927 research outputs found

    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)\%

    Angular analysis of the low K+K− invariant mass enhancement in B+→K+K−π+ decays

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    We study the decay B+→K+K−π+ and investigate the angular distribution of K+K− pairs with invariant mass below 1.1 GeV/c2. This region exhibits both a strong enhancement in signal and very large direct CP violation. We construct a coherent sum model for the angular distribution of S- and P-wave, and report the ratio of their amplitudes, the relative phase and the forward-backward asymmetry. We also report absolute differential branching fractions and direct CP asymmetry for the decay in bins of MK+K− and the differential branching fractions in bins of MK+π−. The results are based on a data sample that contains 772×10^6 BB ̄ pairs collected at the Υ(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e− collider. The measured overall branching fraction and the direct CP asymmetry are (5.38±0.40±0.35)×10^−6 and −0.170±0.073±0.017, respectively, where the first uncertainties are statistical and the second are systematic

    Angular analysis of the low K+ K- invariant mass enhancement in B+ →K+ K- π+ decays

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    We study the decay B+→K+K-π+ and investigate the angular distribution of K+K- pairs with invariant mass below 1.1 GeV/c2. This region exhibits both a strong enhancement in signal and very large direct CP violation. We construct a coherent sum model for the angular distribution of the S- and P-wave, and report the ratio of their amplitudes, the relative phase and the forward-backward asymmetry. We also report absolute differential branching fractions and direct CP asymmetry for the decay in bins of MK+K- and the differential branching fractions in bins of MK+π-. The results are based on a data sample that contains 772×106 BB ̄ pairs collected at the Υ(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+e- collider. The result favors the presence of S- and D-waves in low MK+K- region to the detriment of a P-wave

    Observation of B+pΛˉK+KB^{+} \rightarrow p\bar{\Lambda} K^+ K^- and B+pˉΛK+K+B^{+} \rightarrow \bar{p}\Lambda K^+ K^+

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    International audienceWe report the study of B+→pΛ¯K+K- and B+→p¯ΛK+K+ decays using a 772×106  BB¯ pair data sample recorded on the ϒ(4S) resonance with the Belle detector at KEKB. The following branching fractions are measured: B(B+→pΛ¯K+K-)=(4.10-0.43+0.45±0.50)×10-6, B(B+→p¯ΛK+K+)=(3.70-0.37+0.39±0.44)×10-6, B(ηc→pΛ¯K-+c.c.)=(2.83-0.34+0.36±0.35)×10-3 and B(B+→pΛ¯ϕ)=( 7.95±2.09±0.77)×10-7, where c.c. denotes the corresponding charge-conjugation process. The intermediate resonance decays are excluded in the four-body decay measurements. We also find evidence for B(ηc→Λ(1520)Λ¯+c.c.)=(3.48±1.48±0.46)×10-3 and B(B+→Λ(1520)Λ¯K+)=( 2.23±0.63±0.25)×10-6. No significant signals are found for J/ψ→Λ(1520)Λ¯+c.c. and B+→Λ¯(1520)ΛK+; we set the 90% confidence level upper limits on their decay branching fractions as <1.80×10-3 and <2.08×10-6, respectively

    Experimental constraints on the spin and parity of the Z(4430)+Z(4430)^{+}

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    We perform a full amplitude analysis of anti-B0 -> psi' K- pi+ decays, with psi' -> mu+ mu- or e+ e-, to constrain the spin and parity of the Z(4430)+. The J^P = 1+ hypothesis is favored over the 0- hypothesis at the 2.9 sigma level, while all other hypotheses with J <= 2 are excluded at the level of at least 4.3 sigma. The analysis is based on a 711 fb^-1 data sample that contains 772x10^6 B B pairs, collected at the Y(4S) resonance by the Belle detector at the asymmetric-energy e+ e- collider KEKB

    First observation of γγppˉK+K\gamma \gamma \to p \bar{p} K^+ K^- and search for exotic baryons in pKpK systems

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    The process γγ→pp¯K+K- and its intermediate processes are measured for the first time using a 980 fb-1 data sample collected with the Belle detector at the KEKB asymmetric-energy e+e- collider. The production of pp¯K+K- and a Λ(1520)0 (Λ¯(1520)0) signal in the pK- (p¯K+) invariant mass spectrum are clearly observed. However, no evidence for an exotic baryon near 1540 MeV/c2, denoted as Θ(1540)0 (Θ¯(1540)0) or Θ(1540)++ (Θ(1540)--), is seen in the pK- (p¯K+) or pK+ (p¯K-) invariant mass spectra. Cross sections for γγ→pp¯K+K-, Λ(1520)0p¯K++c.c. and the products σ(γγ→Θ(1540)0p¯K++c.c.)B(Θ(1540)0→pK-) and σ(γγ→Θ(1540)++p¯K-+c.c.)B(Θ(1540)++→pK+) are measured. We also determine upper limits on the products of the χc0 and χc2 two-photon decay widths and their branching fractions to pp¯K+K- at the 90% credibility level

