Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2560
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dc.contributor.authorBhardwaj, V.-
dc.date.accessioned2020-12-03T07:06:42Z-
dc.date.available2020-12-03T07:06:42Z-
dc.date.issued2016-
dc.identifier.citationPhysical Review D,93(11).en_US
dc.identifier.otherhttps://doi.org/10.1103/PhysRevD.93.112013-
dc.identifier.urihttps://journals.aps.org/prd/abstract/10.1103/PhysRevD.93.112013-
dc.identifier.urihttp://hdl.handle.net/123456789/2560-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractThe branching fractions of the Υ ( 1 S ) inclusive decays into final states with a J / ψ or a ψ ( 2 S ) are measured with improved precision to be B ( Υ ( 1 S ) → J / ψ + anything ) = ( 5.25 ± 0.13 ( stat ) ± 0.25 ( syst ) ) × 10 − 4 and B ( Υ ( 1 S ) → ψ ( 2 S ) + anything ) = ( 1.23 ± 0.17 ( stat ) ± 0.11 ( syst ) ) × 10 − 4 . The first search for Υ ( 1 S ) decays into X Y Z states that decay into a J / ψ or a ψ ( 2 S ) plus one or two charged tracks yields no significant signals for X Y Z states in any of the examined decay modes, and upper limits on their production rates in Υ ( 1 S ) inclusive decays are determined.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectDecaysen_US
dc.subjectPrecisionen_US
dc.subjectBranchingen_US
dc.subjectFractionsen_US
dc.titleSearch for X Y Z states in Υ ( 1 S ) inclusive decaysen_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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