Stochastic population dynamics in a Markovian environment implies Taylor’s power law of fluctuation scaling

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Abstract

Taylor’s power law of fluctuation scaling (TL) states that for population density, population abundance, biomass density, biomass abundance, cell mass, protein copy number, or any other nonnegative-valued random variable in which the mean and the variance are positive, variance=a(mean)b,a>0, or equivalently log variance=loga+b×log mean. Many empirical examples and practical applications of TL are known, but understanding of TL’s origins and interpretations remains incomplete. We show here that, as time becomes large, TL arises from multiplicative population growth in which successive random factors are chosen by a Markov chain. We give exact formulas for a and b in terms of the Markov transition matrix and the values of the successive multiplicative factors. In this model, the mean and variance asymptotically increase exponentially if and only if b>2 and asymptotically decrease exponentially if and only if b<2.

Introduction

Fluctuation scaling is a name popular among physicists for a lawful relationship between the mean and variance of any random variable when the mean and variance are functions of some parameter. Among statisticians, such a relationship is often called a variance function. In population biology and ecology, Taylor’s power law of fluctuation scaling (Taylor, 1961, Taylor, 1984) states that when the mean and the variance exist and are positive functions of some parameter, they are related by a power law: variance=a(mean)b,a>0, or equivalently logvariance=loga+b×logmean.

Taylor’s law (TL) began with empirical observations of insect population densities and was verified in hundreds of biological species (Eisler et al., 2008) including, recently, bacteria (Ramsayer et al., 2011, Kaltz et al., 2012), trees (Cohen et al., 2012, Cohen et al., 2013a), and humans (Cohen et al., 2013b). TL is one of the most widely verified empirical relationships in ecology. TL has also been confirmed for cell populations within specific organs (Azevedo and Leroi, 2001), stem cell populations (Klein and Simons, 2011), counts of single nucleotide polymorphisms and genes (Kendal and Jørgensen, 2011), cases of measles and whooping cough (Keeling and Grenfell, 1999), the mass of single-celled organisms of different species (Giometto et al., 2013), and in diverse other fields (for additional references, see review by Eisler et al., 2008), including cancer metastases, single nucleotide polymorphisms and genes on chromosomes, and non-biological measurements such as precipitation, packet switching on the Internet, stock market trading, and number theory. TL has practical applications in the design of sampling plans for the control of insect pests (soybeans: Kogan et al., 1974, Bechinski and Pedigo, 1981; cotton: Wilson et al., 1989; glasshouse roses: Park and Cho, 2004).

There is little consensus about why TL is so widely observed and how its estimated parameters should be interpreted. The theoretical analysis of probability distributions in which the variance is a power-law function of the mean preceded TL (Tweedie, 1946, Tweedie, 1947) (in other words, Taylor did not invent Taylor’s law) and TL has been much studied theoretically with or without recognition of its empirical roots in ecology (e.g., Anderson et al., 1982, Tweedie, 1984, Perry and Taylor, 1985, Gillis et al., 1986, Jørgensen, 1987, Kemp, 1987, Perry, 1988, Lepš, 1993, Jørgensen, 1997, Keeling, 2000, Azevedo and Leroi, 2001, Kilpatrick and Ives, 2003, Kendal, 2004, Ballantyne and Kerkhoff, 2007, Eisler et al., 2008, Engen et al., 2008, Kendal and Jørgensen, 2011, Cohen et al., 2013a). Davidian and Carroll (1987) and Wang and Zhao (2007) emphasized the importance of modeling correctly how the variance is related to the mean if one desires statistical efficiency in estimating the mean. They considered multiple variance functions including TL. But they did not identify a power-law variance function with TL or discuss models that might explain the origin of these variance functions.

Cohen et al. (2013a) showed that the Lewontin and Cohen (1969) (no relation to the present author) stochastic multiplicative population model (a geometric random walk with independently and identically distributed [i.i.d.] multiplicative increments) implies TL. Cohen et al. (2013a) calculated loga and b explicitly. Here we consider a more general model in which the factors that multiply the population density at each time step are history-dependent, not independent as in the Lewontin–Cohen model. We show that a multiplicative model of change in a Markovian environment leads to TL in the limit of large time, and we calculate loga and bexplicitly.

Section snippets

Taylor’s law

Let a family of nonnegative random variables N(t) be parameterized by tΘ, where Θ is an index set. Assume that, for all tΘ, the mean E(N(t)) and the variance V ar(N(t)) are finite and positive, so logV ar(N(t)) and logE(N(t)) are well defined. We may think of N(t) as population density at time t.

Definition

TL applies to N(t) exactly for all tΘ if and only if there exist real constants a>0 and b such that, for all tΘ,V ar(N(t))=a(E(N(t)))b. Equivalently, TL applies to N(t) exactly for all tΘ if and

Scalar discrete-time Markovian multiplicative growth

Assume N(0) is a fixed positive number. Suppose that N(t)=A(t1)A(t2)A(0)N(0),t=0,1,2,.

Then A(t1)=N(t)/N(t1),t=1,2, represents the random factor of change from time t1 to time t. Assume that each value of A(t) is taken from a finite set of positive numbers {d1,,ds},s>1, at least two of which are distinct. Intuitively, s is the number of states of the environment. By assumption, each state of the environment determines a multiplicative factor of change: if A(t1)=di, then N(t)=diN(t1),

Branching processes and birth-and-death processes

Taylor’s power law of fluctuation applies asymptotically to other Markovian population processes in addition to the example just studied.

First, the discrete-generation Galton–Watson branching process (Bartlett, 1955, 1966, Section 2.3, Eq. (3), p. 40 in 1955, p. 42 in 1966) assumes that each individual of the tth generation independently has a stochastically distributed number of offspring in the next generation. If the initial number of individuals is m0>0, and the mean and variance of the

Multiple models lead to Taylor’s law

A wide range of models can yield TL exactly or in the limit of large time. For example, a deterministic model of exponential clonal growth (Cohen, 2013a, Cohen et al., 2013b), the Galton–Watson branching process (with v=0 or m>1), and the birth and death process (with λ>μ) all converge (for large time) to TL with b=2. The gamma distribution satisfies TL exactly with b=2. Hence b=2 in TL need not indicate deterministic population growth. Both the model of Lewontin and Cohen (1969) with i.i.d.

Acknowledgments

I thank Lee Altenberg (as colleague and self-identified reviewer), Roy Malka, Michael Plank, Shripad Tuljapurkar, Meng Xu, and an anonymous reviewer for very helpful comments, Priscilla K. Rogerson for assistance, Michael Plank and the family of William T. Golden for hospitality during this work, and the US National Science Foundation grants EF-1038337 and DMS-1225529 and the Marsden Fund of the Royal Society of New Zealand (08-UOC-034) for partial support.

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