Birth-death processes: transient laws, extinction and generating functions

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Definition 17. A homogeneous Markov process X={X(t),t⩾0}X = \left\{ X(t), t \geqslant 0\right\} with state space S={0,1,…}S = \left\{ 0,1, \ldots \right\} is called a birth-and-death process if its infinitesimal matrix QQ has the following form

qi,i−1=μi,qii=−(λi+μi),qi,i+1=λi,qij=0 for ∣i−j∣>1, q_{i, i-1} = \mu _{i}, \quad q_{i i} = -\left(\lambda _{i}+\mu _{i}\right), \quad q_{i, i+1} = \lambda _{i}, \quad q_{i j} = 0 \quad \text{ for } \quad \left|i-j\right| > 1,

where μ0=0,μi>0,i⩾1\mu_{0} = 0, \mu_{i} > 0, i \geqslant 1 and λi>0,i⩾0\lambda_{i} > 0, i \geqslant 0. If μi=0\mu_{i} = 0 for all i⩾0i \geqslant 0, one speaks of a birth process, and if λi=0,i⩾0\lambda_{i} = 0, i \geqslant 0, of a death process.

The backward and forward systems of Kolmogorov equations for the matrices P(t)=(pij(t))i,j∈SP(t) = \left(p_{i j}(t)\right)_{i, j \in \mathrm{S}}, t⩾0t \geqslant 0, have, respectively, the form

pij′(t)=∑kqikpkj(t)(65) p_{i j}^{\prime }(t) = \sum _{k} q_{i k} p_{k j}(t) \tag {65}

and

pij′(t)=∑kpik(t)qkj for all i,j∈S.(72) p_{i j}^{\prime }(t) = \sum _{k} p_{i k}(t) q_{k j} \quad \text{ for all } \quad i, j \in \mathrm{S} . \tag {72}

Solutions are sought in the class of semistochastic matrices (P(t))t⩾0(P(t))_{t \geqslant 0}, for which ∑jpij(t)⩽1,t⩾0,i∈S\sum_{j} p_{i j}(t) \leqslant 1, t \geqslant 0, i \in \mathrm{S}. If it turns out that ∑jpij(t)=1\sum_{j} p_{i j}(t) = 1 for all t⩾0,i∈St \geqslant 0, i \in \mathrm{S}, then one speaks of a proper solution.

Suppose a birth process is such that ∑iλi−1<∞\sum_{i} \lambda_{i}^{-1} < \infty. Prove that then the system of forward Kolmogorov equations has a unique solution, while the system of backward equations has infinitely many. Prove that if ∑iμi−1<∞\sum_{i} \mu_{i}^{-1} < \infty for a death process, then the system of backward equations has a unique solution, while the system of forward equations has infinitely many, exactly one of which is proper.

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Consider an immigration-death process XX, being a birth-death process with birth rates λn=λ\lambda_{n} = \lambda and death rates μn=nμ\mu_{n} = n \mu. Find the transition matrix of the jump chain YY, and show that it has as stationary distribution

πn=12(n!)(1+nρ)ρne−ρ \pi _{n} = \frac{1}{2(n!)}\left(1+\frac{n}{\rho }\right) \rho ^{n} e^{-\rho }

where ρ=λ/μ\rho = \lambda / \mu. Explain why this differs from the stationary distribution of XX.

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Consider the birth-death process XX with λn=nλ\lambda_{n} = n \lambda and μn=nμ\mu_{n} = n \mu for all n≥0n \geq 0. Suppose X(0)=1X(0) = 1 and let η(t)=P1(X(t)=0)\eta (t) = \mathbb {P}_{1}\left(X(t) = 0\right). Show that η\eta satisfies the differential equation

η′(t)+(λ+μ)η(t)=μ+λη(t)2 \eta ^{\prime }(t)+(\lambda +\mu ) \eta (t) = \mu +\lambda \eta (t)^{2}

Hence find η(t)\eta (t), and calculate P1(X(t)=0∣X(u)=0)\mathbb {P}_{1}\left( X(t) = 0 \mid X(u) = 0 \right) for 0<t<u0 < t < u.

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For the birth-death process of the previous exercise with λ<μ\lambda < \mu, show that the distribution of X(t)X(t), conditional on the event {X(t)>0}\left\{ X(t) > 0\right\}, converges as t→∞t \rightarrow \infty to a geometric distribution.

