Lifetimes of Doubly Charmed Baryons
arXiv:1809.08102 · doi:10.1103/PhysRevD.98.113005
Abstract
The lifetimes of doubly charmed hadrons are analyzed within the framework of the heavy quark expansion (HQE). Lifetime differences arise from spectator effects such as $W$-exchange and Pauli interference. The $Î_{cc}^{++}$ baryon is longest-lived in the doubly charmed baryon system owing to the destructive Pauli interference absent in the $Î_{cc}^+$ and $Ω_{cc}^+$. In the presence of dimension-7 contributions, its lifetime is reduced from $\sim5.2\times 10^{-13}s$ to $\sim3.0\times 10^{-13}s$. The $Î_{cc}^{+}$ baryon has the shortest lifetime of order $0.45\times 10^{-13}s$ due to a large contribution from the $W$-exchange box diagram. It is difficult to make a precise quantitative statement on the lifetime of $Ω_{cc}^+$. Contrary to $Î_{cc}$ baryons, $Ï(Ω_{cc}^+)$ becomes longer in the presence of dimension-7 effects and the Pauli interference $Î^{\rm int}_+$ even becomes negative. This implies that the subleading corrections are too large to justify the validity of the HQE. Demanding the rate $Î^{\rm int}_+$ to be positive for a sensible HQE, we conjecture that the $Ω_c^0$ lifetime lies in the range of $(0.75\sim 1.80)\times 10^{-13}s$. The lifetime hierarchy pattern is $Ï(Î_{cc}^{++})>Ï(Ω_{cc}^+)>Ï(Î_{cc}^+)$ and the lifetime ratio $Ï(Î_{cc}^{++})/Ï(Î_{cc}^+)$ is predicted to be of order 6.7.
17 pages, 1 figure, version to appear in PRD. arXiv admin note: text overlap with arXiv:1807.00916