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VOLUME 99 (2014) | ISSUE 2 | PAGE 61
Magnetic moments of negative parity baryons from effective hamiltonian approach to QCD
DOI: 10.7868/S0370274X14020015
Abstract
Magnetic moments of S11(1535) and S11(1650) baryons are studied in the framework of the relativistic three-quark Hamiltonian derived in the Field Correlation Method. The baryon magnetic moments are expressed via the average current quark energies which are defined by the fundamental QCD parameters: the string tension σ, the quark masses, and the strong coupling constant αs. Resulting magnetic moments for the JP=1/2- nucleons are compared both to model calculations and to those from lattice QCD.