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Nongnapat Ponkhuha

Publications and source records attributed to Nongnapat Ponkhuha.

2 recordsLinked to original sources

Heavy-Quark Spin Symmetry Violation effects in Charmed Baryon Production

In this work, we investigate the Heavy-Quark Spin Symmetry (HQSS) exhibited in the effective Lagrangians governing the three-point interactions of $D$ mesons, charmed baryons, and nucleons. We first construct the effective Lagrangians, and there are 12 distinct terms. As a result, we observe that the invariant Lagrangian under HQSS manifests exclusively in the pseudoscalar $D$ mesons coupling to nucleons and $Λ_c$ baryons, whereas nucleons and $Σ_c$ ($Σ_c^*$) baryons only couple with vector $D$ mesons. By taking into account the violated heavy-quark spin transformation, one can recover all interactions from the effective Lagrangians. Furthermore, we compute the differential cross-sections of the $p\bar p \to Y_c\bar{Y}_c'$ scatterings, where $Y_c,\bar{Y_c}' = Λ_c,~Σ_c,~Σ_c^*$, to reveal the residue of the violating HQSS (VHQSS) on charmed baryon production. Ultimately, by accounting for VHQSS, we aim for precise predictions of production rates, which are essential for the High-Energy Storage Ring (HESR) experiments at the Facility for Antiproton and Ion Research (FAIR).

hep-ph↗

Two-pion emission decays of negative parity singly heavy baryons

We investigate two-pion emission decays of singly charmed and bottom baryons, focusing on $Λ_Q^*(1P)$ and $Ξ_Q^*(1P)$ with $Q=c$ (charm) or $b$ (bottom) quarks and $J^P=1/2^-,3/2^-$, belonging to antisymmetric flavor triplet $\bar{\boldsymbol{3}}_F$. Our analysis encompasses both sequential processes, involving intermediate states belonging to symmetric flavor sextet $\boldsymbol{6}_F$ such as $Σ_Q(1S)$ and $Ξ_Q^\prime(1S)$ respectively with $J^P=1/2^+,3/2^+$, derived from the chiral quark model, and direct process crucial for comparison with experimental data, whose coupling constants estimated using the chiral-partner scheme. We also incorporate the convolution of the parent particle's mass for the Dalitz plot, enabling a more realistic comparison with experimental data. We scrutinize the Dalitz plots of these negative parity states in light of recent Belle measurements for $Λ_c(2625)^+$. Our findings support the assignment of $Λ_c(2625)^+$ as the $λ$-mode excitation with $J^P=3/2^-$ in the quark model, deduced from the the ${Λ_cπ}$ invariant mass distribution, and we then give predictions for other cases, including the $Ξ_Q^*$ decays. The observed asymmetry in the ${ππ}$ invariant mass distribution underscores the important role of the direct process, reflecting the chiral-partner structure in the heavy baryon sector. It is evident that the presence of the direct process is not significant in the three-body decays unless the $S$-wave resonance contribution is suppressed. We suggest further experimental verification to test our predictions and get more insights into the structure of heavy baryons.

hep-ph↗