Publication data of Cleven, Martin: Link to Inspire

Created with Highcharts 9.0.1CitationsCitationsw/o self-citaionself-citaion2010201220142016201820202022202402004006008001000
Created with Highcharts 9.0.1Publicationspublications per yearPublicationsPublications per yearCumulative publications201020122014201620182020202220240510152025012345
Created with Highcharts 9.0.1h-indexh-indexh-indexh-index w/o self-citaion20102012201420162018202020222024024681012
Created with Highcharts 9.0.1CitationsBreakdown of Most Cited PapersrestProperties of open and hidden charm mesons in light quark matterEffects of $Z_b$ states in $Upsilon(3S, 4S)$ dipion transitionsProperties of open and hidden charm meson in light quark matterOpen Charm Contributions to the E1 Transitions of (psi )(3686) and (psi )(3770) ( o ) (gamma chi _{cJ})Open Charm Contributions to the E1 Transitions of (psi )(3686) and (psi )(37…Properties of $J/psi$ in light quark matterThe nature of near-threshold XYZ statesSystematic Study of Hadronic Molecules in the Heavy-Quark SectorOpen charm contributions to the E1 transitions of $psi (3686)$ and $psi (3770) ightarrow gamma chi _{cJ}$Open charm contributions to the E1 transitions of $psi (3686)$ and $psi (37…$X$(3872) in a hot pion bathProperties of open and hidden charm mesons in light quark matterCross section line shape of $e^+e^- ochi_{c0}omega$ around the $Y(4260)$ mass regionCross section line shape of $e^+e^- ochi_{c0}omega$ around the $Y(4260)…Effects of $Z_b$ states and bottom meson loops on $Upsilon(4S) o Upsilon(1S,2S) pi^+pi^-$ transitionsEffects of $Z_b$ states and bottom meson loops on $Upsilon(4S) o Upsilon(…Strong and radiative decays of the $D^*_{s0}(2317)$ and $D_{s1}(2460)$Light meson mass dependence of the positive parity heavy-strange mesonsY(4260): hadronic molecule versus hadro-charmonium interpretationEmploying spin symmetry to disentangle different models for the XYZ statesConfirming the molecular nature of the $Z_b(10610)$ and the $Z_b(10650)$$Y(4260)$ as the first $S$-wave open charm vector molecular state?Bound state nature of the exotic $Z_b$ states2010201220142016201820202022202402004006008001000
Created with Highcharts 9.0.1Fraction [%]Breakdown of Most Cited Papers (Fraction)Properties of open and hidden charm mesons in light quark matterEffects of $Z_b$ states in $Upsilon(3S, 4S)$ dipion transitionsProperties of open and hidden charm meson in light quark matterOpen Charm Contributions to the E1 Transitions of (psi )(3686) and (psi )(3770) ( o ) (gamma chi _{cJ})Open Charm Contributions to the E1 Transitions of (psi )(3686) and (psi )(37…Properties of $J/psi$ in light quark matterThe nature of near-threshold XYZ statesSystematic Study of Hadronic Molecules in the Heavy-Quark SectorOpen charm contributions to the E1 transitions of $psi (3686)$ and $psi (3770) ightarrow gamma chi _{cJ}$Open charm contributions to the E1 transitions of $psi (3686)$ and $psi (37…$X$(3872) in a hot pion bathProperties of open and hidden charm mesons in light quark matterCross section line shape of $e^+e^- ochi_{c0}omega$ around the $Y(4260)$ mass regionCross section line shape of $e^+e^- ochi_{c0}omega$ around the $Y(4260)…Effects of $Z_b$ states and bottom meson loops on $Upsilon(4S) o Upsilon(1S,2S) pi^+pi^-$ transitionsEffects of $Z_b$ states and bottom meson loops on $Upsilon(4S) o Upsilon(…Strong and radiative decays of the $D^*_{s0}(2317)$ and $D_{s1}(2460)$Light meson mass dependence of the positive parity heavy-strange mesonsY(4260): hadronic molecule versus hadro-charmonium interpretationEmploying spin symmetry to disentangle different models for the XYZ statesConfirming the molecular nature of the $Z_b(10610)$ and the $Z_b(10650)$$Y(4260)$ as the first $S$-wave open charm vector molecular state?Bound state nature of the exotic $Z_b$ states201020122014201620182020202220240255075100
Created with Highcharts 9.0.1Citations/1 YearCitations/PeriodCitations / 1 YearMoving average201020122014201620182020202220240255075100125