Abstract / Description of output
First observations of the B0s→ψ(2S)η, B0→ψ(2S)π+π− and B0s→ψ(2S)π+π− decays are made using a dataset corresponding to an integrated luminosity of 1.0fb−1 collected by the LHCb experiment in proton–proton collisions at a centre-of-mass energy of s√=7TeV. The ratios of the branching fractions of each of the ψ(2S) modes with respect to the corresponding J/ψ decays are
B(B0s→ψ(2S)η)B(B0s→J/ψη)=0.83±0.14(stat)±0.12(syst)±0.02(B),
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B(B0→ψ(2S)π+π−)B(B0→J/ψπ+π−)=0.56±0.07(stat)±0.05(syst)±0.01(B),
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B(B0s→ψ(2S)π+π−)B(B0s→J/ψπ+π−)=0.34±0.04(stat)±0.03(syst)±0.01(B),
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where the third uncertainty corresponds to the uncertainties of the dilepton branching fractions of the J/ψ and ψ(2S) meson decays.
B(B0s→ψ(2S)η)B(B0s→J/ψη)=0.83±0.14(stat)±0.12(syst)±0.02(B),
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B(B0→ψ(2S)π+π−)B(B0→J/ψπ+π−)=0.56±0.07(stat)±0.05(syst)±0.01(B),
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B(B0s→ψ(2S)π+π−)B(B0s→J/ψπ+π−)=0.34±0.04(stat)±0.03(syst)±0.01(B),
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where the third uncertainty corresponds to the uncertainties of the dilepton branching fractions of the J/ψ and ψ(2S) meson decays.
Original language | English |
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Pages (from-to) | 403-419 |
Number of pages | 17 |
Journal | Nuclear physics b |
Volume | B871 |
Early online date | 26 Feb 2013 |
DOIs | |
Publication status | Published - 21 Jun 2013 |