Branching processes in correlated random environment
Xinxin Chen (PSPM), Nadine Guillotin-Plantard (ICJ)

TL;DR
This paper investigates the survival probabilities and tail behaviors of critical branching processes in correlated random environments, especially those modeled by fractional Brownian motion, revealing new insights into their probabilistic properties.
Contribution
It introduces analysis of critical branching processes in correlated environments, including fractional Brownian motion, providing new estimates for survival probabilities and tail distributions.
Findings
Survival probability estimates for processes in correlated environments.
Tail behavior of progeny and width in fractional Brownian motion environments.
Extension of classical branching process results to correlated settings.
Abstract
We consider the critical branching processes in correlated random environment which is positively associated and study the probability of survival up to the n-th generation. Moreover, when the environment is given by fractional Brownian motion, we estimate also the tail of progeny as well as the tail of width.
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Taxonomy
TopicsStochastic processes and statistical mechanics · Complex Systems and Time Series Analysis · Theoretical and Computational Physics
Branching processes in correlated random environment
XINXIN CHEN111Institut Camille Jordan - C.N.R.S. UMR 5208 - Université Claude Bernard Lyon 1 (France).
Institut Camille Jordan - C.N.R.S. UMR 5208 - Université Claude Bernard Lyon 1 (France).
MSC 2000 60J80 60K37 60G15. Supported by ANR MALIN ANR-16-CE93-0003
Key words : branching process, correlated random environment , NADINE GUILLOTIN-PLANTARD*†*
We consider the critical branching processes in correlated random environment which is positively associated and study the probability of survival up to the -th generation. Moreover, when the environment is given by fractional Brownian motion, we estimate also the tail of progeny as well as the tail of width.
1 Introduction and results
In the theory of branching process, branching processes in random environment (BPRE), as an important part, was introduced by Smith and Wilkinson [10] by supposing that the environment is i.i.d.. This model has been well investigated by lots of authors. One can refer to [1],[2],[3] for various properties obtained in this setting. In fact, for this so called Smith-Wilkinson model, the behaviour of BPRE depends largely on the behaviour of the corresponding random walk constructed by the logarithms of the quenched expectation of population sizes. As this random walk is of i.i.d. increments due to i.i.d. environment, many questions on this model become quite clear.
However, we are interested in branching processes in correlated random environment. More precisely, we consider the Athreya-Karlin model of BPRE where the environment is assumed to be stationary and ergodic; and moreover correlated.
Let us introduce some notations. Consider a branching process in random environment given by a sequence of random generating functions . Given the environment, individuals reproduce independently of each other. The offspring of an individual in the n-th generation has generating function . If denotes the number of individuals in the n-th generation, then under the quenched probability (and the quenched expectation ),
[TABLE]
We will assume that . Here the random environment is supposed to be stationary, ergodic and correlated. The process will be called a branching process in correlated environment (BPCE, for short).
First of all, the criterion for the process to be subcritical, critical or supercritical was proven by Tanny [11]. In this paper, we only consider the non-sterile critical case, i.e.
[TABLE]
where is the annealed expectation.
We are interested in some important quantities related to this branching process, such as the tail distribution of its extinction time , of its maximum population and of its total population size:
[TABLE]
Let us mention that this problem was considered in [5] in the case where the offspring sizes are geometrically distributed, using the well-known correspondence between recurrent random walks in random environment and critical branching processes in random environment with geometric distribution of offspring sizes. Our aim is to generalise the results obtained in [5] to more general generating functions .
More precisely let for every . Assume that is a stationary, ergodic and centered sequence and define the sequence ()
[TABLE]
We also assume that the scaling limit of is a stochastic process :
[TABLE]
where and is a slowly varying function at infinity such that as
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We will also assume that the tail distribution of the random variable decreases sufficiently fast, namely there exist and such that
[TABLE]
Let us recall that a collection of random variables defined on a same probability space is said quasi-associated provided that
[TABLE]
for any and all coordinatewise nondecreasing, measurable functions and . We will say that is positively associated if
[TABLE]
for all coordinatewise nondecreasing, measurable functions . We refer to [6] for details concerning positively associated random variables. Clearly positive association is a stronger assumption than quasi-association. A sequence of random variables is said positively associated (resp. quasi-associated) if for every , the set is positively associated (resp. quasi-associated).
For every , we denote by the variance of the probability distribution with generating function . Remark that . Our main assumption concerning the sequence is the following one:
There exist positive constants and such that for every ,
[TABLE]
Remark that the assumption is satisfied for the classical discrete probability distributions such as the Poisson distribution, the Geometric distribution, the uniform distribution, the Binomial distribution etc.
In this setup we obtain the following theorem.
Theorem 1**.**
Assume that the sequence is positively associated. Under assumption , there exist positive constants such that for large enough ,
[TABLE]
Remark 2**.**
Actually we will prove that the upper bound holds for every . This is due to the fact that we use strong results on the persistence of the random walk namely Theorem 11 in [4].
