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Yu-Bin Zhang

Publications and source records attributed to Yu-Bin Zhang.

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Probing the inner structures of the observed $Ξ_b$ and $Ξ_b'$ resonances

To shed light on the inner structure of the observed single-bottom strange baryons, in this work we systematically study the Okubo-Zweig-Iizuka allowed strong decay properties of $1P$- and $2S$-wave $Ξ_b$ and $Ξ_b'$ baryons within the $j-j$ coupling scheme in the framework of the quark pair creation model. For a comparison, we also give the predictions of the chiral quark model. The calculations indicate that: (i) The $1P$-wave $λ$-mode $Ξ_b$ states $Ξ_b|J^P=1/2^-,1\rangle_λ$ and $Ξ_b|J^P=3/2^-,1\rangle_λ$ are highly promising candidates for the observed state $Ξ_b(6087)$ and $Ξ_b(6095)/Ξ_b(6100)$, respectively. The $1P$-wave $ρ$-mode $Ξ_b$ states $Ξ_b|J^P=3/2^-,2\rangle_ρ$ and $Ξ_b|J^P=5/2^-,2\rangle_ρ$ are likely candidates for the state $Ξ_b(6227)$. Meanwhile, we cannot rule out the possibility that $Ξ_b(6227)$ could be a candidate of the $1P$-wave $λ$-mode $Ξ_b'$ state $Ξ_b'|J^P=3/2^-,2\rangle_λ$ or $Ξ_b'|J^P=5/2^-,2\rangle_λ$. (ii) For the other $1P$-wave $ρ$-mode $Ξ_b$ states and $1P$-wave $λ$-mode $Ξ_b'$ states, they may be moderate states with a width of several tens of MeV. Their main decay channels are $Ξ_bπ$, $Ξ_b'π$, $Ξ_b^*π$ or $Λ_b\bar{K}$. The width of the $1P$-wave $ρ$-mode $Ξ_b'$ states are slightly broader, approximately several tens to over one hundred MeV, and the dominant decay channels are $Ξ_b'π$, $Ξ_b^*π$, $Σ_bK$ or $Σ_b^*K$. (iii) The $2S$-wave $λ$-mode $Ξ_b$ and $Ξ_b'$ states are most likely to be relatively narrow state with a width of only a few to around ten MeV, and they mainly decay into $Ξ_b'π$ or $Ξ_b^*π$. In addition, the $2S$-wave $λ$-mode $Ξ_b'$ states may also mainly decay into the $1P$-wave $Ξ_b$ baryon via the pionic decay processes.

hep-ph

Possible explanations of the observed $Λ_c$ resonances

Inspired by the latest experimental progress, we systematically study the OZI-allowed two-body strong decay properties of $1P$-, $1D$-, $2S$- and $2P$-wave $Λ_c$ baryons within the $j $-$j$ coupling scheme in the framework of the quark pair creation model. The calculations indicate that: (i) Taking the observed states $Λ_c(2595)^+$ and $Λ_c(2625)^+$ as the $1P$-wave $λ$-modes states $Λ_c|J^P=1/2^-,1\rangle_λ$ and $Λ_c|J^P=3/2^-,1\rangle_λ$, respectively, we can reproduce the experimental data well in theory. (ii) Combining with the measured mass and the decay properties of $Λ_c(2860)^+$, this excited state can be explained as $1D$-wave $λ$-mode state $Λ_c|J^P=3/2^+,1\rangle_{λλ}$. (iii) The newly observed state $Λ_c(2910)^+$ may be assigned as one of the $1P$-wave $ρ$-mode states $Λ_c|J^P=3/2^-,2\rangle_ρ$ or $Λ_c|J^P=5/2^-,2\rangle_ρ$. Meanwhile, we notice that the partial decay width ratio between $Σ_cπ$ and $Σ_c^*π$ for the two candidates is significantly different. Hence, experimental progress in this ratio measurement may shed light on the nature of $Λ_c(2910)^+$. (iv) According to the properties of $Λ_c(2765)^+$, we find that the $2S$-wave $λ$-mode state $Λ_{c1}|J^P=1/2^+,0\rangle_λ$ may be a potential candidate. (v) The $2P$-wave $λ$-mode state $Λ_{c1}|J^P=3/2^-,1\rangle_λ$ is mostly likely to be a good assignment of the controversial state $Λ_c(2940)^+$. Both the total decay width and partial decay ratio between $pD^0$ and $Σ_cπ$ are in good agreement with the observations. (vi) In addition, for the missing $Λ_c$ excitations, we obtain their strong decay properties and hope that's useful for future experimental exploration.

hep-ph