Branching process

For the process in representation theory, see Restricted representation § Classical branching rules.

In probability theory, a branching process is a type of mathematical object known as a stochastic process, which consists of collections of random variables indexed by some set, usually natural or non-negative real numbers. The original purpose of branching processes was to serve as a mathematical model of a population in which each individual in generation $n$ produces some random number of individuals in generation $n+1$, according, in the simplest case, to a fixed probability distribution that does not vary from individual to individual. Branching processes are used to model reproduction; for example, the individuals might correspond to bacteria, each of which generates 0, 1, or 2 offspring with some probability in a single time unit. Branching processes can also be used to model other systems with similar dynamics, e.g., the spread of surnames in genealogy or the propagation of neutrons in a nuclear reactor.

A central question in the theory of branching processes is the probability of ultimate extinction, where no individuals exist after some finite number of generations. Using Wald's equation, it can be shown that starting with one individual in generation zero, the expected size of generation n equals μⁿ where μ is the expected number of children of each individual. If μ < 1, then the expected number of individuals goes rapidly to zero, which implies ultimate extinction with probability 1 by Markov's inequality. Alternatively, if μ > 1, then the probability of ultimate extinction is less than 1 (but not necessarily zero; consider a process where each individual either has 0 or 100 children with equal probability. In that case, μ = 50, but probability of ultimate extinction is greater than 0.5, since that's the probability that the first individual has 0 children). If μ = 1, then ultimate extinction occurs with probability 1 unless each individual always has exactly one child.

In theoretical ecology, the parameter μ of a branching process is called the basic reproductive rate.

Mathematical formulation

The most common formulation of a branching process is that of the Galton–Watson process. Let Z_n denote the state in period n (often interpreted as the size of generation n), and let X_n,i be a random variable denoting the number of direct successors of member i in period n, where X_n,i are independent and identically distributed random variables over all n ∈{ 0, 1, 2, ...} and i ∈ {1, ..., Z_n}. Then the recurrence equation is

$Z_{n+1}=\sum _{i=1}^{Z_{n}}X_{n,i}$

with Z₀ = 1.

Alternatively, the branching process can be formulated as a random walk. Let S_i denote the state in period i, and let X_i be a random variable that is iid over all i. Then the recurrence equation is

$S_{i+1}=S_{i}+X_{i+1}-1=\sum _{j=1}^{i+1}X_{j}-i$

with S₀ = 1. To gain some intuition for this formulation, imagine a walk where the goal is to visit every node, but every time a previously unvisited node is visited, additional nodes are revealed that must also be visited. Let S_i represent the number of revealed but unvisited nodes in period i, and let X_i represent the number of new nodes that are revealed when node i is visited. Then in each period, the number of revealed but unvisited nodes equals the number of such nodes in the previous period, plus the new nodes that are revealed when visiting a node, minus the node that is visited. The process ends once all revealed nodes have been visited.

Continuous-time branching processes

For discrete-time branching processes, the "branching time" is fixed to be 1 for all individuals. For continuous-time branching processes, each individual waits for a random time (which is a continuous random variable), and then divides according to the given distribution. The waiting time for different individuals are independent, and are independent with the number of children. In general, the waiting time is an exponential variable with parameter λ for all individuals, so that the process is Markovian.

Extinction problem for a Galton–Watson process

The ultimate extinction probability is given by

$\lim _{n\to \infty }\Pr(Z_{n}=0).$

For any nontrivial cases (trivial cases are ones in which the probability of having no offspring is zero for every member of the population - in such cases the probability of ultimate extinction is 0), the probability of ultimate extinction equals one if μ ≤ 1 and strictly less than one if μ > 1.

The process can be analyzed using the method of probability generating function. Let p₀, p₁, p₂, ... be the probabilities of producing 0, 1, 2, ... offspring by each individual in each generation. Let d_m be the extinction probability by the m^th generation. Obviously, d₀ = 0. Since the probabilities for all paths that lead to 0 by the m^th generation must be added up, the extinction probability is nondecreasing in generations. That is,

$0=d_{0}\leq d_{1}\leq d_{2}\leq \cdots \leq 1.$

Therefore, d_m converges to a limit d, and d is the ultimate extinction probability. If there are j offspring in the first generation, then to die out by the mth generation, each of these lines must die out in m − 1 generations. Since they proceed independently, the probability is (d_m−1) ^j. Thus,

$d_{m}=p_{0}+p_{1}d_{m-1}+p_{2}(d_{m-1})^{2}+p_{3}(d_{m-1})^{3}+\cdots .\,$

The right-hand side of the equation is a probability generating function. Let h(z) be the ordinary generating function for p_i:

$h(z)=p_{0}+p_{1}z+p_{2}z^{2}+\cdots .\,$

Using the generating function, the previous equation becomes

$d_{m}=h(d_{m-1}).\,$

Since d_m → d, d can be found by solving

$d=h(d).\,$

This is also equivalent to finding the intersection point(s) of lines y = z and y = h(z) for z ≥ 0. y = z is a straight line. y = h(z) is an increasing (since $h'(z)=p_{1}+2p_{2}z+3p_{3}z^{2}+\cdots \geq 0$) and convex (since $h''(z)=2p_{2}+6p_{3}z+12p_{4}z^{2}+\cdots \geq 0$) function. There are at most two intersection points. Since (1,1) is always an intersect point for the two functions, there only exist three cases:

Three cases of y = h(z) intersect with y = z.

