Abstract

To take the full advantage of the ψ(3686) data set collected at e+e- collider at τ-charm energy region, a tag method is developed to directly measure the J/ψ meson decay branching fractions absolutely. The J/ψ meson decay can be measured with the J/ψ sample tagged by the two soft charged pions from the decay ψ(3686)→J/ψπ+π-. This method is illustrated by comparing the input and output branching fractions of J/ψ→γη with 106 million inclusive ψ(3686) Monte Carlo samples. The consistent result confirms the validity of the tag method.

Highlights

  • The firstly discovered charmonium J/ψ [1, 2], JPC = 1−−, is the lowest one among those which can be produced directly in e+e− annihilation

  • An energy scan experiment performed around the J/ψ resonance can solve the problem induced by interference effect, while it is not effective for the final states with undistinguishable backgrounds from other processes

  • The good photon candidate showers reconstructed from the barrel Electromagnetic Calorimeter (EMC) (| cos θ| < 0.80) must have a minimum energy of 25 MeV, while those in the end caps (0.86 < | cos θ| < 0.92) must have at least 50 MeV, where the energies deposited in nearby Time of Flight (TOF) counters are included

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Summary

Introduction

The summation of the measured J/ψ decay branching fraction is not more than 60% [15] without considering the interference between resonance and continuum amplitudes until now, which hampers the understanding of its properties. The J/ψ production and decay property are studied by using the data collected from e+e− collisions at the J/ψ resonance traditionally. At this energy, the events consist mostly of e+e− 󳨀→ J/ψ, e+e− 󳨀→ l+l− (l represents e, μ), with small amounts of three-flavor continuum and other processes such as γV, where V represents vector meson. Considering the large branching fraction of ψ(3686) 󳨀→ J/ψπ+π−, (34.67 ± 0.30)% [15], this sample can naturally be used to study the J/ψ decay. The feasibility of the method is verified by examining the input and output branching fractions of J/ψ 󳨀→ γη in the inclusive ψ(3686) Monte Carlo (MC) sample

BESIII Detector and Simulation
Introduction of the Method
General Track Selection
Reconstruction of Tag Side
Results
Conclusion
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