TY - JOUR
T1 - Rigidity and stability of the Leibniz and the chain rule
AU - König, Hermann
AU - Milman, Vitali
N1 - Funding Information:
We would like to thank D. Faifman for some useful discussions, in particular concerning Theorem 9. This work was supported in part by the Alexander von Humboldt Foundation, by ISF grant 387/09 and by BSF grant 200 6079.
PY - 2013
Y1 - 2013
N2 - We study rigidity and stability properties of the Leibniz and chain rule operator equations. We describe which non-degenerate operators V, T1, T2,A: Ck(ℝ) → C(ℝ) satisfy equations of the generalized Leibniz and chain rule type for f, g ∈ Ck(ℝ), namely, V (f · g) = (T1f) · g + f · (T2g) for k = 1, V (f · g) = (T1f) · g + f · (T2g) + (Af) · (Ag) for k = 2, and V (f ○ g) = (T1f) ○ g · (T2g) for k = 1. Moreover, for multiplicative maps A, we consider a more general version of the first equation, V (f · g) = (T1f) · (Ag) + (Af) · (T2g) for k = 1. In all these cases, we completely determine all solutions. It turns out that, in any of the equations, the operators V, T1 and T2 must be essentially equal. We also consider perturbations of the chain and the Leibniz rule, T (f ○ g) = Tf ○ g · Tg + B(f ○ g, 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.
AB - We study rigidity and stability properties of the Leibniz and chain rule operator equations. We describe which non-degenerate operators V, T1, T2,A: Ck(ℝ) → C(ℝ) satisfy equations of the generalized Leibniz and chain rule type for f, g ∈ Ck(ℝ), namely, V (f · g) = (T1f) · g + f · (T2g) for k = 1, V (f · g) = (T1f) · g + f · (T2g) + (Af) · (Ag) for k = 2, and V (f ○ g) = (T1f) ○ g · (T2g) for k = 1. Moreover, for multiplicative maps A, we consider a more general version of the first equation, V (f · g) = (T1f) · (Ag) + (Af) · (T2g) for k = 1. In all these cases, we completely determine all solutions. It turns out that, in any of the equations, the operators V, T1 and T2 must be essentially equal. We also consider perturbations of the chain and the Leibniz rule, T (f ○ g) = Tf ○ g · Tg + B(f ○ g, 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.
UR - http://www.scopus.com/inward/record.url?scp=84876447890&partnerID=8YFLogxK
U2 - 10.1134/S0081543813010136
DO - 10.1134/S0081543813010136
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AN - SCOPUS:84876447890
VL - 280
SP - 191
EP - 207
JO - Proceedings of the Steklov Institute of Mathematics
JF - Proceedings of the Steklov Institute of Mathematics
SN - 0081-5438
IS - 1
ER -