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 givesFor , 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 givesThus is an Erlang distribution of shape three, equal in law to the sum of three independent exponentials. Addition of independent means and variances yieldsFor 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 givesThis 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 isEquivalently, 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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