“…A procedure, similar to the parametrix method, for constructing the fundamental solution of the Laplace-Beltrami equation on such a manifold ∂u ∂t = 1 2 ∆u was suggested in [9]; namely, the solution was represented by the sum p 0 (t, x, y) = m 0 (t, x, y) + l 0 (t, x, y) = m 0 (t, x, y) + where M (t, x, y) is the discrepancy in the Laplace-Beltrami equation for the initial approximation m(t, x, y). The factor exp{−φ(x, y)/2} in m(t, x, y) removes the singularity with respect to t in the discrepancy.…”