The moment generating function is wherever that expectation is finite. A useful continuity theorem says that if the moment generating functions are finite on a common open interval containing zero and converge pointwise there to the moment generating function of a probability distribution, then the corresponding variables converge in distribution to that law. Equivalently one may assume a finite limiting function on such a neighborhood, with the usual continuity at zero, and obtain the uniquely determined limiting law.
For the gamma density, integrating the exponential against the density and changing variable to givesFor the waiting time to one head, independence of successive tosses gives for . Summing the geometric series givesThe waiting times between consecutive heads are independent copies of , so their sum has moment generating function . ConsequentlyFor fixed , numerator and denominator have leading terms and as . A fixed neighborhood of zero is inside the convergence domain for all sufficiently small , so the continuity theorem applies. The limiting distribution isequivalently a chi-squared distribution with degrees of freedom.
Condition on the intermediate state at time . The Markov property and time homogeneity giveThese nonnegative sums are valid on a countable state space. Starting from , , induction gives . Conditioning on the initial state now yields . If , induction gives for every , so all one-time distributions equal the stationary initial distribution.
A state is recurrent if, starting there, the probability of returning at some strictly positive time is one. It is transient if that return probability is strictly less than one. Suppose communicate. Choose with and . Chapman–Kolmogorov givesIf is recurrent, summing over and using the supplied return-series criterion makes the return series for diverge, so is recurrent. Interchanging the states proves equivalence; therefore transience is also constant on a communicating class.
For the nearest-neighbor walk, return in an odd number of steps is impossible. A return in steps requires exactly steps each way, soAt , the return series diverges like . If and , then , so it converges by exponential decay. At or one the walk never returns. Hence .
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