We introduce a fractional Fokker-Planck equation (FFPE) for Levy flights in
the presence of an external field. The equation is derived within the fram
ework of the subordination of random processes which leads to Levy flights.
It is shown that the coexistence of anomalous transport and a potential di
splays a regular exponential relaxation toward the Boltzmann equilibrium di
stribution. The properties of the Levy-flight FFPE derived here are compare
d with earlier findings for a subdiffusive FFPE. The latter is characterize
d by a nonexponential Mittag-Leffler relaxation to the Boltzmann distributi
on. In both cases, which describe strange kinetics, the Boltzmann equilibri
um is reached, and modifications of the Boltzmann thermodynamics are not re
quired.