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Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass
Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass
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Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass
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Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass
Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass

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Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass
Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass
Journal Article

Observation of Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻decays and a measurement of theΛ_(b)⁰baryon mass

2016
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Overview
The decays Λ_(b)⁰ → ψ(2S)pK⁻and Λ_(b)⁰ → J/ψ π⁺ π⁻ pK⁻are observed in a data sample corresponding to an integrated luminosity of 3fb ⁻¹ , collected in proton-proton collisions at 7 and 8TeV centre-of-mass energies by the LHCb detector. Theψ(2S)mesons are reconstructed through the decay modesψ(2S)→μ⁺μ⁻andψ(2S)→ J/ψπ⁺π⁻ . The branching fractions relative to that of Λ_(b)⁰ → J/ψ pK⁻are measured to be eqnarray* B(_(b)⁰ (2S) pK⁻) B(_(b)⁰ J/ pK⁻) & = & (20.70 0.76 0.46 0.37)10⁻2 , B(_(b)⁰ J/ ⁺ ⁻ pK⁻) B(_(b)⁰ J/ pK⁻) & = & (20.86 0.96 1.34)10⁻2 , eqnarray* where the first uncertainties are statistical, the second are systematic and the third is related to the knowledge ofJ/ψandψ(2S)branching fractions. The mass of theΛ_(b)⁰baryon is measured to be M(Λ_(b)⁰) = 5619.65 ± 0.17 ± 0.17\\mathrm{MeV}{/}{c}²,where the uncertainties are statistical and systematic.
Publisher
Springer