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Divyajyoti Pandey

Publications and source records attributed to Divyajyoti Pandey.

2 recordsLinked to original sources

Ground-State Heavy-Baryon Mass Spectrum in the Relativistic Independent Quark Model

We extend our work to compute the ground-state baryon mass spectrum containing charm and bottom quarks in the relativistic independent quark (RIQ) model with an average flavor--independent confining potential in equally mixed scalar--vector harmonic form. Each quark moves as a Dirac particle inside the potential. The resulting core mass is then corrected perturbatively, accounting for the pion self-energy, pion exchange, and pairwise color--electric and color--magnetic one-gluon exchange. Six input parameters common to every baryon: the potential parameters (confinement strength, the potential offset) and the $u(=d)$, $s$, $c$, and $b$ constituent quark masses are optimized using a few experimentally measured baryon states. The model then uses these optimized parameters to predict the mass spectra of doubly heavy, mixed-$bc$, and triply heavy baryons. We compare our predictions with lattice QCD, relativistic quark model results, and available experimental measurements. Our results are consistent with these model predictions and experimental results.

hep-ph↗

Mass spectrum of S-wave mesons in the relativistic independent quark model

The confining strength or model parameters and constituent quark masses are reparametrized for predicting the ground state meson masses. We analyzed these from the hyperfine splitting of $S$-wave heavy-flavored, heavy-light and light (except non-strange) mesons in the framework of a relativistic independent quark (RIQ) model with one gluon exchange and centre-of-mass correction. These mesons with spin parity $J^P=0^-$ and $1^-$, the masses obtained are in accordance with the experimental physical masses. The results will serve as good complementary tools in further study of hadron dynamics and will behave as a foundation for the higher excited and exotic states of hadrons.

hep-ph↗