The relaxation to equilibrium in many systems that show strange kinetics is
described by fractional Fokker-Planck equations (FFPEs). These can be cons
idered as phenomenological equations of linear nonequilibrium theory. We sh
ow that the FFPEs describe a system whose noise in equilibrium fulfills the
Nyquist theorem. Moreover, we show that for subdiffusive dynamics, the sol
utions of the corresponding FFPEs are probability densities for all cases i
n which the solutions of the normal Fokker-Planck equation (with the same F
okker-Planck operator and with the same initial and boundary conditions) ex
ist. The solutions of the FFPEs for superdiffusive dynamics are not always
probability densities. This fact means only that the corresponding kinetic
coefficients are incompatible with each other and with the initial conditio
ns.