Search For New Physics at BABAR

preprint2013arXivOpen access

Abstract

Using a full BABAR data sample of 426 fb−1fb^{-1}, we present improved measurements of the ratio R(D(∗))=B(Bˉ→D(∗)τ−νˉτ)/{\cal{R}}(D^{(*)}) = {\cal{B}} (\bar{B} \to D^{(*)}τ^{-}\barν_τ)/ B(Bˉ→D(∗)ℓℓ−νˉℓ){\cal{B}} (\bar{B} \to D^{(*)}\ell_{\ell}^{-}\barν_{\ell}), where ℓ\ell is either electron or muon. We measure R(D)=0.440±0.058±0.042{\cal{R}}(D) = 0.440 \pm 0.058 \pm 0.042 and R(D∗)=0.332±0.024±0.018{\cal{R}}(D^*) = 0.332 \pm 0.024 \pm 0.018. These ratios exceed the Standard Model predictions by 2.0σ2.0σ and 2.7σ2.7σ, respectively. The results disagree with the Standard Model predictions at the level of 3.4σ3.4σ. The ratios are sensitive to new physics contributions in the form of a charged Higgs boson. However, the access cannot be explained by a charged Higgs boson in the type II two-Higgs-doublet model.

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