Lattice QCD determination of patterns of excited baryon states
Subhasish Basak, R. G. Edwards, G. T. Fleming, K. J. Juge, A. Lichtl,, C. Morningstar, D. G. Richards, I. Sato, S. J. Wallace

TL;DR
This paper uses lattice QCD to compute energies of excited baryon states, revealing patterns consistent with physical states and decomposing higher spin states for the first time.
Contribution
It introduces a novel lattice QCD method to analyze higher spin excited baryons using nonlocal operators and octahedral group representations.
Findings
Patterns of degenerate energies match physical state predictions
First decomposition of spin 5/2 or higher states in lattice QCD
Low-lying excited states align with continuum spin patterns
Abstract
Energies for excited isospin I=1/2 and I=3/2 states that include the nucleon and Delta families of baryons are computed using quenched, anisotropic lattices. Baryon interpolating field operators that are used include nonlocal operators that provide G_2 irreducible representations of the octahedral group. The decomposition of spin 5/2 or higher spin states is realized for the first time in a lattice QCD calculation. We observe patterns of degenerate energies in the irreducible representations of the octahedral group that correspond to the subduction of the continuum spin 5/2 or higher. The overall pattern of low-lying excited states corresponds well to the pattern of physical states subduced to the irreducible representations of the octahedral group.
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