Excited state baryon spectroscopy from lattice QCD with spin identification

TL;DR

This study uses advanced lattice QCD techniques with spin-specific operators to accurately identify excited baryon states and analyze their spectrum, revealing insights into their structure and symmetry properties.

Contribution

Introduces a method using SU(2)-transformed lattice operators for precise spin identification in baryon spectra, overcoming previous ambiguities.

Findings

Confirmed approximate rotational symmetry in N* spectrum

Found low-lying states match SU(6)xO(3) symmetry

Challenged quark-diquark and parity doubling models

Abstract

Lattice QCD calculations are presented for the spectra of N* excited states with spins up to J = 7/2. Ambiguities of the standard method of spin identification are shown to be overcome by the use of lattice operators that transform according to SU(2) symmetry restricted to the lattice. Such operators are labeled by their continuum spins. Overlaps of the operators with the states obtained by diagonalizing matrices of correlation functions provide a clear link between continuum spins and lattice states, allowing spins to be identified. Evidence for an approximate realization of rotational symmetry in the N* spectrum is presented. In simulations with pion mass = 392 MeV, the low-lying excited states of lattice QCD are found to have the same quantum numbers as the states of SU(6)xO(3) symmetry. The lattice spectra are inconsistent with either a quark-diquark model or parity doubling of states and they suggest that the J = 1/2 Roper resonance may have a complex structure consisting of contributions from L=0, 1 and 2.