Abstract

Inspired by a large decay branching ratio (BR) of B+β†’f0(980)K+B^{+}\to f_{0}(980)K^{+} measured by Belle recently, we propose that a significant evidence of the component of nnΛ‰=(uuΛ‰+ddΛ‰)/2n\bar{n}=(u\bar{u}+d\bar{d})/\sqrt{2} in f0(980)f_{0}(980) could be demonstrated in exclusive bβ†’cb\to c decays by the observation of f0(980)f_{0}(980) in the final states BΛ‰β†’D0(βˆ—)Ο€+Ο€βˆ’(KK)\bar{B}\to D^{0(*)} \pi^{+} \pi^{-}(KK) and BΛ‰β†’J/Ψπ+Ο€βˆ’(KK)\bar{B}\to J/\Psi \pi^{+} \pi^{-}(KK). We predict the BRs of BΛ‰β†’D0(βˆ—)(J/Ξ¨)f0(980)\bar{B}\to D^{0(*)} (J/\Psi) f_{0}(980) to be O(10βˆ’4){\cal {O}}(10^{-4}) (O(10βˆ’5){\cal {O}}(10^{-5})) while the unknown wave functions of D(βˆ—)0D^{(*)0} (J/Ξ¨J/\Psi) are chosen to fit the observed decays of BΛ‰β†’D(βˆ—)0Ο€0(J/Ξ¨K0(βˆ—))\bar{B}\to D^{(*)0} \pi^{0} (J/\Psi K^{0(*)}).Comment: 4 pages, 2 figures, Revtex4, version to appear in PR

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    Last time updated on 02/01/2020