Primary authors:Olga Norniella, Benjamin Carls, Kevin Pitts
Introduction
We report the first observation of Bs &rarr J/&psi K* and Bs &rarr J/&psi KS decays in a sample corresponding to 5.9 fb-1 collected by a dedicated low pT di-muon trigger. A cut based optimization was carried out for the Bs &rarr J/&psi K* analysis, while a neural network was used for the observation of Bs &rarr J/&psi KS. In addition to the observation of the new decay modes, their decay rates were measured using B0 decays in the same final states as a reference. From the measured quantities fsBR(Bs &rarr J/&psi K*)/fdBR(B0 &rarr J/&psi K*) and fsBR(Bs &rarr J/&psi KS)/fdBR(B0 &rarr J/&psi KS), absolute branching fractions were determined using known values of fs/fd and the branching fractions of the reference B0 decays as inputs.
The analysis is described in detail in Public Note 10240.
Motivation
While the phenomenology of B+ and B0 decays has been extensively studied at the B factory experiments, much less is known about Bs decays. This analysis is part of a broader CDF program aimed at a systematic exploration of the physics of Bs mesons. Bs &rarr J/&psi KS is a CP eigenstate and has never been observed. Measurement of its lifetime directly probes &tauBs(heavy). Additionally, large samples of Bs &rarr J/&psi KS can be used to extract the angle &gamma of the unitary triangle (R. Fleischer, Eur. Phys. J. C10:299-306,1999). Bs &rarr J/&psi K* is yet another unobserved mode which contains an admixture of CP final states. An angular analysis of a significantly large enough sample of Bs &rarr J/&psi K* can be carried out to extract sin(2 &betas) as a compliment to Bs &rarr J/&psi &Phi.
Procedure
The analysis initially sought out the reconstruction of B0 &rarr J/&psi K* and B0 &rarr J/&psi KS from a sample of di-muons with pT > 1.5 GeV/c (J/&psi &rarr &mu+&mu&minus ). Using the reconstructed B0 &rarr J/&psi K* and B0 &rarr J/&psi KS samples, a series of cuts were applied to optimize selection of Bs &rarr J/&psi K* and Bs &rarr J/&psi KS. After signal optimization, a binned likelihood fit was applied to the J/&psi KS or J/&psi K &pi mass distributions to extract the ratio of candidates of Bs &rarr J/&psi K*(S) to B0 &rarr J/&psi K*(S). In both channels, the Bs and B0 were modeled by three gaussian templates constructed from MC samples. Combinatorial backgrounds were modeled using an exponential. Partially reconstructed B decays were modeled by ARGUS functions convoluted with a gaussian. In the Bs &rarr J/&psi K* sample, a two gaussian template, normalized from a separate measurement of Bs &rarr J/&psi &Phi, was applied to account for Bs &rarr J/&psi &Phi contributions. After application of a relative acceptance factor determined from simulation, the quantity fsBR(Bs &rarr J/&psi K*(S))/fdBR(B0 &rarr J/&psi K*(S)) was measured.
Systematic uncertainties are classified as either fit-related uncertainties or uncertainties on the relative acceptance. Fit uncertainties included combinatorial background modeling and modeling of the Bs and B0 signals. For the required relative acceptances, there were uncertainties in the modeling of the B hadron transverse momentum spectrum, B hadron lifetime, and polarization for Bs &rarr J/&psi K*.
Significance
In comparing the signal hypotheses to the null hypothesis, we obtain a
p-value for Bs &rarr J/&psi K* of 8.9
× 10&minus 16 or 8 σ. Alternatively, for
Bs &rarr J/&psi KS, we determined a
p-value of 3.9 × 10&minus 13 or 7.2 σ.
Results
For Bs &rarr J/&psi K* we measure:
- B0 &rarr J/&psi K* yield: 9530 ± 110, Bs &rarr J/&psi K* yield: 151 ± 25
- fsBR(Bs &rarr J/&psi K*)/fdBR(B0 &rarr J/&psi K*) = 0.0168 ± 0.0024 (stat.) ± 0.0068 (syst.)