Case 1 has another intersect point at z < 1 (see the red curve in the graph).

Case 2 has only one intersect point at z = 1.(See the green curve in the graph)

Case 3 has another intersect point at z > 1.(See the black curve in the graph)

In case 1, the ultimate extinction probability is strictly less than one. For case 2 and 3, the ultimate extinction probability equals to one.

By observing that h′(1) = p₁ + 2p₂ + 3p₃ + ... = μ is exactly the expected number of offspring a parent could produce, it can be concluded that for a branching process with generating function h(z) for the number of offspring of a given parent, if the mean number of offspring produced by a single parent is less than or equal to one, then the ultimate extinction probability is one. If the mean number of offspring produced by a single parent is greater than one, then the ultimate extinction probability is strictly less than one.

Size dependent branching processes

Along with discussion of a more general model of branching processes known as age-dependent branching processes by Grimmett, in which individuals live for more than one generation, Krishna Athreya has identified three distinctions between size-dependent branching processes which have general application. Athreya identifies the three classes of size-dependent branching processes as sub-critical, stable, and super-critical branching measures. For Athreya, the central parameters are crucial to control if sub-critical and super-critical unstable branching is to be avoided. Size dependent branching processes are also discussed under the topic of resource-dependent branching process

Example of extinction problem

Consider a parent can produce at most two offspring. The extinction probability in each generation is:

$d_{m}=p_{0}+p_{1}d_{m-1}+p_{2}(d_{m-1})^{2}.\,$

with d₀ = 0. For the ultimate extinction probability, we need to find d which satisfies d = p₀ + p₁d + p₂d².

Taking as example probabilities for the numbers of offspring produced p₀ = 0.1, p₁ = 0.6, and p₂ = 0.3, the extinction probability for the first 20 generations is as follows:

Generation # (1–10)	Extinction probability		Generation # (11–20)	Extinction probability
1	0.1		11	0.3156
2	0.163		12	0.3192
3	0.2058		13	0.3221
4	0.2362		14	0.3244
5	0.2584		15	0.3262
6	0.2751		16	0.3276
7	0.2878		17	0.3288
8	0.2975		18	0.3297
9	0.3051		19	0.3304
10	0.3109		20	0.331

In this example, we can solve algebraically that d = 1/3, and this is the value to which the extinction probability converges with increasing generations.

Simulating branching processes

Branching processes can be simulated for a range of problems. One specific use of simulated branching process is in the field of evolutionary biology. Phylogenetic trees, for example, can be simulated under several models, helping to develop and validate estimation methods as well as supporting hypothesis testing.

Multitype branching processes

In multitype branching processes, individuals are not identical, but can be classified into n types. After each time step, an individual of type i will produce individuals of different types, and $\mathbf {X} _{i}$, a random vector representing the numbers of children in different types, satisfies a probability distribution on $\mathbb {N} ^{n}$.

For example, consider the population of cancer stem cells (CSCs) and non-stem cancer cells (NSCCs). After each time interval, each CSC has probability $p_{1}$ to produce two CSCs (symmetric division), probability $p_{2}$ to produce one CSC and one NSCC (asymmetric division), probability $p_{3}$ to produce one CSC (stagnation), and probability $1-p_{1}-p_{2}-p_{3}$ to produce nothing (death); each NSCC has probability $p_{4}$ to produce two NSCCs (symmetric division), probability $p_{5}$ to produce one NSCC (stagnation), and probability $1-p_{4}-p_{5}$ to produce nothing (death).

Law of large numbers for multitype branching processes

For multitype branching processes that the populations of different types grow exponentially, the proportions of different types converge almost surely to a constant vector under some mild conditions. This is the strong law of large numbers for multitype branching processes.

For continuous-time cases, proportions of the population expectation satisfy an ODE system, which has a unique attracting fixed point. This fixed point is just the vector that the proportions converge to in the law of large numbers.

The monograph by Athreya and Ney summarizes a common set of conditions under which this law of large numbers is valid. Later there are some improvements through discarding different conditions.

Other branching processes

There are many other branching processes, for example, branching processes in random environments, in which the reproduction law is chosen randomly at each generation, or branching processes, where the growth of the population is controlled by external influences or interacting processes. Branching processes where particles have to work (contribute resources to the environment) in order to be able to reproduce, and live in a changing society structure controlling the distribution of resources, are so-called resource-dependent branching processes.

The scaling limit of near-critical branching processes can be used to obtain superprocesses.

See also

• Galton–Watson process
• Random tree
• Branching random walk
• Resource-dependent branching process
• Bruss–Duerinckx theorem
• Martingale (probability theory)
• Superprocess

References

• C. M. Grinstead and J. L. Snell, Introduction to Probability Archived 2011-07-27 at the Wayback Machine, 2nd ed. Section 10.3 discusses branching processes in detail together with the application of generating functions to study them.
• G. R. Grimmett and D. R. Stirzaker, Probability and Random Processes, 2nd ed., Clarendon Press, Oxford, 1992. Section 5.4 discusses the model of branching processes described above. Section 5.5 discusses a more general model of branching processes known as age-dependent branching processes, in which individuals live for more than one generation.