Flavor structure of $\Lambda$ baryons from lattice QCD: From strange to charm quarks

TL;DR

This study uses lattice QCD to analyze the flavor structure and mass evolution of $\Lambda$ baryons with strange and charm quarks, revealing stability in most states and a notable flavor change in the lowest negative-parity state.

Contribution

It provides a detailed lattice QCD analysis of $\Lambda$ baryons across different heavy quark masses, highlighting flavor structure stability and the evolution of energy levels.

Findings

Energy levels increase linearly with quark mass

Most states maintain stable flavor structure

Lowest negative-parity state changes flavor composition

Abstract

We study $\Lambda$ baryons of spin-parity $\frac{1}{2}^{\pm}$ with either a strange or charm valence quark in full 2+1 flavor lattice QCD. Multiple $SU(3)$ singlet and octet operators are employed to generate the desired single baryon states on the lattice. Via the variational method, the couplings of these states to the different operators provide information about the flavor structure of the $\Lambda$ baryons. We make use of the gauge configurations of the PACS-CS Collaboration and chirally extrapolate the results for the masses and $SU(3)$ flavor components to the physical point. We furthermore gradually change the hopping parameter of the heaviest quark from strange to charm to study how the properties of the $\Lambda$ baryons evolve as a function of the heavy quark mass. It is found that the baryon energy levels increase almost linearly with the quark mass. Meanwhile, the flavor structure of most of the states remains stable, with the exception of the lowest $\frac{1}{2}^{-}$ state, which changes from a flavor singlet $\Lambda$ to a $\Lambda_c$ state with singlet and octet components of comparable size. Finally, we discuss whether our findings can be interpreted with the help of a simple quark model and find that the negative-parity $\Lambda_c$ states can be naturally explained as diquark excitations of the light $u$ and $d$ quarks. On the other hand, the quark-model picture does not appear to be adequate for the negative-parity $\Lambda$ states, suggesting the importance of other degrees of freedom to describe them.