This birth-death process has birth rates and death rates . With , its birth-death master equation is
The first two terms are inflow by a birth from and a death from ; the bracketed term is the total outflow from .
Multiply the birth-death master equation by and sum. Equivalently, a birth changes by and a death by , so
The equation is not closed in the mean because the quadratic death rate introduces the second factorial moment.
For a Poisson random variable of mean ,
Substitution into part (b) gives the closed Riccati equation
Its positive equilibrium is stable on the nonnegative half-line and equals
Thus under the Poisson approximation,
The diffusion approximation of a birth-death process uses the first two jump moments. For these unit upward and downward jumps they give
The factor in is required because the equation is written with , rather than .
Assuming the boundary terms vanish, integration by parts gives
Consequently
which is precisely the discrete first-moment equation in part (b).

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