In level flight, T - D = m * a, where a is acceleration, m is mass of aircraft, T is thrust, and D is drag; or a = (T - D) / m. T = thrust of engine, D = drag = 0.5 * C_D * rho * v^2 * S, where C_D = coefficient of drag, rho = density of air, v = velocity of aircraft, S = wing area. Let me define Z as 0.5 * rho * v^2 * S. Then D = C_D * Z. Also from aerodynamics of airfoils, C_D = C_D_min + C_L^2 / (pi * e * A), where C_D_min is drag at zero lift, e is Oswald's efficiency factor, and A is aspect ratio of the wings. In level flight, L = W = weight = m * g = C_L * Z. Overall, a = T / m - C_D_min * Z / m - m * g^2 / (Z * pi * e * A).
So, in level flight, a is highly negatively impacted by m. Not only do you have the T/m term, but m * g^2 / (Z * pi * e *A) is substantial (the contribution to drag as a result of generating lift). C_D_min is much smaller than drag due to lift in level flight.
In a vertical dive pulling zero g's of lift, T + W - D = m * a. Overall, a = T / m + g - C_D_min * Z / m, as lift and thus C_L is zero. Here, T/m is negatively impacted by m, but at all speeds for WWII aircraft, and especially at speeds above near zero, T/W is much less than 1. So T/m is much less than g. C_D_min * Z / m is reduced as m gets larger, so the negative contribution from parasitic drag is lessened by larger mass.
Assuming that I haven't made any math errors (which is certainly possible), general trends from above: all else equal, a heavier plane accelerates more poorly in level flight (no surprise there) but accelerates better in a vertical dive (at least when starting at a high enough speed) compared to a lighter version.