Inspired by recent research on the \(p \Omega\) and \(p \bar{\Lambda }\) systems, we investigate the \(p \bar{\Omega }\) systems within the framework of the quark delocalization color-screening model. Our results indicate that the nucleon– \(\bar{\Omega }\) interaction is slightly stronger than the nucleon– \(\Omega\) interaction, implying a higher likelihood of the \(p \bar{\Omega }\) system to forming bound states. Dynamic calculations show that the \(p \bar{\Omega }\) systems with \(J^{P}=1^{-}\) and \(2^{-}\) form bound states, whose binding energies are deeper than that of the \(p \Omega\) system with \(J^{P}=2^{+}\) . The scattering phase shifts and extracted scattering parameters also support the existence of \(p \bar{\Omega }\) bound states. Additionally, we discuss the behavior of the femtoscopic correlation function for \(p \bar{\Omega }\) pairs for the first time. Building on the recent experimental progress on the \(p\Omega\) correlation function, future femtoscopic investigations of the \(p\bar{\Omega }\) system in heavy-ion collisions will be particularly valuable for constraining baryon–antibaryon interactions.
