The Newtonian potential of a merely continuous function f does not have, in general, continuous second order derivatives. As a consequence, the Poisson equation Δ u = - f {Δ u=-f} is not, in general, solvable in the pointwise classical sense. However, a 1909 result by Pizzetti shows that the previous Poisson equation is pointwise solvable in a suitable generalized sense for every continuous function f . We show how Pizzetti’s approach works for wide classes of hypoelliptic linear second order PDEs.
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Alessia Elisabetta Kogoj (2026) studied this question.
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