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Rigidity and stability of the Leibniz and the chain rule

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Abstract

We study rigidity and stability properties of the Leibniz and chain rule operator equations. We describe which non-degenerate operators V, T 1, T 2,A: C k(ℝ) → C(ℝ) satisfy equations of the generalized Leibniz and chain rule type for f, gC k(ℝ), namely, V (f · g) = (T 1 f) · g + f · (T 2 g) for k = 1, V (f · g) = (T 1 f) · g + f · (T 2 g) + (Af) · (Ag) for k = 2, and V (fg) = (T 1 f) ○ g · (T 2 g) for k = 1. Moreover, for multiplicative maps A, we consider a more general version of the first equation, V (f · g) = (T 1 f) · (Ag) + (Af) · (T 2 g) for k = 1. In all these cases, we completely determine all solutions. It turns out that, in any of the equations, the operators V, T 1 and T 2 must be essentially equal. We also consider perturbations of the chain and the Leibniz rule, T (fg) = Tfg · Tg + B(fg, g) and T (f · g) = Tf · g + f · Tg + B(f, g), and show under suitable conditions on B in the first case that B = 0 and in the second case that the solution is a perturbation of the solution of the standard Leibniz rule equation.

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König, H., Milman, V. Rigidity and stability of the Leibniz and the chain rule. Proc. Steklov Inst. Math. 280, 191–207 (2013). https://doi.org/10.1134/S0081543813010136

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