Put . The independent pair has the same joint distribution as from part (ii), because both first coordinates are uniform and independent of the same sum law. Hence
Consequently
The rate is one. This multiplication identity is the mechanism behind the exponential invariant law of a random affine recursion.
Every has the same exponential distribution, so for . Part (ii) gives . Applying Slutsky's theorem to yields
The limiting probability distribution does not depend on . This is precisely the attraction to the exponential invariant law of a random affine recursion.
Figure 1.
Common random inputs make different initial values approach the same stationary trajectory
. Original simulations of the affine recursion with shared inputs. The right panel compares an exactly propagated path difference with its unconditional expected value; the geometric expectation estimate, rather than the simulation, proves convergence. Details.