“…The basic ingredients of the calculus of F q -linear functions [9] are the Frobenius operator τ u = u q , the difference operator ∆u(t) = u(xt) − xu(t) (1.1) introduced in [3], and the nonlinear (F q -linear) operator d = τ −1 ∆ called the Carlitz derivative. The latter appears, as an analog of the classical derivative, in the theory of ordinary differential equations for F q -linear functions, which has been developed both in the traditional analytic direction (the Cauchy problem [10,13], regular singularity [11], new special functions defined via differential equations [14]) and within various algebraic frameworks (analogs of the canonical commutation relations of quantum mechanics [8,9], umbral calculus [12], an analog of the Weyl algebra [10,15,2]). Note that in our situation the meaning of a polynomial coefficient in a differential equation is not a usual multiplication by a polynomial, but the action of a polynomial in the operator τ (similarly, for holomorphic coefficients).…”