1,373 research outputs found

    Recent Results in Bottomonium

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    Great strides have been made in the understanding of bound states of the bottom quark, b, and its antiquark, (b) over bar, since the discovery of the first Upsilon resonances in 1977. These bound states, known as bottomonium, have a rich spectrum whose masses and transition amplitudes shed valuable light on the strong interactions. We review some recent developments in bottomonium physics, including the discovery of the spin-singlet states eta(b) (1S, 2S) and h(b) (1P, 2P), the first D-wave states, one or more candidates for spin-triplet.XbJ(3P) excitations, and above-threshold states with strong transitions to states below threshold. We also present information about transitions, production, and signatures of new physics

    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)\%

    Measurement of the branching fractions for Cabibbo-suppressed decays D+→K+K−π+π0 and D(s)+→K+π−π+π0 at Belle

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    We present measurements of the branching fractions for the singly Cabibbo-suppressed decays D+→K+K−π+π0 and D+s→K+π−π+π0, and the doubly Cabibbo-suppressed decay D+→K+π−π+π0, based on 980 fb−1 of data recorded by the Belle experiment at the KEKB e+e− collider. We measure these modes relative to the Cabibbo-favored modes D+→K−π+π+π0 and D+s→K+K−π+π0. Our results for the ratios of branching fractions are B(D+→K+K−π+π0)/B(D+→K−π+π+π0)=(11.32±0.13±0.26)%, B(D+→K+π−π+π0)/B(D+→K−π+π+π0)=(1.68±0.11±0.03)%, and B(D+s→K+π−π+π0)/B(D+s→K+K−π+π0)=(17.13±0.62±0.51)%, where the uncertainties are statistical and systematic, respectively. The second value corresponds to (5.83±0.42)×tan4θC, where θC is the Cabibbo angle; this value is larger than other measured ratios of branching fractions for a doubly Cabibbo-suppressed charm decay to a Cabibbo-favored decay. Multiplying these results by world average values for B(D+→K−π+π+π0) and B(D+s→K+K−π+π0) yields B(D+→K+K−π+π0)=(7.08±0.08±0.16±0.20)×10^−3, B(D+→K+π−π+π0)=(1.05±0.07±0.02±0.03)×10^−3, and B(D+s→K+π−π+π0)=(9.44±0.34±0.28±0.32)×10^−3, where the third uncertainty is due to the branching fraction of the normalization mode. The first two results are consistent with, but more precise than, the current world averages. The last result is the first measurement of this branching fraction

    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

    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 branching fraction and search for CP violation in D0KS0KS0π+πD^0\rightarrow K^0_S\,K^0_S\,\pi^+\pi^- decays at Belle

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    9 pages, 4 figures, to be submitted to Phys. Rev. DInternational audienceWe measure the branching fraction for the Cabibbo-suppressed decay D0KS0KS0π+πD^0\rightarrow K^0_S\,K^0_S\,\pi^+\pi^- and search for CPCP violation via a measurement of the CPCP asymmetry ACPA_{\rm CP} as well as the TT-odd triple-product asymmetry aCPTa^T_{\rm CP}. We use 922 fb1^{-1} of data recorded by the Belle experiment, which ran at the KEKB asymmetric-energy e+ee^+e^- collider. The branching fraction is measured relative to the Cabibbo-favored normalization channel D0KS0π+πD^0\rightarrow K^0_S\,\pi^+\pi^-; the result is B(D0KS0KS0π+π)=[4.82±0.08(stat)0.11+0.10(syst)±0.31(norm)]×104\mathcal{B}(D^0\rightarrow K^0_S\,K^0_S\,\pi^+\pi^-) = [4.82 \pm 0.08\,({\rm stat})\,^{+0.10}_{-0.11}\,({\rm syst}) \pm 0.31\,({\rm norm})]\times 10^{-4}, where the first uncertainty is statistical, the second is systematic, and the third is from uncertainty in the normalization channel. We also measure ACP=[2.51±1.44(stat)0.52+0.35(syst)]%A_{\rm CP} = [-2.51\,\pm 1.44\,({\rm stat})\,^{+0.35}_{-0.52}\,({\rm syst})]\%, and aCPT=[1.95±1.42(stat)0.12+0.14(syst)]%a^T_{\rm CP} = [-1.95\,\pm 1.42\,({\rm stat})\,^{+0.14}_{-0.12}\,({\rm syst})]\%. These results show no evidence of CP violation

    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

    Search for CPCP Violation and Measurement of the Branching Fraction in the Decay D0KS0KS0D^{0} \to K^0_S K^0_S

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    We report a study of the decay D0KS0KS0D^0 \to K^0_S K^0_S using 921~fb1^{-1} of data collected at or near the Υ(4S)\Upsilon(4S) and Υ(5S)\Upsilon(5S) resonances with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. The measured time-integrated CP asymmetry is ACP(D0KS0KS0)=(0.02±1.53±0.02±0.17)% A_{CP}(D^0 \to K^0_S K^0_S) = (-0.02 \pm 1.53 \pm 0.02 \pm 0.17) \% and the branching fraction is B(D0KS0KS0)\mathcal{B} (D^{0}\rightarrow K_{S}^{0}K_{S}^{0}) = (1.32 ±\pm 0.02 ±\pm 0.04 ±\pm 0.04) ×\times 104^{-4}, where the first uncertainty is statistical, the second is systematic, and the third is due to the normalization mode (D0KS0π0D^0 \to K_S^0 \pi^0) used in the analysis. These results are significantly more precise than previous measurements for this mode. The ACPA_{CP} measurement is consistent with the Standard Model expectation
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