667 research outputs found

    Observation of charmed strange meson pair production in Y(2S) decays and in e+e− annihilation at sqrt(s)=10.52 GeV

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    We observe the process Y(2S)→D(*)+s D−sJ and continuum production e+e-→D(*)+s D-sJ at sqrt(s)=10.52 GeV (and their charge conjugates) using the data samples collected by the Belle detector at KEKB, where D-sJ is Ds1(2536)− or D*s2(2573)−. Both D-sJ states are identified through their decay into KD(*). We measure the products of branching fractions B(Y(2S)→D(*)+s D−sJ)B(D-sJ→KD(*)) and the Born cross sections σBorn(e+e-→D(*)+s D-sJ)B(D-sJ→KD(*)), and then compare the ratios R1=B(Y(2S)→D(*)+s D−sJ)/B(Y(2S)→μ+μ−) for Y(2S) decays and R1=σBorn(e+e-→D(*)+s D-sJ)/σBorn(e+e-→μ+μ−) for continuum production. We obtain R1/R2=9.7±2.3±1.1, 6.8±2.1±0.8, 10.2±3.3±2.5, and 3.4±2.1±0.8 for the D+s Ds1(2536)−, D*+s Ds1(2536)−, D+s D*s2(2573)−, and D*+s D*s2(2573)− final states in the D-sJ→K−D(*)0 modes, respectively. The measured R1/R2 values indicate that the strong decay dominates in Y(2S)→D(*)+s D−sJ processes. We also measure the ratios of branching fractions B(Ds1(2536)−→K0SD*(2010)−)/B(Ds1(2536)−→K-D*(2007)0)=0.48±0.07±0.02 and B(D*s2(2573)−→K0SD-)/B(D*s2(2573)−→K-D0)=0.49±0.10±0.02, which are consistent with isospin symmetry. The second ratio is the first measurement of this quantity. Here, the first uncertainties are statistical and the second are systematic

    Observation of e+e- → ωχbJ (1P) and Search for Xb → ω Υ (1S) at s near 10.75 GeV

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    We study the processes e+e-→ωχbJ(1P) (J=0, 1, or 2) using samples at center-of-mass energies s=10.701, 10.745, and 10.805 GeV, corresponding to 1.6, 9.8, and 4.7 fb-1 of integrated luminosity, respectively. These data were collected with the Belle II detector during special operations of the SuperKEKB collider above the Υ(4S) resonance. We report the first observation of ωχbJ(1P) signals at s=10.745 GeV. By combining Belle II data with Belle results at s=10.867 GeV, we find energy dependencies of the Born cross sections for e+e-→ωχb1,b2(1P) to be consistent with the shape of the Υ(10753) state. These data indicate that the internal structures of the Υ(10753) and Υ(10860) states may differ. Including data at s=10.653 GeV, we also search for the bottomonium equivalent of the X(3872) state decaying into ωΥ(1S). No significant signal is observed for masses between 10.45 and 10.65 GeV/c2

    Observation of e+eωχbJ(1P)e^+e^-\to\omega\chi_{bJ}(1P) and search for XbωΥ(1S)X_b \to \omega\Upsilon(1S) at s\sqrt{s} near 10.75 GeV

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    We study the processes e+eωχbJ(1P)e^+e^-\to\omega\chi_{bJ}(1P) (JJ = 0, 1, or 2) using samples at center-of-mass energies s\sqrt{s} = 10.701, 10.745, and 10.805 GeV, corresponding to 1.6, 9.8, and 4.7 fb1^{-1} of integrated luminosity, respectively. These data were collected with the Belle II detector during a special run of the SuperKEKB collider above the Υ(4S)\Upsilon(4S) resonance. We report the first observation of ωχbJ(1P)\omega\chi_{bJ}(1P) signals at s\sqrt{s} = 10.745 GeV. By combining Belle II data with Belle results at s\sqrt{s} = 10.867 GeV, we find energy dependencies of the Born cross sections for e+eωχb1,b2(1P)e^+e^-\to \omega\chi_{b1,b2}(1P) to be consistent with the shape of the Υ(10753)\Upsilon(10753) state. Including data at s\sqrt{s} = 10.653 GeV, we also search for the bottomonium equivalent of the X(3872)X(3872) state decaying into ωΥ(1S)\omega\Upsilon(1S). No significant signal is observed for masses between 10.45 and 10.65 GeV/c2c^2

    Search for CPCP violation in D(s)+K+KS0h+hD^{+}_{(s)}\rightarrow K^{+}K^{0}_{S}h^{+}h^{-} (h=K,π)(h=K,\pi) decays and observation of the Cabibbo-suppressed decay Ds+K+KKS0π+D^{+}_{s}\rightarrow K^{+}K^{-}K^{0}_{S}\pi^{+}

