Abstract
A groupoid is alternative if it satisfies the alternative laws and . These laws induce four partial maps on , , , , that taken together form a dynamical system. We describe the orbits of this dynamical system, which allows us to show that th powers in a free alternative groupoid on one generator are well-defined if and only if . We then discuss some number theoretical properties of the orbits, and the existence of alternative loops without two-sided inverses.
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