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Let XX be a birth-death process with λn=nλ\lambda_{n} = n \lambda and μn=nμ\mu_{n} = n \mu, and suppose X(0)=1X(0) = 1. Show that the time TT at which X(t)X(t) first takes the value 0 satisfies

E[T∣T<∞]={1λlog⁡(μμ−λ) if λ<μ1μlog⁡(λλ−μ) if λ>μ \mathbb {E}\left[T \mid T < \infty \right] = \begin{cases} \frac{1}{\lambda } \log \left(\frac{\mu }{\mu -\lambda }\right) & \text{ if } \lambda < \mu \\ \frac{1}{\mu } \log \left(\frac{\lambda }{\lambda -\mu }\right) & \text{ if } \lambda > \mu \end{cases}

What happens when λ=μ\lambda = \mu?

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Let XX be the birth-death process of Exercise (6.11.5) with λ≠μ\lambda \neq \mu, and let Vr(t)V_{r}(t) be the total amount of time the process has spent in state r≥0r \geq 0, up to time tt. Find the distribution of V1(∞)V_{1}(\infty ) and the generating function ∑rsrE[Vr(t)]\sum_{r} s^{r} \mathbb {E}\left[V_{r}(t)\right]. Hence show in two ways that E[V1(∞)]=[max⁡{λ,μ}]−1\mathbb {E}\left[V_{1}(\infty )\right] = [\max \left\{ \lambda , \mu \right\} ]^{-1}. Show further that E[Vr(∞)]=λr−1r−1[max⁡{λ,μ}]−r\mathbb {E}\left[V_{r}(\infty )\right] = \lambda^{r-1} r^{-1}[\max \left\{ \lambda , \mu \right\} ]^{-r}.

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Repeat the calculations of Exercise (6.11.6) in the case λ=μ\lambda = \mu.

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Immigrants arrive at the instants of a Poisson process of rate ν\nu, and each independently founds a simple birth process of rate λ\lambda. At the instants of an independent Poisson process of rate δ\delta, the population is annihilated. Find the probability generating function of the population X(t)X(t), given that X(0)=0X(0) = 0.

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In the framework of Exercise (6.12.2), suppose that each immigrant gives rise to a simple birth-death process of rates λ\lambda and μ\mu. Show that the mean population size stays bounded if and only if δ>λ−μ\delta > \lambda -\mu.

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Consider an immigration-death process X(t)X(t), being a birth-death process with rates λn=λ\lambda_{n} = \lambda, μn=nμ\mu_{n} = n \mu. Show that its generating function G(s,t)=E[sX(t)]G(s, t) = \mathbb {E}\left[s^{X(t)}\right] is given by

G(s,t)={1+(s−1)e−μt}Iexp⁡{ρ(s−1)(1−e−μt)} G(s, t) = \left\{ 1+(s-1) e^{-\mu t}\right\} ^{I} \exp \left\{ \rho (s-1)\left(1-e^{-\mu t}\right)\right\}

where ρ=λ/μ\rho = \lambda / \mu and X(0)=IX(0) = I. Deduce the limiting distribution of X(t)X(t) as t→∞t \rightarrow \infty.

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Let XX be a simple symmetric birth-death process with λn=μn=nλ\lambda_{n} = \mu_{n} = n \lambda, and let TT be the time until extinction. Show that

P(T≤x∣X(0)=I)=(λx1+λx)I \mathbb {P}\left(T \leq x \mid X(0) = I\right) = \left(\frac{\lambda x}{1+\lambda x}\right)^{I}

and deduce that extinction is certain if P(X(0)<∞)=1\mathbb {P}\left(X(0) < \infty \right) = 1. Show that P(λT/I≤x∣X(0)=I)→e−1/x\mathbb {P}\left(\lambda T / I \leq x \mid X(0) = I\right) \rightarrow e^{-1 / x} as I→∞I \rightarrow \infty.

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Let XX be an immigration-death-disaster process, that is, a birth-death process with parameters λi=λ,μi=iμ\lambda_{i} = \lambda , \mu_{i} = i \mu, and with the additional possibility of 'disasters' which reduce the population to 0. Disasters occur at the times of a Poisson process with intensity δ\delta, independently of all previous births and deaths.

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(a)

Show that XX has a stationary distribution, and find an expression for the generating function of this distribution.

(b)

Show that, in equilibrium, the mean of X(t)X(t) is λ/(δ+μ)\lambda /(\delta +\mu ).

References

[БуШи05] Булинский А.В., Ширяев А.Н. Теория случайных процессов. ФИЗМАТЛИТ, 2005.
[GrSt20] Grimmett G.R., Stirzaker D.R. Probability and Random Processes. 4th ed., Oxford University Press, 2020.