Integrating against the Gamma density gives the moment-generating function of a gamma distribution:
The change of variables reduces the integral to using the gamma function. For the defining integral is infinite. In particular the moment-generating function is finite on a neighbourhood of zero.
Independence makes the moment-generating function of the sum the product of the two moment-generating functions. For ,
The expectations are finite on, for example, , as is the moment-generating function of the candidate Gamma distribution. The uniqueness theorem for moment-generating functions therefore applies, proving
This is additivity of independent gamma distributions with a common rate; a common rate is essential to this specific formula.
An exponential distribution of rate is a Gamma distribution with shape one. Repeated additivity of independent gamma distributions with a common rate therefore gives
With integer shape this is also called an Erlang distribution.
The Poisson interarrival times of a homogeneous Poisson process are independent and identically distributed with the exponential distribution of rate . Consequently are independent random variables and their joint probability density is
Here is the second interarrival duration, rather than the time of the second arrival.
The inverse change of variables is , , on , . Its absolute Jacobian determinant is
The change of variables for probability densities therefore gives
This factorizes on a product domain into a unit uniform density in and a shape-two Gamma density in . Thus and are independent, with and . This is the shape- case of beta-gamma independence.
By part (c) with , let for independent and identically distributed exponential random variables. The requested integral is . Each summand has expectation one and variance one, so the central limit theorem gives
Zero is a continuity point of the standard normal distribution, and consequently

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