Populations with interaction and environmental dependence: From few, (almost) independent, members into deterministic evolution of high densities

Pavel Chigansky, Peter Jagers, Fima C. Klebaner

Research output: Contribution to journalArticleResearchpeer-review

Abstract

Many populations, e.g. not only of cells, bacteria, viruses, or replicating DNA molecules, but also of species invading a habitat, or physical systems of elements generating new elements, start small, from a few lndividuals, and grow large into a noticeable fraction of the environmental carrying capacity K or some corresponding regulating or system scale unit. Typically, the elements of the initiating, sparse set will not be hampering each other and their number will grow from Z 0 = z 0 in a branching process or Malthusian like, roughly exponential fashion, Z t ~a t W, where Z t is the size at discrete time t → ∞, a > 1 is the offspring mean per individual (at the low starting density of elements, and large K), and W a sum of z 0 i.i.d. random variables. It will, thus, become detectable (i.e. of the same order as K) only after around K generations, when its density X t := Z t /K will tend to be strictly positive. Typically, this entity will be random, even if the very beginning was not at all stochastic, as indicated by lower case z 0 , due to variations during the early development. However, from that time onwards, law of large numbers effects will render the process deterministic, though inititiated by the random density at time log K, expressed through the variable W. Thus, W acts both as a random veil concealing the start and a stochastic initial value for later, deterministic population density development. We make such arguments precise, studying general density and also system-size dependent, processes, as K → ∞. As an intrinsic size parameter, K may also be chosen to be the time unit. The fundamental ideas are to couple the initial system to a branching process and to show that late densities develop very much like iterates of a conditional expectation operator. The “random veil”, hiding the start, was first observed in the very concrete special case of finding the initial copy number in quantitative PCR under Michaelis-Menten enzyme kinetics, where the initial individual replication variance is nil if and only if the efficiency is one, i.e. all molecules replicate.

Original languageEnglish
Pages (from-to)108-118
Number of pages11
JournalStochastic Models
Volume35
Issue number2
DOIs
Publication statusPublished - 2019

Keywords

  • Branching processes
  • carrying capacity
  • density dependence
  • population dynamics
  • threshold size

Cite this

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title = "Populations with interaction and environmental dependence: From few, (almost) independent, members into deterministic evolution of high densities",
abstract = "Many populations, e.g. not only of cells, bacteria, viruses, or replicating DNA molecules, but also of species invading a habitat, or physical systems of elements generating new elements, start small, from a few lndividuals, and grow large into a noticeable fraction of the environmental carrying capacity K or some corresponding regulating or system scale unit. Typically, the elements of the initiating, sparse set will not be hampering each other and their number will grow from Z 0 = z 0 in a branching process or Malthusian like, roughly exponential fashion, Z t ~a t W, where Z t is the size at discrete time t → ∞, a > 1 is the offspring mean per individual (at the low starting density of elements, and large K), and W a sum of z 0 i.i.d. random variables. It will, thus, become detectable (i.e. of the same order as K) only after around K generations, when its density X t := Z t /K will tend to be strictly positive. Typically, this entity will be random, even if the very beginning was not at all stochastic, as indicated by lower case z 0 , due to variations during the early development. However, from that time onwards, law of large numbers effects will render the process deterministic, though inititiated by the random density at time log K, expressed through the variable W. Thus, W acts both as a random veil concealing the start and a stochastic initial value for later, deterministic population density development. We make such arguments precise, studying general density and also system-size dependent, processes, as K → ∞. As an intrinsic size parameter, K may also be chosen to be the time unit. The fundamental ideas are to couple the initial system to a branching process and to show that late densities develop very much like iterates of a conditional expectation operator. The “random veil”, hiding the start, was first observed in the very concrete special case of finding the initial copy number in quantitative PCR under Michaelis-Menten enzyme kinetics, where the initial individual replication variance is nil if and only if the efficiency is one, i.e. all molecules replicate.",
keywords = "Branching processes, carrying capacity, density dependence, population dynamics, threshold size",
author = "Pavel Chigansky and Peter Jagers and Klebaner, {Fima C.}",
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Populations with interaction and environmental dependence : From few, (almost) independent, members into deterministic evolution of high densities. / Chigansky, Pavel; Jagers, Peter; Klebaner, Fima C.

