$e^+e^- \to γX(3872)$ near the $D^* {\bar D}^*$ threshold

dc.creatorDubynskiy, S.
dc.creatorVoloshin, M. B.
dc.date2006-09-28
dc.date.accessioned2026-07-07T11:05:49Z
dc.date.available2026-07-07T11:05:49Z
dc.descriptionWe evaluate the cross section of the process $e^+e^- \to γX(3872)$ in terms of the content of the $D^{*0} {\bar D}^0$ `molecular' component in the wave function of the resonance X(3872). If this component is dominating, the cross section of the reaction $e^+e^- \to γX(3872)$ can reach up to about $10^{-3}$ of that for $e^+e^- \to D^* {\bar D}^*$ at energy slightly above the $D^* {\bar D}^*$ threshold, and the considered process can be a realistic source of the X(3872) particles for the studies of this resonance.
dc.description8 pages, 1 figure
dc.identifierhttps://arxiv.org/abs/hep-ph/0609302
dc.identifierhttp://arxiv.org/abs/hep-ph/0609302
dc.identifierPhys.Rev.D74:094017,2006
dc.identifierdoi:10.1103/PhysRevD.74.094017
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/189324
dc.subjectHigh Energy Physics - Phenomenology
dc.title$e^+e^- \to γX(3872)$ near the $D^* {\bar D}^*$ threshold
dc.typetext

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