We report a measurement of the branching fraction of the decay $B^0_s\to J/\psi,\phi(1020)B^0_s\to J/\psi,f’_2(1525)B^0_s\to J/\psi,K^+K^-$ branching fraction, including the resonant and non-resonant contributions to the channel. We also determine the -wave contribution within the mass region. The absolute branching fractions are $[B^0_s\to J/\psi,\phi(1020)]=(1.25 \pm 0.07\left(\right)\pm 0.08\left(\right)\pm 0.22\left(f_s\right))\times 10^{-3}[B^0_s\to J/\psi,f’_2(1525)]=(0.26\pm 0.06\left(\right)\pm 0.02\left(\right) \pm 0.05\left(f_s\right))\times 10^{-3}[B^0_s\to J/\psi,K^+K^-] = (1.01\pm 0.09\left(\right) \pm 0.10\left(\right)\pm 0.18\left(f_s\right))\times 10^{-3}$, where the last systematic error is due to the branching fraction of . The branching fraction ratio is found to be $[B^0_s\to J/\psi,f’_2(1525)]/[B^0_s\to J/\psi,\phi(1020)]=(21.5\pm 4.9\left(\right) \pm2.6\left(\right))%^{-1}\Upsilon(5S)$ resonance by the Belle experiment at the KEKB asymmetric-energy collider.

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