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    We search for CPCP violation by measuring a TT-odd asymmetry in the Cabibbo-suppressed D+K+KS0π+πD^{+}\rightarrow K^{+}K^{0}_{S}\pi^{+}\pi^{-} decay, and in the Cabibbo-favored Ds+K+KS0π+πD^{+}_{s}\rightarrow K^{+}K^{0}_{S}\pi^{+}\pi^{-} and D+K+KKS0π+D^{+}\rightarrow K^{+}K^{-}K^{0}_{S}\pi^{+} decays. We use 980 fb1{\rm fb}^{-1} of data collected by the Belle detector running at the KEKB asymmetric-energy e+ee^{+}e^{-} collider. The C ⁣PC\!P-violating TT-odd parameter aCPT-odd{a}^{T\text{-}\rm{odd}}_{CP} is measured to be aCPT-odd(D+K+KS0π+π)=(0.34±0.87±0.32)%,{a}^{T\text{-}\rm{odd}}_{CP}(D^{+}\rightarrow K^{+}K^{0}_{S}\pi^{+}\pi^{-})=(0.34\pm0.87\pm0.32)\%, aCPT-odd(Ds+K+KS0π+π)=(0.46±0.63±0.38)%,{a}^{T\text{-}\rm{odd}}_{CP}(D^{+}_{s}\rightarrow K^{+}K^{0}_{S}\pi^{+}\pi^{-})=(-0.46\pm0.63\pm0.38)\%, and aCPT-odd(D+K+KKS0π+)=(3.34±2.66±0.35)%,{a}^{T\text{-}\rm{odd}}_{CP}(D^{+}\rightarrow K^{+}K^{-}K^{0}_{S}\pi^{+})=(-3.34\pm2.66\pm0.35)\%, where the first uncertainty is statistical and the second is systematic. We also report the first observation of the Cabibbo-suppressed decay Ds+K+KKS0π+D^{+}_{s}\rightarrow K^{+}K^{-}K^{0}_{S}\pi^{+}. The branching fraction is measured relative to that of the analogous Cabibbo-favored decay : B(Ds+K+KKS0π+)/B(Ds+K+KS0π+π)=(1.36±0.15±0.04)%B(D^{+}_{s}\rightarrow K^{+}K^{-}K^{0}_{S}\pi^{+}) / B(D^{+}_{s}\rightarrow K^{+}K^{0}_{S}\pi^{+}\pi^{-}) = (1.36\pm 0.15\pm 0.04)\%

    Search for the ηc2(1D)\eta_{c2}(1D) in e+eγηc2(1D)e^+e^-\to\gamma\eta_{c2}(1D) at s\sqrt{s} near 10.6 GeV at Belle

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    International audienceFor the first time we search for the ηc2(1D)\eta_{c2}(1D) in e+eγηc2(1D)e^+e^-\to\gamma\eta_{c2}(1D) at s\sqrt{s} = 10.52, 10.58, and 10.867 GeV with data samples of 89.5 fb1^{-1}, 711 fb1^{-1}, and 121.4 fb1^{-1}, respectively, accumulated with the Belle detector at the KEKB asymmetric energy electron-positron collider. No significant ηc2(1D)\eta_{c2}(1D) signal is observed in the mass range between 3.8 and 3.88 GeV/c2c^2. The upper limit at 90% confidence level on the product of the Born cross section for e+eγηc2(1D)e^+e^- \to \gamma\eta_{c2}(1D) and branching fraction for ηc2(1D)γhc(1P)\eta_{c2}(1D)\to \gamma h_c(1P) is determined to be σ(e+eγηc2(1D))B(ηc2(1D)γhc(1P))\sigma(e^+e^- \to \gamma\eta_{c2}(1D)){\cal B}(\eta_{c2}(1D)\to \gamma h_c(1P))<< 4.9 fb at s\sqrt{s} near 10.6 GeV

    Observation of charmed strange meson pair production in Υ(2S)\Upsilon(2S) decays and in e+ee^{+}e^{-} annihilation at s=10.52 GeV\sqrt{s} = 10.52~ \rm{GeV}

