6533b836fe1ef96bd12a12e7
RESEARCH PRODUCT
Amplitude analysis of theD+→KS0π+π0Dalitz plot
D. J. AmbroseY. H. GuanZ. H. WangKai LiuW. B. YanX. R. ChenXiao-tong LuJ. B. JiaoM. N. AchasovC. F. RedmerXiaocong AiY. NefedovM. AlbrechtS. PacettiH. L. MaD. M. LiS. MaX. T. HuangW. D. LiD. LiH. MuramatsuA. A. ZafarG. RongD. TothH. J. LuJ. G. LuH. P. HuangM. PelizaeusJ. Z. BaiM. G. ZhaoCui LiY. T. LiangF. E. MaasT. HuXuejun WangZ. B. LiS. L. ZangM. Y. DongMichael WernerM. KavatsyukH. B. LiuF. LiF. C. MaY. X. YangJ. H. ZouO. FuksGuangming HuangC. S. JiS. S. SunY. P. ChuX. B. JiS. QianJialun PingZ. WuL. W. JiangB. X. ZhangX. LiuZ. J. XiaoT. GuoX. Y. ZhangM. LaraSerkant Ali CetinM. R. ShepherdJ. S. HuangY. H. ZhengCong-feng QiaoY. J. SunQ. ZhaoY. Z. SunY. P. LuZhiqing ZhangC. X. LiuO. AlbayrakZ. A. LiuXiang ZhouI. TapanY. H. YanJ. F. QiuN. Yu. MuchnoiL. FavaX. S. KangHeng-yun YeR. E. MitchellJ. W. ZhaoGang ZhaoH. LiangK. LiY. H. ZhangXiangdong RuanFang LiuS. J. ChenY. BanP. WeidenkaffO. BondarenkoD. Cronin-hennessyY. C. ZhuS. P. WenQ. P. JiX. H. MoI. DenysenkoL. S. WangG. LiZ. G. WangH. Y. ZhangFeng LiuR. Baldini FerroliX. S. QinM. H. YeM. AblikimX. R. ZhouC. D. FuC. Q. FengCheng LiS. L. OlsenZ. Y. WangE. BogerRoy A. BriereK. GoetzenG. F. ChenW. KuehnB. Y. ZhangQ. J. XuY. J. MaoJ. Y. ZhangZ. Y. DengX. S. JiangT. HeldQ. LiuL. H. WuX. K. ChuL. L. WangH. CaiX. N. LiS. SchumannXingguo LiB. SpruckHaiping PengHai YuE. H. ThorndikeYao WangY. K. HengL. Q. QinJ. Q. ZhangJ. H. LiuH. L. LuKe WangQ. GaoY. N. GaoJ. M. BianY. ZhangQ. AnQun-yao WangZhenyu ZhangW. LaiL. G. XiaP. LarinP. L. WangW. C. YanJ. P. DaiR. PolingJ. Z. FanO. CakirJ. C. ChenXuanhong LouM. H. GuFenfen AnY. F. WangX. C. ChenZhiqiang LiuMiao HeS. BraunNasser Kalantar-nayestanakiA. ZalloJifeng HuL. P. ZhouT. C. ZhaoYang QinJie YuM. H. YeH. Y. ShengC. Morales MoralesZ. P. MaoC. X. YuY. X. XiaTao LuoM. KornicerJ. V. BennettC. GengT. J. MinK. J. ZhuH. P. ChengB. X. YuJ. FangTao LiL. Y. DongB. ZhengR. G. PingX. Y. MaH. MoeiniW. X. GongH. S. ChenW. M. DingShujun ZhaoC. B. ZhangD. X. LinI. B. NikolaevK. H. RashidM. ShaoY. T. GuH. L. DaiIgor BoykoC. H. LiX. Y. ZhouYaquan FangAlexey ZhemchugovH. M. HuQ. J. LiG. F. XuJ. W. ZhangS. JinX. Q. LiM. GrecoX. L. KangA. SarantsevD. H. WeiJ. S. LangeQ. W. ZhaoQ. M. MaK. SchoenningB. S. ZouB. KlossX. Y. NiuK. Y. LiuY. YuanY. S. ZhuX. Y. SongTord JohanssonJ. C. LiJ. ZhuangM. X. LuoJian WeiYucheng HuangD. V. DedovichA. CalcaterraZ. G. ZhaoL. HuangZ. J. SunH. LoehnerZhiqing LiuH. B. LiA. G. DenigJ. F. ChangC. L. LuoC. C. ZhangB. ZhongL. B. GuoLei LiUlrich WiednerT. MaX. CaiZ. NingN. WuKrisztian PetersY. L. HanX. K. ZhouJianping ZhengChi ZhangM. LvL. L. JiangZ. XueJ. J. ZhangM. DestefanisJ. F. SunY. ZengF. A. HarrisZhe SunQ. A. MalikC. DongY. B. ChenXiaofeng ZhuJ. Z. ZhangC. HuX. TangB. WangK. J. ZhuXuantong ZhangK. MoriyaQ. L. XiuW. L. YuanQ. OuyangS. S. FangY. B. LiuP. L. WangX. L. LuoW. P. WangY. B. ZhaoW. ShanJ. DongY. Q. WangS. NisarC. J. TangY. P. LuD. XiaoM. MaggioraLing ZhaoLei ZhaoZ. Y. HeZ. L. HouYang YangD. Y. WangC. Z. YuanY. P. GuoZ. P. ZhangGuangshun HuangZujian WangH. H. ZhangG. A. ChelkovM. QiX. H. ZhaoP. R. LiS. B. LiuJ. MinB. KopfG. X. SunLi YanK. L. HeM. Z. WangZ. JiaoFu-hu LiuD. H. ZhangM. BertaniL. YangX. L. JiS. P. YuW. GradlM. RipkaA. Q. GuoTalib HussainW. M. SongY. G. XieLi ZhouS. X. DuM. LeyheZ. H. QinShan WangChuan LiuY. DingW. G. LiB. J. LiuS. SpataroX. P. XuG. S. VarnerG. R. LuH. M. LiuZ. A. ZhuG. F. CaoH. X. YangHuihui LiuC. P. ShenJ. P. LiuJ. G. MesschendorpQiunan XuY. J. MoQ. P. JiLiqing XuS. H. ZhangX. Y. ShenMagnus WolkeY. F. LiangD. P. JinDayong WangN. QinP. L. LiuI. UmanM. UllrichAndrzej KupscM. L. Chensubject
PhysicsNuclear and High Energy PhysicsParticle physicsAmplitude010308 nuclear & particles physicsPartial wave analysisElectron–positron annihilation0103 physical sciencesPiDalitz plot010306 general physics01 natural sciencesdescription
We perform an analysis of the D+ -> K-S(0)pi + (0)(pi) Dalitz plot using a data set of 2.92 fb(-1) of e(+) e(-) collisions at the (3770) mass accumulated by the BESIII experiment, in which 166694 candidate events are selected with a background of 15.1%. The Dalitz plot is found to be well represented by a combination of six quasitwo- body decay channels [k(SP)(0)(+) (1450)(+,) ] plus a small nonresonant component. Using the fit fractions from this analysis, partial branching ratios are updated with higher precision than previous measurements.
year | journal | country | edition | language |
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2014-03-11 | Physical Review D |