6533b857fe1ef96bd12b4ebd
RESEARCH PRODUCT
Observation of ${{e^+e^- \rightarrow D_s^+} \overline{ D}^{\bf (*)0} {K^-}}$ and study of the P -wave ${{D_s}}$ mesons
M. RichterZ. NingQ. LiuL. L. MaL. GongS. J. ZhaoA. AmorosoG. R. LiaoG. F. XuS. GuA. DbeyssiQ. J. XuB. Q. WangX. Y. JiangP. L. WangAngelo RivettiMuhammad IrshadX. Y. SongJ. C. ChenX. TangXuanhong LouM. QiDean LiuDean LiuM. RoloH. J. YangH. J. YangNasser Kalantar-nayestanakiW. L. ChangH. J. LiMichael PapenbrockF. YanF. De MoriC. Morales MoralesH. LeithoffL. ZhangY. PanJ. ChaiMeng WangY. H. ZhengShan JinK. GoetzenQ. A. MalikG. MezzadriF. CossioK. J. ZhuJ. H. YinCong-feng QiaoZ. Q. YangF. LiF. C. MaJ. F. HuJ. F. HuJ. F. SunJ. S. HuangY. NefedovC. X. LiuN. Yu. MuchnoiN. Yu. MuchnoiX. S. KangZhiqing LiuY. H. ZhangG. X. SunJ. V. BennettZhiyong ZhangR. FarinelliX. F. WangX. L. JiG. A. ChelkovG. A. ChelkovG. A. ChelkovS. MarcelloM. ShaoY. T. GuY. ZengS. L. OlsenZhe SunS. LussoI. K. KeshkL. J. WuM. Y. DongQ. M. MaY. ZhangA. MustafaYunlong ZhangH. L. LiuZ. JiaoFu-hu LiuD. H. ZhangD. BettoniZ. Y. WangW. G. LiH. L. MaM. N. AchasovM. N. AchasovL. P. ZhouP. R. LiJ. L. ZhangY. J. MoF. F. SuiM. H. GuR. KiuchiH. B. LiuJ. F. QiuS. B. LiuY. B. ChenXiaofeng ZhuJ. Z. ZhangJ. J. SongR. PolingH. L. JiangL. FavaY. F. WangY. YuanY. S. ZhuL. SunJianping ZhengYu ZhangH. Y. ShengM. G. ZhaoY. H. YangX. X. MaR. P. GuoZ. X. MengC. X. YuT. JohanssonJ. F. ChangC. SowaY. B. ZhaoD. M. LiH. MuramatsuY. M. MaZ. P. MaoJ. H. ZouTao LuoT. J. MinY. K. SunB. ZhengR. G. PingW. ImoehlZ. J. XiaoO. B. KolcuO. B. KolcuJ. DongH. J. LuJ. G. LuM. PelizaeusJ. FangZ. G. WangS. S. SunH. Y. ZhangX. N. MaHaiwen LiuY. T. LiangCui LiM. DestefanisZ. GaoXiaoyu ZhouB. X. YuX. A. XiongYang ZhangM. BertaniZ. HaddadiL. YangQiang ZhaoZ. A. LiuQ. P. JiM. KuemmelMatthew Glenn KurthCh. RosnerS. AhmedY. X. YangF. E. MaasX. S. QinX. CaiL. LavezziS. NisarS. NisarG. F. ChenS. SpataroX. L. GaoX. P. XuW. ShanC. J. TangA. A. ZafarY. HuA. SarantsevA. SarantsevY. P. LuKai LiuT. HuY. BanP. WeidenkaffF. H. HeinsiusJ. Y. ZhangHuanhuan LiuQ. P. JiM. AlbrechtA. CalcaterraZ. G. ZhaoMinglin MaC. DongL. Z. LiaoS. SosioD. H. WeiJ. S. LangeT. HussainS. P. WenX. R. ZhouO. BakinaH. LiangI. B. NikolaevI. B. NikolaevR. E. MitchellX. Q. HaoCheng LiX. Y. MaG. FeliciJoachim PetterssonLei LiY. K. HengY. T. TanS. QianJialun PingY. Z. SunLiqing XuH. H. ZhangK. ZhangX. Y. ShenW. D. LiW. X. GongH. S. ChenW. GradlM. FritschB. T. TsedneeM. RipkaBibo KeP. X. ShenZ. WuXiang ZhouZ. J. SunX. Y. ZhangA. YuncuA. YuncuJun-yi ZhangY. P. GuoD. Y. WangZhiqing ZhangW. B. YanC. X. LinS. MaldanerM. RumpGang ZhaoZ. P. ZhangKe LiuJ. MinY. FuH. L. DaiIgor BoykoY. DingX. H. MoL. S. WangG. F. CaoJ. C. LiD. W. BennettZujian WangM. H. YeS. PacettiX D ShiY. G. XieB. KopfX. H. SunJ. Y. LiuJ. B. LiuY. BaiK. H. RashidK. H. RashidJ. ZhuangM. KavatsyukY. H. YanJ. LibbyS. F. ZhangYaquan FangL. M. GuM. X. LuoY. J. MaoF. A. HarrisK. L. HeL. L. WangH. X. YangJ. W. ZhaoA. PitkaD. V. DedovichI. GarziaH. CaiP. KieseY. J. SunYifan YangKe LiXu ZhouB. J. LiuL. KochA. KhoukazQ. GaoY. N. GaoM. Z. WangY. C. ZhuM. H. YeS. X. DuJimin ZhaoR. A. BriereMagnus WolkeQ. AnS. L. YangY. F. LiangKlaus PetersKlaus PetersX. K. ZhouJ. Z. FanK. SchoenningQ. Y. LiB. S. ZouP. L. LiFang LiuX. S. JiangNiklaus BergerI. DenysenkoW. C. YanT. HeldQ. L. XiuB. GarillonH. B. LiHuihui LiuY. P. LuA. G. DenigZ. L. DouW. KühnR. Baldini FerroliD. P. JinC. L. LuoH. H. WangQ. ZhouWei