Abstract

The principle of local gauge invariance is applied to fractional wave equations and the interaction term is determined up to order o(gˉ)o(\bar{g}) in the coupling constant gˉ\bar{g}. As a first application, based on the Riemann-Liouville fractional derivative definition, the fractional Zeeman effect is used to reproduce the baryon spectrum accurately. The transformation properties of the non relativistic fractional Schr\"odinger-equation under spatial rotations are investigated and an internal fractional spin is deduced.Comment: remarks on fractional spin added, references added, in press Phys.Lett.

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