Precisely determining the ground state mass of Spin-3/2 $Ω_{ccc}$ baryon from Lattice QCD
Navdeep Singh Dhindsa, Debsubhra Chakraborty, Archana Radhakrishnan, Nilmani Mathur, M. Padmanath
TL;DR
This paper determines the ground-state masses of the triply charmed baryon Ω_{ccc} in both parity channels using lattice QCD with six $N_f=2+1+1$ HISQ ensembles and two valence actions (Overlap and HISQ). By forming heavy-quark mass-subtracted splittings and performing continuum extrapolations with $a^2$ (and $a^4$) terms, then adding the experimental $M_{J/ψ}$ contribution, the authors obtain $M_{Ω_{ccc}}(3/2^+)=4793(5)^{+11}_{-8}$ MeV and $M_{Ω_{ccc}}(3/2^-)=5094(12)^{+19}_{-17}$ MeV, the most precise lattice results to date. The study demonstrates cross-method consistency between Overlap and HISQ valence quarks on fine lattices, validates hyperfine splittings against experimental expectations, and provides a robust benchmark for forthcoming experimental measurements and theoretical studies of confinement in triply heavy systems. Overall, the results advance the precision frontier in heavy baryon spectroscopy and offer critical targets for high-luminosity facilities seeking to observe the Ω_{ccc}.
Abstract
We present the most precise determination to date of the ground-state masses of the triply charmed baryons with both parities, obtained by continuum extrapolation and fully addressing the systematic uncertainties. The calculations are performed on six $N_f=2+1+1$ HISQ ensembles, generated by the MILC collaboration, with two complementary setups for the valence charm action, one using the HISQ action and the other using the overlap fermion action. Our prediction for the mass of the lowest two triply charmed spin-3/2 baryons are: $M_{Ω_{ccc}} (3/2^{+}) = 4793 (5) \left(^{+11}_{-8}\right)$ MeV, and $M_{Ω_{ccc}} (3/2^{-}) = 5094 (12) \left(^{+19}_{-17}\right)$ MeV.
