Study of B→ppˉππB \to p {\bar p} ππ

preprint2019arXivOpen access
K. ChuM. -Z. WangI. AdachiH. AiharaS. Al SaidD. M. AsnerV. AulchenkoT. AushevR. AyadV. BabuI. BadhreesS. BahinipatiA. M. BakichP. BeheraC. BelenoJ. BennettV. BhardwajB. BhuyanJ. BiswalA. BobrovG. BonviciniA. BozekM. BrackoM. CampajolaL. CaoD. CervenkovP. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. CunliffeN. DashF. Di CapuaS. Di CarloZ. DolezalT. V. DongS. EidelmanD. EpifanovJ. E. FastT. FerberA. FreyB. G. FulsomR. GargV. GaurN. GabyshevA. GarmashA. GiriP. GoldenzweigB. GolobO. HartbrichK. HayasakaH. HayashiiW. -S. HouC. -L. HsuT. IijimaK. InamiA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsH. B. JeonY. JinD. JoffeK. K. JooG. KaryanT. KawasakiD. Y. KimS. H. KimK. KinoshitaP. KodysS. KorparP. KrizanR. KroegerP. KrokovnyR. KulasiriY. -J. KwonY. -T. LaiI. S. LeeS. C. LeeL. K. LiL. Li GioiJ. LibbyK. LieretD. LiventsevT. LuoM. MasudaD. MatvienkoM. MerolaK. MiyabayashiR. MizukT. MoriR. MussaE. NakanoT. NakanoM. NakaoK. J. NathM. NayakN. K. NisarS. NishidaK. NishimuraH. OnoY. OnukiP. OskinP. PakhlovG. PakhlovaB. PalT. PangS. PardiC. W. ParkH. ParkS. -H. ParkS. PaulT. K. PedlarR. PestotnikL. E. PiilonenV. PopovE. PrencipeM. T. PrimP. K. ResmiM. RitterA. RostomyanN. RoutG. RussoD. SahooY. SakaiS. SandilyaL. SanteljV. SavinovO. SchneiderG. SchnellJ. SchuelerC. SchwandaY. SeinoK. SenyoM. E. SeviorC. P. ShenJ. -G. ShiuE. SolovievaM. StaricZ. S. StottlerT. SumiyoshiW. SutcliffeM. TakizawaU. TamponiK. TanidaF. TenchiniT. UglovY. UnnoS. UnoP. UrquijoY. UsovG. VarnerA. VinokurovaA. VossenB. WangC. H. WangP. WangX. L. WangJ. WiechczynskiE. WonS. B. YangH. YeJ. YeltonJ. H. YinY. YusaZ. P. ZhangV. ZhilichV. ZhukovaV. Zhulanov

Abstract

Using a data sample of 772×106772 \times 10^6 BB pairs collected on the Υ(4S)Υ(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e−e^+e^- collider, we report the observations of B0→ppˉπ+π−B^0\to p{\bar p}π^+π^- and B+→ppˉπ+π0B^+ \to p{\bar p}π^+π^0. We measure a decay branching fraction of (0.83±0.17±0.17)×10−6(0.83 \pm 0.17 \pm 0.17) \times 10^-6 in B0→ppˉπ+π−B^0\to p{\bar p}π^+π^- for Mπ+π−<1.22GeV/c2M_{π^+π^-} < 1.22 GeV/c^2 with a significance of 5.5 standard deviations. The contribution from B0→ppˉK0B0 \to p{\bar p}K^0 is excluded. We measure a decay branching fraction of (4.58±1.17±0.67)×10−6(4.58 \pm 1.17 \pm 0.67) \times 10^-6 for B+→ppˉπ+π0B^+ \to p{\bar p}π^+π^0 with Mπ+π0<1.3GeV/c2M_{π^+π^0} < 1.3 GeV/c^2 with a significance of 5.4 standard deviations. We study the difference of the MppˉM_{p{\bar p}} distributions in B0→ppˉπ+π−B^0\to p{\bar p}π^+π^- and B+→ppˉπ+π0B^+ \to p{\bar p}π^+π^0.

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