Study of J/ψ→ppˉJ/ψ\to p\bar{p} and J/ψ→nnˉJ/ψ\to n\bar{n}

preprint2012arXivOpen access
BESIII CollaborationM. AblikimM. N. AchasovD. J. AmbroseF. F. AnQ. AnZ. H. AnJ. Z. BaiR. B. FerroliY. BanJ. BeckerN. BergerM. B. BertaniJ. M. BianE. BogerO. BondarenkoI. BoykoR. A. BriereV. BytevX. CaiA. C. CalcaterraG. F. CaoJ. F. ChangG. ChelkovG. ChenH. S. ChenJ. C. ChenM. L. ChenS. J. ChenY. ChenY. B. ChenH. P. ChengY. P. ChuD. Cronin-HennessyH. L. DaiJ. P. DaiD. DedovichZ. Y. DengA. DenigI. DenysenkoM. DestefanisW. M. DingY. DingL. Y. DongM. Y. DongS. X. DuJ. FangS. S. FangL. FavaF. FeldbauerC. Q. FengC. D. FuJ. L. FuY. GaoC. GengK. GoetzenW. X. GongW. GradlM. GrecoM. H. GuY. T. GuY. H. GuanA. Q. GuoL. B. GuoY. P. GuoY. L. HanX. Q. HaoF. A. HarrisK. L. HeM. HeZ. Y. HeT. HeldY. K. HengZ. L. HouH. M. HuJ. F. HuT. HuB. HuangG. M. HuangJ. S. HuangX. T. HuangY. P. HuangT. HussainC. S. JiQ. JiX. B. JiX. L. JiL. K. JiaL. L. JiangX. S. JiangJ. B. JiaoZ. JiaoD. P. JinS. JinF. F. JingN. Kalantar-NayestanakiM. KavatsyukW. KuehnW. LaiJ. S. LangeJ. K. C. LeungC. H. LiCheng LiCui LiD. M. LiF. LiG. LiH. B. LiJ. C. LiK. LiLei LiN. B. LiQ. J. LiS. L. LiW. D. LiW. G. LiX. L. LiX. N. LiX. Q. LiX. R. LiZ. B. LiH. LiangY. F. LiangY. T. LiangG. R. LiaoX. T. LiaoB. J. LiuC. L. LiuC. X. LiuC. Y. LiuF. H. LiuFang LiuFeng LiuH. LiuH. B. LiuH. H. LiuH. M. LiuH. W. LiuJ. P. LiuKun LiuKai LiuK. Y. LiuP. L. LiuS. B. LiuX. LiuX. H. LiuY. B. LiuY. LiuZ. A. LiuZhiqiang LiuZhiqing LiuH. LoehnerG. R. LuH. J. LuJ. G. LuQ. W. LuX. R. LuY. P. LuC. L. LuoM. X. LuoT. LuoX. L. LuoM. LvC. L. MaF. C. MaH. L. MaQ. M. MaS. MaT. MaX. Y. MaY. MaF. E. MaasM. MaggioraQ. A. MalikH. MaoY. J. MaoZ. P. MaoJ. G. MesschendorpJ. MinT. J. MinR. E. MitchellX. H. MoC. Morales MoralesC. MotzkoN. Yu. MuchnoiY. NefedovC. NicholsonI. B. NikolaevZ. NingS. L. OlsenQ. OuyangS. P. PacettiJ. W. ParkM. PelizaeusK. PetersJ. L. PingR. G. PingR. PolingE. PrencipeC. S. J. PunM. QiS. QianC. F. QiaoX. S. QinY. QinZ. H. QinJ. F. QiuK. H. RashidG. RongX. D. RuanA. SarantsevJ. SchulzeM. ShaoC. P. ShenX. Y. ShenH. Y. ShengM. R. ShepherdX. Y. SongS. SpataroB. SpruckD. H. SunG. X. SunJ. F. SunS. S. SunX. D. SunY. J. SunY. Z. SunZ. J. SunZ. T. SunC. J. TangX. TangE. H. ThorndikeH. L. TianD. TothM. U. UlrichG. S. VarnerB. WangB. Q. WangK. WangL. L. WangL. S. WangM. WangP. WangP. L. WangQ. WangQ. J. WangS. G. WangX. F. WangX. L. WangY. D. WangY. F. WangY. Q. WangZ. WangZ. G. WangZ. Y. WangD. H. WeiP. WeidenkaffQ. G. WenS. P. WenM. W. WernerU. WiednerL. H. WuN. WuS. X. WuW. WuZ. WuL. G. XiaZ. J. XiaoY. G. XieQ. L. XiuG. F. XuG. M. XuH. XuQ. J. XuX. P. XuY. XuZ. R. XuF. XueZ. XueL. YanW. B. YanY. H. YanH. X. YangT. YangY. YangY. X. YangH. YeM. YeM. H. YeB. X. YuC. X. YuJ. S. YuS. P. YuC. Z. YuanW. L. YuanY. YuanA. A. ZafarA. Z. ZalloY. ZengB. X. ZhangB. Y. ZhangC. C. ZhangD. H. ZhangH. H. ZhangH. Y. ZhangJ. ZhangJ. G. ZhangJ. Q. ZhangJ. W. ZhangJ. Y. ZhangJ. Z. ZhangL. ZhangS. H. ZhangT. R. ZhangX. J. ZhangX. Y. ZhangY. ZhangY. H. ZhangY. S. ZhangZ. P. ZhangZ. Y. ZhangG. ZhaoH. S. ZhaoJ. W. ZhaoK. X. ZhaoLei ZhaoLing ZhaoM. G. ZhaoQ. ZhaoS. J. ZhaoT. C. ZhaoX. H. ZhaoY. B. ZhaoZ. G. ZhaoA. ZhemchugovB. ZhengJ. P. ZhengY. H. ZhengZ. P. ZhengB. ZhongJ. ZhongL. ZhouX. K. ZhouX. R. ZhouC. ZhuK. ZhuK. J. ZhuS. H. ZhuX. L. ZhuX. W. ZhuY. M. ZhuY. S. ZhuZ. A. ZhuJ. ZhuangB. S. ZouJ. H. ZouJ. X. Zuo

Abstract

The decays J/ψ→ppˉJ/ψ\to p\bar{p} and J/ψ→nnˉJ/ψ\to n\bar{n} have been investigated with a sample of 225.2 million J/ψJ/ψ events collected with the BESIII detector at the BEPCII e+e−e^+e^- collider. The branching fractions are determined to be B(J/ψ→ppˉ)=(2.112±0.004±0.031)×10−3\mathcal{B}(J/ψ\to p\bar{p})=(2.112\pm0.004\pm0.031)\times10^{-3} and B(J/ψ→nnˉ)=(2.07±0.01±0.17)×10−3\mathcal{B}(J/ψ\to n\bar{n})=(2.07\pm0.01\pm0.17)\times10^{-3}. Distributions of the angle θθ between the proton or anti-neutron and the beam direction are well described by the form 1+αcos⁡2θ1+α\cos^2θ, and we find α=0.595±0.012±0.015α=0.595\pm0.012\pm0.015 for J/ψ→ppˉJ/ψ\to p\bar{p} and α=0.50±0.04±0.21α=0.50\pm0.04\pm0.21 for J/ψ→nnˉJ/ψ\to n\bar{n}. Our branching-fraction results suggest a large phase angle between the strong and electromagnetic amplitudes describing the J/ψ→NNˉJ/ψ\to N\bar{N} decay.

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