From now on we will assume that is a standard Gaussian sequence with positive correlations satisfying as ,
[TABLE]
where and is a slowly varying function at infinity. In that case the process is the fractional Brownian motion with Hurst parameter (see [13], [14, Theorem 4.6.1]). Recall that is the real centered Gaussian process with covariance function
[TABLE]
When , the sequence is positively associated as positively correlated Gaussian random variables.
Theorem 3**.**
Under assumption , there exists a function that is slowly varying at infinity such that for large enough
[TABLE]
Note that
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As a consequence,
[TABLE]
so Theorems 1 and 3 lead to the following result.
Theorem 4**.**
Under assumption , there exists a function that is slowly varying at infinity such that for large enough
[TABLE]
2 Extinction time: Proof of Theorem 1
2.1 Upper bound
Observe that for any ,
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Then,
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as . Let us bound for . Let . Note that for every ,
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by quasi-association of . Note that by stationarity, we have
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On the other hand, by positive association,
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So,
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Let us prove that the sequence satisfies the hypotheses of Theorems 2 and 4 in [4]. Due to the convergence in law of to as goes to infinity, we can show that for any fixed, converges in distribution to as goes to infinity (see Section 12.3 in [14]). Let us prove that is uniformly integrable. To this end we will use the fact that the increments of are centered and positively associated. Due to Theorem 2.1 of [8], there exists some constant such that
[TABLE]
The uniform integrability of follows from assumption (1.3), and then as goes to infinity. From Theorem 4 in [4], there exists such that for every ,
[TABLE]
Moreover, if we choose , the probability converges to . So, we get that (here are two positive constants) for large and for any
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where is a slowly varying function at infinity. Then, from the upper bound in Theorem 2 in [4], we get that for large and for any ,
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Plugging this into (2.1) implies that there exists such that for every ,
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2.2 Lower bound
Note that (see (2.1) in [7])
[TABLE]
It is known in [7] that
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where
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with
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From Lemma 2.1 in [7],
[TABLE]
This yields that
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where .
Let us take with so that
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is bounded by where are positive constants. It follows that
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By the fact that the increments of the sequence are positively associated, one sees that
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Let where with and any so that for large enough
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Consequently, by (1.4), for some and ,
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Take a_{n}=\big{(}\frac{1}{c_{7}}\log(2\alpha_{n}))^{1/\alpha} such that
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Now by remarking that converges to and by applying Theorem 4 in [4], there exists some constant such that for large enough
[TABLE]
3 Maximal population and total population
3.1 Proof of Theorem 3
Let be the first passage time of the sequence above/below the level
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3.2 Upper bound
Let us define for every , the random variable
[TABLE]
It is well-known that is a martingale under the quenched probability. Note that for every ,
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Observe that
[TABLE]
First, from the upper bound in Theorem 1, there exists some constant such that for large ( will be chosen later)
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On the other hand, let ,
[TABLE]
Since is a martingale under the quenched distribution , we get
[TABLE]
By observing that , the second probability in (3.2) is bounded from above by
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which is equal, by symmetry of Gaussian variables, to . Applying the maximal inequality in Proposition 2.2 in [9] implies that
[TABLE]
where is the variance of by (1.5).
Let us choose with . Then,
[TABLE]
The upper bound follows by gathering , and .
3.3 Lower bound
On the other hand, for the lower bound, we take and for certain . Then,
[TABLE]
We will take so that and obtain by Paley-Zygmund inequality that
[TABLE]
As is a martingale, the following equality holds
[TABLE]
where and . It follows that
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Thus,
[TABLE]
It is enough to bound from below the following expectation (since )
[TABLE]
Let . Let us consider the set defined by:
[TABLE]
with
[TABLE]
where with determined in (3.9). The lower bound will follow from the following lemma.
Lemma 5**.**
There exists a function that is slowly varying at infinity such that for large ,
[TABLE]
Indeed,
[TABLE]
where is a function slowly varying at infinity.
The proof of Lemma 5 rests on the two following lemma.
Lemma 6**.**
There exists a function slowly varying at infinity such that for large ,
[TABLE]
Lemma 7**.**
[TABLE]
Proof of Lemma 5.
Note that, by Lemma 7, there exists such that for every ,
[TABLE]
Due to Lemma 6, for large ,
[TABLE]
since the probability of the set \big{(}\mathcal{G}_{N}^{(2)}\big{)}^{c} is of a lower order by (3.5). ∎
Proof of Lemma 6.
(see Step 1 in the proof of Lemma 9 in [5]) Let with and L:=L_{N}:=\big{\lfloor}(\log\log N)^{\frac{q}{2H}}\big{\rfloor}, with and . Then,
[TABLE]
We show that the last term in (3.3) is not relevant since it is bounded from above by the probability
[TABLE]
using inequality (35) in [5]. For the first term in (3.3), observe that
[TABLE]
where are defined in the proof of the lower bound in Theorem 1 (see Section 2). On the set inside the previous probability (Remark that for large , and that we take ):
[TABLE]
Using techniques developed in the proof of the lower bound in Theorem 1, the probability (3.8) is bounded from below by
[TABLE]
for large enough. ∎
Proof of Lemma 7.
[TABLE]
by applying Theorem 11 of [4]. ∎
The reference list from the paper itself. Each links out to its DOI / PubMed record.
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