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    We observe the process Υ(2S)Ds()+DsJ\Upsilon(2S)\to D_s^{(*)+} D_{sJ}^{-} and continuum production e+eDs()+DsJe^+e^- \to D_s^{(*)+} D_{sJ}^- at s=10.52\sqrt{s} = 10.52 GeV (and their charge conjugates) using the data samples collected by the Belle detector at KEKB, where DsJD_{sJ}^- is Ds1(2536)D_{s1}(2536)^- or Ds2(2573)D^{*}_{s2}(2573)^-. Both DsJD_{sJ}^- states are identified through their decay into KˉDˉ()\bar{K}\bar{D}^{(*)}. We measure the products of branching fractions B(Υ(2S)Ds()+DsJ)B(DsJKˉDˉ()){\cal B}(\Upsilon(2S) \to D_{s}^{(*)+} D_{sJ}^-) {\cal B}(D_{sJ}^-\to \bar{K} \bar{D}^{(*)}) and the Born cross sections σBorn(e+eDs()+DsJ)B(DsJKˉDˉ())\sigma^{\rm Born}(e^+e^- \to D_{s}^{(*)+} D_{sJ}^-) {\cal B}(D_{sJ}^-\to \bar{K} \bar{D}^{(*)}), and then compare the ratios R1B(Υ(2S)Ds()+DsJ)/B(Υ(2S)μ+μ)R_1 \equiv {\cal B}(\Upsilon(2S)\to D_{s}^{(*)+} D_{sJ}^-)/{\cal B}(\Upsilon(2S)\to\mu^{+}\mu^-) for Υ(2S)\Upsilon(2S) decays and R2σBorn(e+eDs()+DsJ)/σBorn(e+eμ+μ)R_2 \equiv \sigma^{\rm Born}(e^+e^-\to D_{s}^{(*)+}D_{sJ}^-)/\sigma^{\rm Born}(e^+e^-\to \mu^{+}\mu^-) for continuum production. We obtain R1/R2=9.7±2.3±1.1R_1/R_2 = 9.7\pm 2.3 \pm 1.1, 6.8±2.1±0.86.8 \pm 2.1 \pm 0.8, 10.2±3.3±2.510.2 \pm 3.3 \pm 2.5, and 3.4±2.1±0.53.4 \pm 2.1 \pm 0.5 for the Ds+Ds1(2536)D_s^+ D_{s1}(2536)^-, Ds+Ds1(2536)D_s^{*+} D_{s1}(2536)^-, Ds+Ds2(2573)D_s^+ D_{s2}^{*}(2573)^{-}, and Ds+Ds2(2573)D_s^{*+} D_{s2}^{*}(2573)^{-} final states in the DsJKDˉ()0D_{sJ}^-\to K^{-} \bar{D}^{(*)0} modes, respectively. Therefore, the strong decay is expected to dominate in the Υ(2S)Ds()+DsJ\Upsilon(2S)\to D_{s}^{(*)+}D_{sJ}^- processes. We also measure the ratios of branching fractions B(Ds1(2536)KS0D(2010))/B(Ds1(2536)KD(2007)0)=0.48±0.07±0.02{\cal B}(D_{s1}(2536)^-\to K_S^0 D^{*}(2010)^{-})/{\cal B}(D_{s1}(2536)^-\to K^{-} D^{*}(2007)^0) = 0.48 \pm 0.07 \pm 0.02 and B(Ds2(2573)KS0D)/B(Ds2(2573)KD0)=0.49±0.10±0.02{\cal B}(D_{s2}^{*}(2573)^- \to K_S^0 D^-)/{\cal B}(D_{s2}^{*}(2573)^- \to K^{-}D^0) = 0.49 \pm 0.10 \pm 0.02, which are consistent with isospin symmetry. The second ratio is the first measurement of this quantity. Here, the first uncertainties are statistical and the second are systematic

    Search for a long-lived spin-0 mediator in b →s transitions at the Belle II experiment

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    Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles S in B-meson decays mediated by a b→s quark transition in e+e- collisions at the δ(4S) resonance at the Belle II experiment. Based on a sample corresponding to an integrated luminosity of 189 fb-1, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions B(B0→K∗(892)0(→K+π-)S)×B(S→x+x-) and B(B+→K+S)×B(S→x+x-), where x+x- indicates e+e-,μ+μ-,π+π-, or K+K-, as functions of S mass and lifetime at the level of 10-7

    Search for a long-lived spin-0 mediator in b→s transitions at the Belle II experiment

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    Additional spin-0 particles appear in many extensions of the standard model. We search for long-lived spin-0 particles S in B-meson decays mediated by a b→s quark transition in e+e− collisions at the Υ(4S) resonance at the Belle II experiment. Based on a sample corresponding to an integrated luminosity of 189 fb−1, we observe no evidence for signal. We set model-independent upper limits on the product of branching fractions B(B0→K∗(892)0(→K+π−)S)×B(S→x+x−) and B(B+→K+S)×B(S→x+x−), where x+x− indicates e+e−,μ+μ−,π+π−, or K+K−, as functions of S mass and lifetime at the level of 10−7

    Measurement of the time-integrated CP asymmetry in D0KS0KS0D^{0}\rightarrow K^{0}_{S}K^{0}_{S} decays using Belle and Belle II data

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    We measure the time-integrated CP asymmetry in D0KS0KS0D^{0} \rightarrow K^{0}_{S}K^{0}_{S} decays reconstructed in e+ecce^{+}e^{-} \rightarrow c\overline{c} events collected by the Belle and Belle II experiments. The corresponding data samples have integrated luminosities of 980 fb1^{-1} and 428 fb1^{-1}, respectively. The D0D^{0} decays are required to originate from the D+D0π+D^{*+} \rightarrow D^{0}\pi^{+} decay, which determines the charm flavor at production time. A control sample of D0K+KD^{0} \rightarrow K^{+}K^{-} decays is used to correct for production and detection asymmetries. The result, (1.4±1.3(stat)±0.1(syst))%(-1.4\pm1.3{\rm(stat)}\pm0.1{\rm (syst)})\%, is consistent with previous determinations and with CP symmetry
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