Abstract
The \(K_S-K_L\) (SL) asymmetry occurs in the two-body charmed baryon decay with neutral kaon contained in their final states.In this work, based on the topological diagram approach and separated contributions calculated in naive factorization and the pole model, we provide explicit predictions on SL asymmetries for all the singly charmed baryon two-body decays. Especially, for the first time, we predict a sizable SL asymmetry for \(\Omega_c\) decays in its unique decay channel \(\Omega_c\to \Xi^0 K_{S,L}\). Among the four groups of decays in antitriplet charmed baryons, the \(R\) values for \(\Xi_c^+\to \Sigma^+ K_{S,L}\) and \(\Xi_c^0\to \Sigma^0 K_{S,L}\) are around \(-0.5\), which are promising to be measured. However, the other two groups \(\Lambda_c^+\to p K_{S,L}\) and \(\Xi_c^0\to \Lambda^0 K_{S,L}\) are relatively small. Our predictions are partially consistent with theoretical results provided by two other groups and an examination by future experiments is highly anticipated.
Highlights
INTRODUCTIONProgress has been made in the experimental study of charm baryons
In recent years, progress has been made in the experimental study of charm baryons
We find that SL values can be as large as one-half in the two types of modes Ξ+c → Σ+KS,L and Ξ0c → Σ0KS,L, while in the two modes Λ+c → pKS,L and Ξ0c → Λ0 their values are relatively small, less than 10%
Summary
Progress has been made in the experimental study of charm baryons. Both Belle [2] and BESIII [3] have measured the absolute branching fraction of the decay Λ+c → pK−π+, leading to a new average of (6.28 ± 0.32)% for this benchmark mode quoted by the Particle Data Group (PDG) [1]. Though no two-body decays for doubly Cabibbo-suppressed (DCS) processes have been measured yet, it is anticipated regarding the recent published white paper [14] on its future prospect by BESIII. A full calculation of charmed baryon decays should contain contributions from both factorizable and nonfactorizable components.
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