“…The operator L has a basis of eigenfunctions φ ν n (see Subsection 2.1) in L 2 ((0, 1), µ), where dµ(x) = x 2ν+1 dx, see [15,Chapter 2]. Therefore, by applying the Fourier method, we see that the solution of the Dirichlet problem (1.1) is u(x, t) = e −t It is known, see [4,16,21,22], that such operator is bounded on L p ((0, 1), µ), for 1 < p < ∞, and of weak type (1,1). Then, as usual, we can get the desired almost everywhere convergence.…”