XuS. J. ChenL. Y. DongB. Y. ZhangC. C. ZhangB. ZhongL. B. GuoJ. G. MesschendorpJ. Q. ZhangA. N. ZhuUlrich WiednerTao ZhangTao ZhangS. L. NiuZ. Y. YouZ. Y. YouZ. A. ZhuF. Y. LiX. Q. LiY. F. LongT. WeberR. X. YangM. GrecoN. QinJ. P. DaiJ. P. DaiXu ShanX. N. LiZongyuan WangXiao-rui LyuHaiping PengB. X. ZhangC. P. ShenK. Y. LiuKe WangS. Q. QuZ. B. LiW. Ikegami AnderssonJ. D. LuXiaozhong HuangT. KhanFenfen AnB. L. WangA. Q. GuoC. W. WangG. RongT. C. ZhaoX. LiuQ. OuyangY. G. GaoJ. ZhuAndrzej KupscF. FeldbauerW. P. WangZ. H. QinS. S. FangZ. L. HuangFeng LiuM. L. ChenC. F. RedmerSerkant Ali CetinSerkant Ali CetinM. AblikimA. ZhemchugovA. ZhemchugovX. T. HuangY. B. LiuV. PrasadS. HanD. Y. LiuJ. B. JiaoP. L. WangYi-tao WangX. L. LuoL. H. WuM. SavrieK. BegzsurenYi JinJ. W. LiL. XiaF. BianchiR. M. WangY. J. XiaoN. HueskenGuangshun HuangL. YanM. KuessnerI. UmanBingxuan LiuBingxuan LiuW. S. ChengYao ZhangG. LiA. GilmanC. D. FuY. H. XieC. Q. FengZ. Y. DengP. LarinM. MaggioraLing ZhaoXingguo LiP. W. LuoLei ZhaoZ. L. HouL. K. LiX. B. JiM. TiemensC. Z. YuanP. PatteriR. KliemtG. Y. TangA. MangoniA. GuskovS. NakhoulS. NakhoulJie YuK. J. ZhuJie ZhaoD. X. LinG. CibinettoH. M. HuJ. W. ZhangF. NerlingF. NerlingM. AlekseevT. Y. QiY. X. XiaS. H. Zhusubject
PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationFOS: Physical sciencesAstronomy and Astrophysics01 natural sciencesHigh Energy Physics - ExperimentLuminosityHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesBorn approximation010306 general physicsInstrumentationdescription
Studies of $e^+e^- \to D_s^+ \overline{D}{}^{(*)0}K^-$ and the $P$-wave charmed-strange mesons are performed based on an $e^+e^-$ collision data sample corresponding to an integrated luminosity of 567 pb$^{-1}$ collected with the BESIII detector at $\sqrt{s}= 4.600$ GeV. The processes of $e^+e^-\to D_s^+ \overline{D}{*}^{0} K^-$ and $D_s^+ \overline{D}{}^{0} K^-$ are observed for the first time and are found to be dominated by the modes $D_s^+ D_{s1}(2536)^-$ and $D_s^+ D^*_{s2}(2573)^-$, respectively. The Born cross sections are measured to be $\sigma^{B}(e^+e^-\to D_s^+ \overline{D}{*}^{0} K^-) = (10.1\pm2.3\pm0.8) pb$ and $\sigma^{B}(e^+e^-\to D_s^+ \overline{D}{}^{0} K^-) = (19.4\pm2.3\pm1.6) pb$, and the products of Born cross section and the decay branching fraction are measured to be $\sigma^{B}(e^+e^-\to D_s^+D_{s1}(2536)^- + c.c.)\cdot\mathcal{B}(D_{s1}(2536)^- \to \overline{D}{*}^{0} K^-) = (7.5 \pm 1.8 \pm 0.7) pb$ and $\sigma^{B}(e^+e^-\to D_s^+ D^*_{s2}(2573)^- + c.c.)\cdot\mathcal{B}(D^*_{s2}(2573)^- \to \overline{D}{}^{0} K^-) = (19.7 \pm 2.9 \pm 2.0) pb$. For the $D_{s1}(2536)^-$ and $D^*_{s2}(2573)^-$ mesons, the masses and widths are measured to be $M(D_{s1}(2536)^-) = (2537.7 \pm 0.5 \pm 3.1)~MeV/c^2,$ $ \Gamma(D_{s1}(2536)^-)) = (1.7\pm 1.2 \pm 0.6)~\rm MeV,$ and $M(D^*_{s2}(2573)^-) = (2570.7\pm 2.0 \pm 1.7)~MeV/c^2,$ $\Gamma(D^*_{s2}(2573)^-) = (17.2 \pm 3.6 \pm 1.1)~\rm MeV.$ The spin-parity of the $D^*_{s2}(2573)^-$ meson is determined to be $J^P=2^{+}$. In addition, the process $e^+e^-\to D_s^+ \overline{D}{}^{(*)0} K^-$ are searched for using the data samples taken at four (two) center-of-mass energies between 4.416 (4.527) and 4.575 GeV, and upper limits at the $90\%$ confidence level on the cross sections are determined.
year | journal | country | edition | language |
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2018-12-23 | Chinese Physics C |