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تسجيل مستخدم جديدMeasurements of sin2phi_1 in B0 -> eta K0, omega KS and pi0 K0 decays
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T.Aushev
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In this report we summarize the most recent sin2phi_1 measurements in the b -> q anti-q s decays.
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We present a precise measurement of the CP violation parameter sin2phi_1 and the direct CP violation parameter A_f using the final data sample of 772x10^6 Bbar B pairs collected at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmet
ric-energy e+e- collider. One neutral B meson is reconstructed in a J/psi K0S, psi(2S) K0S, chi_c1 K0S or J/psi K0L CP-eigenstate and its flavor is identified from the decay products of the accompanying B meson. From the distribution of proper time intervals between the two B decays, we obtain the following CP violation parameters: sin2phi_1=0.667+-0.023(stat)+-0.012(syst) and A_f=0.006+-0.016(stat)+-0.012(syst).
We present results on time-dependent CP asymmetries in neutral B decays to several CP eigenstates. The measurements use a data sample of about 227 million Upsilon(4S) -> BBbar decays collected by the BABAR detector at the PEP-II asymmetric-energy B F
actory at SLAC. The amplitude of the CP asymmetry, sin2Beta in the Standard Model, is derived from decay-time distributions from events in which one neutral B meson is fully reconstructed in a final state containing a charmonium meson and the other $B$ meson is determined to be either a B0 or B0bar from its decay products. We measure sin2Beta = 0.722 +/- 0.040 (stat.) +/- 0.23 (syst.) in agreement with the Standard Model expectation.
We present for the first time a measurement of the weak phase 2b+g obtained from a time-dependent Dalitz plot analysis of B^0 -> D-(+) K0 Pi+(-) decays. Using a sample of approximately 347*10^{6} BBbar pairs collected by the BABAR detector at the PEP
-II asymmetric-energy storage rings, we obtain 2b+g = (83 +/- 53 +/- 20) degrees and (263 +/- 53 +/- 20) degrees assuming the ratio r of the b -> u and b -> c decay amplitudes to be 0.3. The magnitudes and phases for the resonances associated with the b -> c transitions are also extracted from the fit.
The rare decay K0(L) --> pi0 pi0 nu nu-bar was studied with the E391a detector at the KEK 12-GeV proton synchrotron. Based on 9.4 x 10^9 K0L decays, an upper limit of 8.1 x 10^{-7} was obtained for the branching fraction at 90% confidence level. We a
lso set a limit on the K0(L) --> pi0 pi0 X (X --> invisible particles) process; the limit on the branching fraction varied from 7.0 x 10^{-7} to 4.0 x 10^{-5} for the mass of X ranging from 50 MeV/c^2 to 200 MeV/c^2.
We study the charmless decays B to Lambda Lambdabar h, where h stands for pi^+, K^+,K^0,K^{*+}, or K^{*0}, using a 605 fb^{-1} data sample collected at the Upsilon(4S)resonance with the Belle detector at the KEKB asymmetric energy e^+ e^- collider. W
e observe B0 to Lambda Lambdabar K0 and B0 to Lambda Lambdabar K*0 with branching fractions of (4.76^{+0.84}_{-0.68} (stat.) pm 0.61 (syst.)) times 10^{-6} and (2.46^{+0.87}_{-0.72} pm 0.34) times 10^{-6}, respectively. The significances of these signals in the threshold-mass enhanced mass region are 12.4 sigma and 9.3 sigma, respectively. We also update the branching fraction BF(B+ to Lambda Lambdabar K+) = (3.38^{+0.41}_{-0.36} pm 0.41)times 10^{-6} with better accuracy,and report the following measurement or 90% confidence level upper limit in the threshold-mass-enhanced region: BF(B+ to Lambda Lambdabar K*+) = (2.19^{+1.13}_{-0.89} pm 0.33) times 10^{-6} with 3.7 sigma significance; BF(B+ to Lambda Lambdabar pi+) < 0.94 times 10^{-6}. A related search for B0 to Lambda Lambdabar D0bar yields a branching fraction BF(B0 to Lambda Lambdabar D0bar) = (1.05_{-0.44}^{+0.57} pm 0.13)times 10^{-5}. This may be compared with the large, ~10^{-4}, branching fraction observed for B0 to p pbar D0bar. The m_{Lambda Lambdabar} enhancements near threshold and related angular distributions for the observed modes are also reported. PACS:13.25.Hw, 14.40.Nd
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