quark theoryImplications of the B --> X lepton anti-lepton-neutrino lepton spectrum for he…Precision determination of |V(ub)| from inclusive decaysImplications of the measurement of the $B^0_{s} - ar{B}^0_s$ mass differenceImplications of the measurement of the $B^0_{s} - ar{B}^0_s$ mass diffe…Heavy quark expansion for the inclusive decay anti-B ---> tau anti-neutrino XLessons from CLEO and FOCUS measurements of D0 - anti-D0 mixing parametersLessons from CLEO and FOCUS measurements of D0 - anti-D0 mixing param…SU(3) relations and the CP asymmetries in B decays to eta-prime K(S), phi K(S) and K+ K- K(S)SU(3) relations and the CP asymmetries in B decays to eta-prime K(S), phi K(…Semileptonic B decays to excited charmed mesonsTreating the b quark distribution function with reliable uncertaintiesGlobal analysis of inclusive B decaysThe D0 - anti-D0 mass difference from a dispersion relationB decay and the Upsilon massB decays in the upsilon expansionSU(3) breaking and D0 - anti-D0 mixingFlavor models for $ar{B} o D^{(*)} au ar{ u}$Combined analysis of semileptonic $B$ decays to $D$ and $D^*$: $R(D^{(*)})$, $|V_{cb}|$, and new physicsCombined analysis of semileptonic $B$ decays to $D$ and $D^*$: $R(D^{(*…199520002005201020152020202502500500075001000012500
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)New limit on inclusive $B o X_{s}$ anti-neutrino neutrino decay and constraints on new physicsNew limit on inclusive $B o X_{s}$ anti-neutrino neutrino decay and constra…|V(ub)| from exclusive B and D decaysOn dark matter models with uniquely spin-dependent detection possibilitiesImplications of the LHCb Evidence for Charm CP ViolationImplications of the B --> X lepton anti-lepton-neutrino lepton spectrum for heavy quark theoryImplications of the B --> X lepton anti-lepton-neutrino lepton spectrum for he…Precision determination of |V(ub)| from inclusive decaysImplications of the measurement of the $B^0_{s} - ar{B}^0_s$ mass differenceImplications of the measurement of the $B^0_{s} - ar{B}^0_s$ mass diffe…Heavy quark expansion for the inclusive decay anti-B ---> tau anti-neutrino XLessons from CLEO and FOCUS measurements of D0 - anti-D0 mixing parametersLessons from CLEO and FOCUS measurements of D0 - anti-D0 mixing param…SU(3) relations and the CP asymmetries in B decays to eta-prime K(S), phi K(S) and K+ K- K(S)SU(3) relations and the CP asymmetries in B decays to eta-prime K(S), phi K(…Semileptonic B decays to excited charmed mesonsTreating the b quark distribution function with reliable uncertaintiesGlobal analysis of inclusive B decaysThe D0 - anti-D0 mass difference from a dispersion relationB decay and the Upsilon massB decays in the upsilon expansionSU(3) breaking and D0 - anti-D0 mixingFlavor models for $ar{B} o D^{(*)} au ar{ u}$Combined analysis of semileptonic $B$ decays to $D$ and $D^*$: $R(D^{(*)})$, $|V_{cb}|$, and new physicsCombined analysis of semileptonic $B$ decays to $D$ and $D^*$: $R(D^{(*…19952000200520102015202020250255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average19952000200520102015202020250100200300400500600