Direct CP violation in ΛbΛ_b decays

preprint2014arXivOpen access

Abstract

We study direct CP violating asymmetries (CPAs) in the two-body ΛbΛ_b decays of Λb→pM(V)Λ_b\to pM(V) with M(V)=K−(K∗−)M(V)=K^-(K^{*-}) and π−(ρ−)π^-(ρ^-) based on the generalized factorization method. After simultaneously explaining the observed decay branching ratios of Λb→(pK− ,  pπ−)Λ_b\to (p K^-\,,\; p π^-) with RπK≡B(Λb→pπ−)/B(Λb→pK−){\cal R}_{πK}\equiv {\cal B}(Λ_b\to p π^-)/{\cal B}(Λ_b\to p K^-) being 0.84±0.090.84\pm 0.09, we find that their corresponding direct CPAs are (5.8±0.2, −3.9±0.2)%(5.8\pm 0.2,\,-3.9\pm 0.2)\% in the standard model (SM), in comparison with (−5− 5+26, −31− 1+43)%(-5^{+26}_{-~5},\, -31^{+43}_{-~1})\% and (−10±8±4, 6±7±3)%(-10\pm8\pm4,\, 6\pm7\pm3)\% from the perturbative QCD calculation and the CDF experiment, respectively. For Λb→(pK∗−, pρ−)Λ_b\to ( p K^{*-},\, pρ^-), the decay branching ratios and CPVs in the SM are predicted to be (2.5±0.5, 11.4±2.1)×10−6(2.5\pm0.5,\,11.4\pm2.1)\times 10^{-6} with RρK∗=4.6±0.5{\cal R}_{ρK^*}=4.6\pm0.5 and (19.6±1.6, −3.7±0.3)%(19.6\pm1.6,\, -3.7\pm0.3)\%, respectively. The uncertainties for the CPAs in these decay modes as well as RπK, ρK∗−{\cal R}_{πK,\,ρK^{*-}} mainly arise from the quark mixing elements and non-factorizable effects, whereas those from the hadronic matrix elements are either totally eliminated or small. We point out that the large CPA for Λb→pK∗−Λ_b\to p K^{*-} is promising to be measured by the CDF and LHCb experiments, which is a clean test of the SM.

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