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, provingThis 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 givesWith 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 isHere is the second interarrival duration, rather than the time of the second arrival.
The inverse change of variables is , , on , . Its absolute Jacobian determinant isThe change of variables for probability densities therefore givesThis 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 givesZero is a continuity point of the standard normal distribution, and consequently
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