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Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays
Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays
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Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays
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Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays
Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays

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Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays
Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays
Journal Article

Improved measurement of η/η′ mixing in B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ decays

A
2025
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Overview
Abstract Branching fraction ratios between the decays B s 0 → J / ψ η ′ $$ {B}_{(s)}^0\\to J/\\psi {\\eta}^{\\left(\\prime \\right)} $$ are measured using proton-proton collision data collected by the LHCb experiment at centre-of-mass energies of 7, 8 and 13 TeV, corresponding to an integrated luminosity of 9 fb −1. The measured ratios of these branching fractions are B B 0 → J / ψη ′ B B 0 → J / ψη = 0.48 ± 0.06 ± 0.02 ± 0.01 , B B s 0 → J / ψη ′ B B s 0 → J / ψη = 0.80 ± 0.02 ± 0.02 ± 0.01 , $$ {\\displaystyle \\begin{array}{c}\\frac{\\mathcal{B}\\left({B}^0\\to J/{\\psi \\eta}^{\\prime}\\right)}{\\mathcal{B}\\left({B}^0\\to J/\\psi \\eta \\right)}=0.48\\pm 0.06\\pm 0.02\\pm 0.01,\\\ {}\\frac{\\mathcal{B}\\left({B}_s^0\\to J/{\\psi \\eta}^{\\prime}\\right)}{\\mathcal{B}\\left({B}_s^0\\to J/\\psi \\eta \\right)}=0.80\\pm 0.02\\pm 0.02\\pm 0.01,\\end{array}} $$ where the uncertainties are statistical, systematic and related to the precision of the η (′) branching fractions, respectively. They are used to constrain the η/η′ mixing angle, ϕ P, and to probe the presence of a possible glueball component in the η′ meson, described by the gluonic mixing angle ϕ G. The obtained results are ϕ P = 41.6 − 1.2 + 1.0 ∘ , ϕ G = 28.1 − 4.0 + 3.9 ∘ , $$ {\\displaystyle \\begin{array}{c}{\\phi}_{\\textrm{P}}={\\left({41.6}_{-1.2}^{+1.0}\\right)}^{\\circ },\\\ {}{\\phi}_{\\textrm{G}}={\\left({28.1}_{-4.0}^{+3.9}\\right)}^{\\circ },\\end{array}} $$ where the uncertainties are statistically dominated. While the value of ϕ P is compatible with existing experimental determinations and theoretical calculations, the angle ϕ G differs from zero by more than four standard deviations, which points to a substantial glueball component in the η′ meson and/or unexpectedly large contributions from gluon-mediated processes in these decays. The absolute branching fractions are also measured relative to that of the well-established B s 0 → J / ψϕ $$ {B}_s^0\\to J/\\psi \\phi $$ decay, which serves as the normalisation channel. These results supersede the previous LHCb measurements and are the most precise to date.
Publisher
SpringerOpen