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Measurement of CPCP asymmetries and polarisation fractions in Bs0K0Kˉ0B_s^0 \rightarrow K^{*0}\bar{K}{}^{*0} decays

Abstract

An angular analysis of the decay Bs0K0Kˉ0B_s^0 \rightarrow K^{*0}\bar{K}{}^{*0} is performed using pppp collisions corresponding to an integrated luminosity of 1.01.0 fb1{fb}^{-1} collected by the LHCb experiment at a centre-of-mass energy s=7\sqrt{s} = 7 TeV. A combined angular and mass analysis separates six helicity amplitudes and allows the measurement of the longitudinal polarisation fraction fL=0.201±0.057(stat.)±0.040(syst.)f_L = 0.201 \pm 0.057 {(stat.)} \pm 0.040{(syst.)} for the Bs0K(892)0Kˉ(892)0B_s^0 \rightarrow K^*(892)^0 \bar{K}{}^*(892)^0 decay. A large scalar contribution from the K0(1430)K^{*}_{0}(1430) and K0(800)K^{*}_{0}(800) resonances is found, allowing the determination of additional CPCP asymmetries. Triple product and direct CPCP asymmetries are determined to be compatible with the Standard Model expectations. The branching fraction B(Bs0K(892)0Kˉ(892)0)\mathcal{B}(B_s^0 \rightarrow K^*(892)^0 \bar{K}{}^*(892)^0) is measured to be (10.8±2.1 (stat.)±1.4 (syst.)±0.6 (fd/fs))×106(10.8 \pm 2.1 {\ \rm (stat.)} \pm 1.4 {\ \rm (syst.)} \pm 0.6 \ (f_d/f_s) ) \times 10^{-6}

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    Last time updated on 10/05/2016