Dalitz analysis of D0→K−π+ηD^{0}\to K^{-}π^{+}η decays at Belle

preprint2020arXivOpen access
Belle CollaborationY. Q. ChenL. K. LiW. B. YanI. AdachiH. AiharaS. Al SaidD. M. AsnerH. AtmacanV. AulchenkoT. AushevR. AyadV. BabuI. BadhreesS. BahinipatiP. BeheraJ. BennettV. BhardwajT. BilkaJ. BiswalA. BozekM. BračkoT. E. BrowderM. CampajolaL. CaoD. ČervenkovM. -C. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinH. E. ChoK. ChoS. -K. ChoiY. ChoiS. ChoudhuryD. CinabroS. CunliffeN. DashG. De NardoF. Di CapuaZ. DoležalT. V. DongS. EidelmanD. EpifanovJ. E. FastT. FerberD. FerlewiczB. G. FulsomR. GargV. GaurN. GabyshevA. GarmashA. GiriP. GoldenzweigB. GolobO. HartbrichK. HayasakaH. HayashiiW. -S. HouC. -L. HsuK. InamiG. IngugliaA. IshikawaR. ItohM. IwasakiY. IwasakiW. W. JacobsE. -J. JangH. B. JeonS. JiaY. JinK. K. JooK. H. KangG. KaryanT. KawasakiD. Y. KimS. H. KimT. D. KimmelK. KinoshitaP. KodyšS. KorparP. KrižanR. KroegerP. KrokovnyT. KuhrR. KulasiriR. KumarA. KuzminY. -J. KwonK. LalwaniJ. S. LangeI. S. LeeS. C. LeeY. B. LiL. Li GioiJ. LibbyK. LieretD. LiventsevJ. MacNaughtonC. MacQueenM. MasudaD. MatvienkoM. MerolaK. MiyabayashiR. MizukS. MohantyR. MussaM. NakaoZ. NatkaniecM. NayakS. NishidaS. OgawaH. OnoP. OskinP. PakhlovG. PakhlovaS. PardiH. ParkS. PatraS. PaulT. K. PedlarR. PestotnikL. E. PiilonenT. PodobnikV. PopovE. PrencipeM. T. PrimA. RabusovM. RitterM. RöhrkenN. RoutG. RussoD. SahooT. SanukiV. SavinovO. SchneiderG. SchnellJ. SchuelerC. SchwandaA. J. SchwartzY. SeinoK. SenyoM. E. SeviorM. ShapkinV. ShebalinJ. -G. ShiuA. SokolovE. SolovievaM. StaričZ. S. StottlerM. SumihamaT. SumiyoshiW. SutcliffeM. TakizawaK. TanidaF. TenchiniK. TrabelsiM. UchidaT. UglovS. UnoP. UrquijoG. VarnerV. VorobyevC. H. WangE. WangM. -Z. WangP. WangM. WatanabeE. WonX. XuS. B. YangH. YeJ. H. YinC. Z. YuanY. YusaZ. P. ZhangV. ZhilichV. ZhukovaV. Zhulanov

Abstract

We present the results of the first Dalitz plot analysis of the decay D0→K−π+ηD^{0}\to K^{-}π^{+}η. The analysis is performed on a data set corresponding to an integrated luminosity of 953 fb−1\rm{fb}^{-1} collected by the Belle detector at the asymmetric-energy e+e−e^{+}e^{-} KEKB collider. The Dalitz plot is well described by a combination of the six resonant decay channels Kˉ∗(892)0η\bar{K}^{*}(892)^0η, K−a0(980)+K^{-}a_0(980)^+, K−a2(1320)+K^{-}a_2(1320)^+, Kˉ∗(1410)0η\bar{K}^{*}(1410)^0η, K∗(1680)−π+K^{*}(1680)^-π^{+} and K2∗(1980)−π+K_2^{*}(1980)^-π^{+}, together with KπKπ and KηKη S-wave components. The decays K∗(1680)−→K−ηK^{*}(1680)^{-}\to K^{-}η and K2∗(1980)−→K−ηK_{2}^{*}(1980)^{-}\to K^{-}η are observed for the first time. We measure ratio of the branching fractions, B(D0→K−π+η)B(D0→K−π+)=0.500±0.002(stat)±0.020(syst)±0.003(BPDG)\frac{\mathcal{B}(D^{0}\to K^{-}π^{+}η)}{\mathcal{B}(D^{0}\to K^{-}π^{+})}=0.500\pm0.002{\rm(stat)}\pm0.020{\rm(syst)}\pm0.003{\rm (\mathcal{B}_{PDG})}. Using the Dalitz fit result, the ratio B(K∗(1680)→Kη)B(K∗(1680)→Kπ)\frac{\mathcal{B}(K^{*}(1680)\to Kη)}{\mathcal{B}(K^{*}(1680)\to Kπ)} is measured to be 0.11±0.02(stat)−0.04+0.06(syst)±0.04(BPDG)0.11\pm0.02{\rm(stat)}^{+0.06}_{-0.04}{\rm(syst)}\pm0.04{\rm(\mathcal{B}_{\text{PDG}})}; this is much lower than the theoretical expectations (≈1\approx1) made under the assumption that K∗(1680)K^{*}(1680) is a pure 13D11^{3}D_1 state. The product branching fraction B(D0→[K2∗(1980)−→K−η]π+)=(2.2−1.9+1.7)×10−4\mathcal{B}(D^0\to [K_2^{*}(1980)^-\to K^{-}η]π^{+})=(2.2^{+1.7}_{-1.9})\times10^{-4} is determined. In addition, the πη′πη^{\prime} contribution to the a0(980)±a_0(980)^{\pm} resonance shape is confirmed with 10.1σσ statistical significance using the three-channel Flatté model. We also measure B(D0→Kˉ∗(892)0η)=(1.41−0.12+0.13)%\mathcal{B}(D^0\to\bar{K}^{*}(892)^0η)=(1.41^{+0.13}_{-0.12})\%. This is consistent with, and more precise than, the current world average (1.02±0.30)%(1.02\pm0.30)\%, deviates with a significance of more than 3σ3σ from the theoretical predictions of (0.51-0.92)%.

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