Angular analysis of B0→ϕK∗B^0 \to ϕK^{*} decays and search for CP violation at Belle

preprint2013arXivOpen access
Belle CollaborationM. PrimI. AdachiH. AiharaD. M. AsnerT. AushevA. M. BakichA. BalaB. BhuyanG. BonviciniA. BozekM. Bra\vT. E. BrowderD. \vM. -C. ChangP. ChangV. ChekelianA. ChenP. ChenB. G. CheonR. ChistovK. ChoV. ChobanovaY. ChoiD. CinabroM. DanilovZ. Dole\vZ. DrásalD. DuttaS. EidelmanH. FarhatM. FeindtT. FerberA. FreyV. GaurS. GangulyR. GillardY. M. GohB. GolobH. HayashiiM. HeiderY. HoshiW. -S. HouY. B. HsiungT. IijimaK. InamiA. IshikawaR. ItohI. JaegleT. JuliusD. H. KahH. KawaiT. KawasakiH. KichimiC. KieslingD. Y. KimH. O. KimJ. B. KimJ. H. KimM. J. KimY. J. KimK. KinoshitaJ. KlucarB. R. KoP. Kody\vP. Kri\vP. KrokovnyB. KronenbitterT. KuhrT. KumitaY. -J. KwonJ. S. LangeS. -H. LeeJ. LiJ. LibbyP. LukinD. MatvienkoK. MiyabayashiH. MiyataR. MizukG. B. MohantyA. MollN. MuramatsuR. MussaI. NakamuraE. NakanoM. NakaoM. NayakE. NedelkovskaC. NiebuhrN. K. NisarS. NishidaO. NitohY. OnukiG. PakhlovaH. ParkH. K. ParkT. K. PedlarR. PestotnikM. Petri\vL. E. PiilonenM. RitterM. RöhrkenA. RostomyanM. RozanskaH. SahooT. SaitoY. SakaiS. SandilyaT. SanukiY. SatoV. SavinovO. SchneiderG. SchnellC. SchwandaD. SemmlerK. SenyoM. E. SeviorM. ShapkinC. P. ShenT. -A. ShibataJ. -G. ShiuA. SibidanovY. -S. SohnA. SokolovE. SolovievaM. Stari\vM. StederT. SumiyoshiU. TamponiG. TatishviliY. TeramotoK. TrabelsiT. TsuboyamaM. UchidaS. UeharaT. UglovY. UnnoS. UnoY. UsovS. E. VahsenC. Van HulseP. VanhoeferG. VarnerV. VorobyevC. H. WangM. -Z. WangP. WangX. L. WangM. WatanabeY. WatanabeK. M. WilliamsE. WonY. YamashitaS. YashchenkoZ. P. ZhangV. ZhilichA. Zupanc

Abstract

We report the measurements of branching fractions and CP violation asymmetries in B0→ϕK∗B^0 \to ϕK^{*} decays obtained in an angular analysis using the full data sample of 772×106BBˉ772 \times 10^6 B\bar{B} pairs collected at the Υ(4S)Υ(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e−e^+ e^- collider. We perform a partial wave analysis to distinguish among scalar [B0→ϕ(Kπ)0∗B^0 \to ϕ(Kπ)^{*}_{0}], vector [B0→ϕK∗(892)0B^0 \to ϕK^{*}(892)^{0}] and tensor [B0→ϕK2∗(1430)0B^0 \to ϕK^{*}_{2}(1430)^{0}] components, and determine the corresponding branching fractions to be B[B0→ϕ(Kπ)0∗]=(4.3±0.4±0.4)×10−6\mathcal{B}[B^0 \to ϕ(Kπ)^{*}_{0}] = (4.3 \pm 0.4 \pm 0.4) \times 10^{-6}, B[B0→ϕK∗(892)0]=(10.4±0.5±0.6)×10−6\mathcal{B}[B^0 \to ϕK^{*}(892)^{0}] = (10.4 \pm 0.5 \pm 0.6) \times 10^{-6} and B[B0→ϕK2∗(1430)0]=(5.5−0.7+0.9±1.0)×10−6\mathcal{B}[B^0 \to ϕK^{*}_{2}(1430)^{0}] = (5.5 ^{+0.9}_{-0.7} \pm 1.0) \times 10^{-6}. We also measure the longitudinal polarization fraction fLf_L in B0→ϕK∗(892)0B^0 \to ϕK^{*}(892)^{0} and B0→ϕK2∗(1430)0B^0 \to ϕK^{*}_{2}(1430)^{0} decays to be 0.499±0.030±0.0180.499 \pm 0.030 \pm 0.018 and 0.918−0.060+0.029±0.0120.918 ^{+0.029}_{-0.060} \pm 0.012, respectively. The first quoted uncertainties are statistical and the second are systematic. In total, we measure 26 parameters related to branching fractions, polarization and CP violation in the B0→ϕK∗B^0 \to ϕK^{*} system. No evidence for CP violation is found.

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