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arXiv 0902.2660hep-ex
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半轻子衰变B --> D τ- nubar_tau和B --> D* τ- nubar_tau的测量

Measurement of the Semileptonic Decays B --> D tau- nubar_tau and B --> D* tau- nubar_tau

The BABAR Collaboration, B. Aubert

摘要:

我们给出了半轻子衰变B-> D 0 τ- nubar_tau,B-> D*0 τ- nubar_tau,B 0 bar--> D+ τ- nubar_tau和B 0 bar--> D*+ τ- nubar_tau的测量结果,这些衰变在某些情况下对非标准模型振幅敏感。数据样本由PEP-II e+e对撞机上BaBar探测器收集的232 × 10^6 Upplane(4S)-> BBbar衰变组成。我们选择事件与D或D* 介子和轻轻子(ell=e或mu)反冲对一个完全重建的B介子。我们对轻子动量和丢失质量平方的联合分布进行拟合,以区分信号B --> D(*)tau- nubar_tau(tau-> ell-nubar_ellnu_tau)事件和背景,主要是B --> D(*)ell-nubar_ell。我们测量了分支分数比R(D)= BR(B --> D tau- nubar_tau)/ BR(B --> D ell- nubar_ell)和R(D*)== BR(B --> D* tau- nubar_tau)/ BR(B --> D* ell- nubar_ell),并且,根据对B-和B 0 bar通道的组合拟合,获得结果R(D)=(41.6 +/- 11.7 +/- 5.2)%和R(D*)=(29.7 +/- 5.6 +/- 1.8)%,其中不确定度为统计和系统不确定度。归一化到测量的B-> D(*)0 ell-nubar_ell支化分数,我们得到BR(B --> D τ- nubar_τ)=(0.86 +/- 0.24 +/- 0.11 +/- 0.06)%和BR(B --> D* tau- nubar_tau)=(1.62 +/- 0.31 +/- 0.10 +/- 0.05)%,其中附加的第三不确定度来自归一化模式。我们还首次给出了轻子动量p*_ell和平方动量转移q ^2的分布。

英文摘要:

We present measurements of the semileptonic decays B- --> D0 tau- nubar_tau, B- --> D*0 tau- nubar_tau, B0bar --> D+ tau- nubar_tau, and B0bar --> D*+ tau- nubar_tau, which are sensitive to non--Standard Model amplitudes in certain scenarios. The data sample consists of 232x10^6 Upsilon(4S) --> BBbar decays collected with the BaBar detector at the PEP-II e+e- collider. We select events with a D or D* meson and a light lepton (ell=e or mu) recoiling against a fully reconstructed B meson. We perform a fit to the joint distribution of lepton momentum and missing mass squared to distinguish signal B --> D(*) tau- nubar_tau (tau- --> ell- nubar_ell nu_tau) events from the backgrounds, predominantly B --> D(*) ell- nubar_ell. We measure the branching-fraction ratios R(D) == BR(B --> D tau- nubar_tau) / BR(B --> D ell- nubar_ell) and R(D*) == BR(B --> D* tau- nubar_tau) / BR(B --> D* ell- nubar_ell) and, from a combined fit to B- and B0bar channels, obtain the results R(D)=(41.6 +/- 11.7 +/- 5.2)% and R(D*)=(29.7 +/- 5.6 +/- 1.8)%, where the uncertainties are statistical and systematic. Normalizing to measured B- --> D(*)0 ell- nubar_ell branching fractions, we obtain BR(B --> D tau- nubar_tau)=(0.86 +/- 0.24 +/- 0.11 +/- 0.06)% and BR(B --> D* tau- nubar_tau)=(1.62 +/- 0.31 +/- 0.10 +/- 0.05)%, where the additional third uncertainty is from the normalization mode. We also present, for the first time, distributions of the lepton momentum, p*_ell, and the squared momentum transfer, q^2.

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