    Measurement of CPCP asymmetries in B0KS0KS0KS0B^0 \rightarrow K^0_S K^0_S K^0_S decays at Belle II

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    We report a measurement of decay-time dependent charge-parity (CPCP) asymmetries in B0KS0KS0KS0B^0 \rightarrow K^0_S K^0_S K^0_S decays. We use 387×106BBˉ387 \times 10^6 B\bar{B} pairs collected at the Υ(4S)\Upsilon(4S) resonance with the Belle II detector at the SuperKEKB asymmetric-energy electron-positron collider. We reconstruct 220 signal events and extract the CPCP-violating parameters SS and CC from a fit to the distribution of the decay-time difference between the two BB mesons. The resulting confidence region is consistent with previous measurements in B0KS0KS0KS0B^0 \rightarrow K^0_S K^0_S K^0_S and B0(ccˉ)K0B^0 \rightarrow (c\bar{c})K^0 decays, and with predictions based on the standard model

    Measurement of branching fraction and direct CPCP asymmetry in charmless B+K+Kπ+B^+ \to K^+K^- \pi^+ decays at Belle

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    We report a study of the charmless hadronic decay of the charged BB meson to the three-body final state K+Kπ+K^+ K^- \pi^+. The results are based on a data sample that contains 772×106772\times10^6 BBˉB \bar{B} pairs collected at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+ e^- collider. The measured inclusive branching fraction and the direct CPCP asymmetry are (5.38±0.40±0.35)×106(5.38\pm0.40\pm0.35)\times 10^{-6} and 0.182±0.071±0.016-0.182\pm0.071\pm0.016, respectively, where the first uncertainties are statistical and the second are systematic. The K+KK^{+}K^{-} invariant mass distribution of the signal candidates shows an excess in the region below 1.51.5 GeV/c2c^2, which is consistent with the previous studies from BaBar and LHCb. In addition, strong evidence of a large direct CPCP asymmetry is found in the K+KK^{+}K^{-} low-invariant-mass region

    Measurement of the Resonant and Non-Resonant Branching Ratios in Ξc0Ξ0K+K\Xi_{c}^{0} \rightarrow \Xi^{0} K^+ K^-

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    Using the entire data sample of 980980 fb1fb^{-1} integrated luminosity collected with the Belle detector at the KEKB asymmetric-energy e+ee^{+}e^{-} collider, we present an amplitude analysis measuring the branching fractions of the Cabibbo-allowed, WW-exchange resonant decay Ξc0Ξ0ϕ(K+K)\Xi_{c}^{0} \rightarrow \Xi^{0} \phi (\to K^+ K^-) with a polarized ϕ\phi and the non-resonant decay via a direct process Ξc0Ξ0K+K\Xi_{c}^{0} \rightarrow \Xi^{0} K^+ K^-. We present these measurements, relative to the normalization mode Ξπ+\Xi^{-}\pi^{+}, and find branching ratios B(Ξc0Ξ0ϕ(K+K))B(Ξc0Ξπ+)=0.036±0.004(stat.)±0.002(syst.)\frac{\mathcal{B}(\Xi_{c}^{0} \rightarrow \Xi^{0} \phi (\rightarrow K^{+}K^{-}))}{\mathcal{B}(\Xi_{c}^{0} \rightarrow \Xi^{-} \pi^{+})} = 0.036 \pm 0.004 (stat.) \pm 0.002 (syst.) and B(Ξc0Ξ0K+K)B(Ξc0Ξπ+)=0.039±0.004(stat.)±0.002(syst.)\frac{\mathcal{B}(\Xi_{c}^{0} \rightarrow \Xi^{0} K^{+} K^{-})}{\mathcal{B}(\Xi_{c}^{0} \rightarrow \Xi^{-} \pi^{+})} = 0.039 \pm 0.004 (stat.) \pm 0.002 (syst.) which suggest that only minor cusping peaks occur in the combinatorial background of ΩΞ0K\Omega^{*-} \to \Xi^{0}K^{-} due to these Ξc0\Xi_{c}^{0} decays
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