In: Stochastic Models, Vol. 35, No. 2, 2019, p. 108-118.

Research output: Contribution to journalArticleResearchpeer-review

TY - JOUR

T1 - Populations with interaction and environmental dependence

T2 - From few, (almost) independent, members into deterministic evolution of high densities

AU - Chigansky, Pavel

AU - Jagers, Peter

AU - Klebaner, Fima C.

PY - 2019

Y1 - 2019

N2 - Many populations, e.g. not only of cells, bacteria, viruses, or replicating DNA molecules, but also of species invading a habitat, or physical systems of elements generating new elements, start small, from a few lndividuals, and grow large into a noticeable fraction of the environmental carrying capacity K or some corresponding regulating or system scale unit. Typically, the elements of the initiating, sparse set will not be hampering each other and their number will grow from Z 0 = z 0 in a branching process or Malthusian like, roughly exponential fashion, Z t ~a t W, where Z t is the size at discrete time t → ∞, a > 1 is the offspring mean per individual (at the low starting density of elements, and large K), and W a sum of z 0 i.i.d. random variables. It will, thus, become detectable (i.e. of the same order as K) only after around K generations, when its density X t := Z t /K will tend to be strictly positive. Typically, this entity will be random, even if the very beginning was not at all stochastic, as indicated by lower case z 0 , due to variations during the early development. However, from that time onwards, law of large numbers effects will render the process deterministic, though inititiated by the random density at time log K, expressed through the variable W. Thus, W acts both as a random veil concealing the start and a stochastic initial value for later, deterministic population density development. We make such arguments precise, studying general density and also system-size dependent, processes, as K → ∞. As an intrinsic size parameter, K may also be chosen to be the time unit. The fundamental ideas are to couple the initial system to a branching process and to show that late densities develop very much like iterates of a conditional expectation operator. The “random veil”, hiding the start, was first observed in the very concrete special case of finding the initial copy number in quantitative PCR under Michaelis-Menten enzyme kinetics, where the initial individual replication variance is nil if and only if the efficiency is one, i.e. all molecules replicate.

AB - Many populations, e.g. not only of cells, bacteria, viruses, or replicating DNA molecules, but also of species invading a habitat, or physical systems of elements generating new elements, start small, from a few lndividuals, and grow large into a noticeable fraction of the environmental carrying capacity K or some corresponding regulating or system scale unit. Typically, the elements of the initiating, sparse set will not be hampering each other and their number will grow from Z 0 = z 0 in a branching process or Malthusian like, roughly exponential fashion, Z t ~a t W, where Z t is the size at discrete time t → ∞, a > 1 is the offspring mean per individual (at the low starting density of elements, and large K), and W a sum of z 0 i.i.d. random variables. It will, thus, become detectable (i.e. of the same order as K) only after around K generations, when its density X t := Z t /K will tend to be strictly positive. Typically, this entity will be random, even if the very beginning was not at all stochastic, as indicated by lower case z 0 , due to variations during the early development. However, from that time onwards, law of large numbers effects will render the process deterministic, though inititiated by the random density at time log K, expressed through the variable W. Thus, W acts both as a random veil concealing the start and a stochastic initial value for later, deterministic population density development. We make such arguments precise, studying general density and also system-size dependent, processes, as K → ∞. As an intrinsic size parameter, K may also be chosen to be the time unit. The fundamental ideas are to couple the initial system to a branching process and to show that late densities develop very much like iterates of a conditional expectation operator. The “random veil”, hiding the start, was first observed in the very concrete special case of finding the initial copy number in quantitative PCR under Michaelis-Menten enzyme kinetics, where the initial individual replication variance is nil if and only if the efficiency is one, i.e. all molecules replicate.

KW - Branching processes

KW - carrying capacity

KW - density dependence

KW - population dynamics

KW - threshold size

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