After application of the CDF value of fs/fd =
0.269 ± 0.033 (determined from Phys. Rev. D77, 072003 (2008) and the new PDG value for BR(Ds &rarr &Phi &pi)), the ratio of branching ratios is determined to be:
- BR(Bs &rarr J/&psi K*)/BR(B0 &rarr J/&psi K*) = 0.062 ± 0.009 (stat.) ± 0.025 (syst.) ± 0.008 (frag.)
Using the PDG value of BR(B0 &rarr J/&psi K*) = (1.33 ± 0.06) × 10&minus 3, we arrive at the absolute branching ratio:
- BR(Bs &rarr J/&psi K*) = (8.3 ± 1.2 (stat.) ± 3.3 (syst.) ± 1.0 (frag.) ± 0.4(PDG)) × 10 &minus 5
Alternatively, for Bs &rarr J/&psi KS we measure:
- B0 &rarr J/&psi KS yield: 5954 ± 79, Bs &rarr J/&psi KS yield: 64 ± 14
- fsBR(Bs &rarr J/&psi KS)/fdBR(B0 &rarr J/&psi KS) = 0.0109 ± 0.0019 (stat.) ± 0.0011 (syst.)
After application of the CDF value of fs/fd = 0.269 ± 0.033, the ratio of branching ratios is determined to be:
- BR(Bs &rarr J/&psi KS)/BR(B0 &rarr J/&psi KS) = 0.0405 ± 0.0070 (stat.) ± 0.0041 (syst.) ± 0.0050 (frag.)
Using the PDG value of BR(B0 &rarr J/&psi KS) = (8.71 ± 0.32) × 10&minus 3, we arrive at the absolute branching ratio:
- BR(Bs &rarr J/&psi K0) = (3.53 ± 0.61 (stat.) ± 0.35 (syst.) ± 0.43 (frag.) ± 0.13 (PDG)) × 10 &minus 5
Figures
The figures crucial to the analyses appear below:
- Figure 1: Bs &rarr J/&psi K* mass distribution, fit, and residuals (.ps) (.gif)
- Figure 2: Log likelihood scan of N(Bs &rarr J/&psi K*)/N(B0 &rarr J/&psi K*) (.ps) (.gif)
- Figure 3: Sideband subtracted B proper decay length of Bs &rarr J/&psi K* signal region (.ps) (.gif)
- Figure 4: Optimization of efficiency/(1.5 + &radic B) as a function of K pT for Bs &rarr J/&psi K* (.ps) (.gif)
- Figure 5: Optimization of efficiency/(1.5 + &radic B) as a function of &pi pT for Bs &rarr J/&psi K* (.ps) (.gif)
- Figure 6: Optimization of efficiency/(1.5 + &radic B) as a function of B Lxy for Bs &rarr J/&psi K* (.ps) (.gif)
- Figure 7: Optimization of efficiency/(1.5 + &radic B) as a function of Prob(B) for Bs &rarr J/&psi K* (.ps) (.gif)
- Figure 8: Mass distribution and fit with layered contributions for Bs &rarr J/&psi K* (.ps) (.gif)
- Figure 9: Zoomed in Mass distribution and fit with layered contributions for Bs &rarr J/&psi K* (.ps) (.gif)
- Figure 10: Bs &rarr J/&psi KS mass distribution, fit, and residuals (.ps) (.gif)
- Figure 11: Log likelihood scan of N(Bs &rarr J/&psi KS)/N(B0 &rarr J/&psi KS) (.ps) (.gif)
- Figure 12: KS mass distribution for Bs &rarr J/&psi KS (.ps) (.gif)
- Figure 13: The J/&psi KS invariant mass distribution without the neural network cut (.ps) (.gif)
- Figure 14: The J/&psi KS invariant mass distribution with the neural network cut (.ps) (.gif)
- Figure 15: The J/&psi KS invariant mass distribution with different neural network cuts (.ps) (.gif)
- Figure 16: The optimization of efficiency/(1.5 + &radic B) for Bs &rarr J/&psi KS (.ps) (.gif)
- Figure 17: The Bs &rarr J/&psi KS signal and background regions for the neural network (.ps) (.gif)
- Figure 18: Neural network response for Bs &rarr J/&psi KS (.ps) (.gif)
- Figure 19: Mass distribution and fit with layered contributions for Bs &rarr J/&psi KS (.ps) (.gif)
- Figure 20: Zoomed in Mass distribution and fit with layered contributions for Bs &rarr J/&psi KS (.ps) (.gif)