Let be independent exponential random variables of rate , let and , and define . The strong law of large numbers gives , so there is no finite-time explosion. This defines the Poisson process of rate .
For , repeated convolution gives the gamma distribution with density . Independence of gives
For , the probability is . Hence for all , including the degenerate law at .
Convolve three rate- exponential distributions. The first two have convolution density ; convolving once more gives
Thus is an Erlang distribution of shape three, equal in law to the sum of three independent exponentials. Addition of independent means and variances yields
For the moment-generating function is infinite.
Realize each holding time as a consecutive block of three exponential holding times from one Poisson process . The renewal count is then pathwise under this coupling. If is the remainder of modulo three, and . Taking expectations gives
This proves the formula without assuming that the renewal count itself is Poisson.
The equilibrium-delay theorem for a renewal process with positive holding time , finite mean , and distribution function says that the first future renewal must have the equilibrium residual-life distribution,
independently of subsequent ordinary holding times. This is the residual lifetime seen at a stationary observation time, rather than an ordinary inter-renewal lifetime.
Here and . Thus the required initial-delay density is
Equivalently, choose with equal probability a sum of one, two, or three independent rate- exponential random variables. The three Erlang distributions have densities that average to the displayed density. A concrete stationary construction chooses the phase modulo three of a stationary Poisson clock uniformly; the number of exponential stages until its next third-stage renewal is then uniform on .

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