Inclusive weak-annihilation decays and lifetimes of beauty-charmed baryons

TL;DR

This paper investigates the inclusive weak-annihilation decays and lifetimes of beauty-charmed baryons $\\Xi_{bc}^{+,0}$ using heavy diquark effective theory, revealing their sensitivity to the $bc$ diquark spin and proposing promising decay channels for experimental detection.

Contribution

It introduces a novel application of heavy diquark effective theory to compute inclusive decay widths and lifetimes of $\\Xi_{bc}^{+,0}$ baryons, highlighting the impact of $bc$ diquark spin configurations.

Findings

Both lifetimes and branching ratios are highly sensitive to the $bc$ diquark spin.

$\\Xi_{bc}^+$ has a longer lifetime and larger decay branching ratios than $\\Xi_{bc}^0$.

Certain exclusive decay channels are promising for experimental searches at the LHC.

Abstract

Imbalanced beauty-charmed baryons $ \Xi_{bc}^{+,0} $ are of great significance to the development of heavy flavor physics. In this work, we study the inclusive weak-annihilation decays of $\Xi_{bc}^{+,0}$ and their contributions to the $\Xi_{bc}^{+,0}$ lifetimes. For the calculation of the inclusive $\Xi_{bc}^{+,0}\to X_{cs}$ decay width where $X_{cs}$ stands for the sum of the final states with charm number +1 and strange number -1, we work in the heavy diquark effective theory which provides us with a convenient technical tool to construct the operator product expansion. The $\Xi_{bc}^{+,0}$ is considered to be a superposition of two states with one containing a spin-0 $bc$ diquark and the other one containing a spin-1 $bc$ diquark. It is found that both the $\Xi_{bc}^{+,0}$ lifetimes and the $\Xi_{bc}^{+,0}\to X_{cs}$ branching ratios are very sensitive to the $bc$ spin in $\Xi_{bc}^{+,0}$. The $\Xi_{bc}^{+,0}\to X_{cd}$ results are also presented. As $\Xi_{bc}^+$ has a longer lifetime than $\Xi_{bc}^{0}$ and bigger branching ratios of similar decay channels, the exclusive decays $\Xi_{bc}^+\to D^{(*)+}\Lambda$, $\Xi_{bc}^+\to \Lambda_c^+\bar{K}^{(*)0}$, $\Xi_{bc}^+\to D^{(*)+}K^-p$, and $\Xi_{bc}^+\to D^{0}\bar{K}^{(*)0}p$ are more promising for experimental searches of $\Xi_{bc}^{+,0}$ at the LHC comparing with exclusive decay $\Xi_{b c} ^{0} \to D^0pK^-$.