Study of D∗∗D^{**} production and light hadronic states in the Bˉ0→D∗+ωπ−\bar{B}^0 \to D^{*+} ωπ^- decay

preprint2015arXivOpen access
Belle CollaborationD. MatvienkoA. KuzminS. EidelmanA. AbdesselamI. AdachiH. AiharaS. Al SaidK. ArinsteinD. M. AsnerV. AulchenkoT. AushevR. AyadV. BabuI. BadhreesS. BahinipatiA. M. BakichV. BansalV. BhardwajB. BhuyanJ. BiswalA. BobrovA. BondarG. BonviciniA. BozekM. BračkoT. E. BrowderD. ČervenkovA. ChenB. G. CheonK. ChilikinR. ChistovK. ChoV. ChobanovaS. -K. ChoiD. CinabroJ. DalsenoJ. DingfelderZ. DoležalZ. DrásalA. DrutskoyD. DuttaD. EpifanovH. FarhatJ. E. FastT. FerberB. G. FulsomV. GaurN. GabyshevA. GarmashD. GetzkowR. GillardY. M. GohP. GoldenzweigB. GolobT. HaraK. HayasakaH. HayashiiX. H. HeW. -S. HouT. IijimaG. IngugliaA. IshikawaR. ItohY. IwasakiI. JaegleD. JoffeK. K. JooT. JuliusT. KawasakiD. Y. KimJ. B. KimJ. H. KimK. T. KimM. J. KimS. H. KimY. J. KimB. R. KoP. KodyšS. KorparP. KrokovnyR. KumarJ. S. LangeD. H. LeeL. Li GioiJ. LibbyD. LiventsevK. MiyabayashiH. MiyataR. MizukG. B. MohantyA. MollR. MussaE. NakanoM. NakaoT. NanutM. NayakN. K. NisarS. NishidaS. OgawaG. PakhlovaB. PalC. W. ParkH. ParkT. K. PedlarL. PesántezR. PestotnikM. PetričL. E. PiilonenC. PulvermacherE. RibežlM. RitterA. RostomyanY. SakaiS. SandilyaL. SanteljT. SanukiO. SchneiderG. SchnellC. SchwandaK. SenyoO. SeonM. E. SeviorM. ShapkinV. ShebalinC. P. ShenT. -A. ShibataJ. -G. ShiuB. ShwartzA. SibidanovF. SimonY. -S. SohnA. SokolovM. StaričM. StederM. SumihamaK. SumisawaU. TamponiK. TanidaY. TeramotoM. UchidaS. UeharaY. UnnoS. UnoP. UrquijoY. UsovC. Van HulseP. VanhoeferG. VarnerA. VinokurovaV. VorobyevM. N. WagnerC. H. WangM. -Z. WangP. WangY. WatanabeK. M. WilliamsE. WonH. YamamotoS. YashchenkoY. YookZ. P. ZhangV. ZhilichV. ZhulanovA. Zupanc

Abstract

We report on the first observations of Bˉ0→D1(2430)0ω\bar{B}^0 \to D_1(2430)^0 ω, Bˉ0→D1(2420)0ω\bar{B}^0 \to D_1(2420)^0 ω and Bˉ0→D2∗(2460)0ω\bar{B}^0 \to D^*_2(2460)^0 ω decays. The Bˉ0→D∗+ρ(1450)−\bar{B}^0 \to D^{*+} ρ(1450)^- decay is also observed. The branching fraction measurements are based on (771.6±10.6)×106(771.6 \pm 10.6)\times 10^6 BBˉB\bar{B} events collected at the Υ(4S)Υ(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e−e^+e^- collider. The fractions of longitudinal polarization of the D∗∗D^{**} states as well as partial wave fractions of the D1(2430)0D_1(2430)^0 are obtained. We also set a 90%90\% confidence level upper limit for the product of branching fractions of B(Bˉ0→D∗+b1(1235)−)×B(b1(1235)−→ωπ−)\mathcal{B}(\bar{B}^0 \to D^{*+} b_1(1235)^-) \times \mathcal{B}(b_1(1235)^- \to ωπ^-). The measurements show evidence of nontrivial final-state interaction phases for the ρρ-like amplitudes.

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