Deviation inequalities for separately Lipschitz functionals of composition of random functions
J\'er\^ome Dedecker, Paul Doukhan, Xiequan Fan

TL;DR
This paper develops deviation and moment inequalities for separately Lipschitz functions of non-homogeneous Markov chains, broadening the understanding of their probabilistic behavior under certain moment conditions.
Contribution
It introduces new deviation inequalities for Lipschitz functionals of non-homogeneous Markov chains using martingale techniques, applicable to a wide class of models.
Findings
Established deviation inequalities under moment conditions
Applied martingale methods to non-homogeneous Markov chains
Extended results to a broad class of natural examples
Abstract
We consider a class of non-homogeneous Markov chains, that contains many natural examples. Next, using martingale methods, we establish some deviation and moment inequalities for separately Lipschitz functions of such a chain, under moment conditions on some dominating random variables.
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Deviation inequalities
for separately Lipschitz functionals of composition of random functions
Jérôme Dedecker,111Université Paris Descartes, Sorbonne Paris Cité, Laboratoire MAP5 and CNRS UMR 8145, 75016 Paris, France. E-mail: [email protected]: 1 Paul Doukhan222AGM UMR 8088, Université Paris Seine, UCP site Saint-Martin, 2 Bd. Adolphe Chauvin 95000 Cergy-Pontoise, France, and CIMFAV, Universidad de Valparaiso, Chile. Email: [email protected]: 2 and Xiequan Fan333Center for Applied Mathematics, Tianjin University, Tianjin, China. E-mail: [email protected]: 3 444All authors contributed equally to this work
Abstract
We consider a class of non-homogeneous Markov chains, that contains many natural examples. Next, using martingale methods, we establish some deviation and moment inequalities for separately Lipschitz functions of such a chain, under moment conditions on some dominating random variables.
Keywords: Non-homogeneous Markov chains, martingales, exponential inequalities, moment inequalities.
Mathematics Subject Classification (2010): 60G42, 60J05, 60E15.
1 Introduction
Concentration inequalities are essential tools for ensuring the validity of many statistical procedures; let us cite for instance [18] for classification problems, [21] for model selection, and [3] for high dimensional procedures (see also [2] and [33] in a dependent framework).
These inequalities are not easy to prove in a dependent context; up to now this has been done under quite restrictive assumptions, and mainly for bounded functionals of the variables in a stationary/homogeneous context. As a non exhaustive list, let us quote [31], [27], [12], [1], [10] and [11]. Among these references, the case of unbounded functionals has been investigated in [1] for geometrically ergodic Markov chains, and in [10] for iterated random functions satisfying a mean-contraction condition (see condition (2.8) below, with ).
In the paper [10], the authors obtained very precise inequalities for Lipschitz functionals of the chain, by assuming moreover a Lipschitz condition on the function that generates the chain (see condition (2.9) below). However, this last condition is in fact quite restrictive, and does not hold for many natural models satisfying the mean-contraction property.
In the present paper we enlarge the class of Markov chains studied in [10], by considering non-homogeneous Markov chains obtained through composition of random functions (see the recursive mechanism (2.7) below), and by making no extra assumptions than the (uniform) mean-contraction (2.8). As in [10], we shall use the decomposition of the functional of the chain in terms of martingale differences, as first introduced by Yurinskii [32]. This method is well adapted to the non-homogeneous Markov context, because it is intrinsically a non-stationary method. Following this approach, we obtain deviation and moment inequalities for separately Lipschitz functionals of the chain that are driven by the distribution of some dominating random variables.
The present article was conceived within the general framework of non stationary time series, which is now widely discussed in the context global warming [6]. Besides temperatures or ozone concentration, most of the real life phenomena present trends and periodicities. A first excellent view of those questions may be found in [5], but this is a linear view of time series analysis. It appears important to consider cases where the dynamic of the models itself is non time-homogeneous. For instance [8] and [4] provide different views for a more relevant dynamical approach including local stationarity and non-periodic features. The present paper aims at developing reasonable concentration and probability inequalities for non-homogeneous Markov chains able to model some of the above features.
Before going into further details, let us give a simple class of examples to which our results apply. We consider a generalized -valued auto-regressive processes
[TABLE]
where is a random matrix and is an -valued random variable. Here are independent random variables, and is independent of the initial random variable . Let be a norm on . Then, the Markov chain satisfies the mean contraction condition (2.8) for the norm as soon as
[TABLE]
where as usual .
Model (1.1) contains a lot of natural examples (see for instance [9], Sections 2.2 and 2.3), but does not fit within the framework of [10]; moreover, it has no reason to be mixing in the sense of Rosenblatt [30] without further assumptions on the distribution of . Recall that the chain is non-homegeneous, since we do not assume here that the variables are iid.
Let now be a separately Lipschitz function, such that
[TABLE]
and let also .
For simplicity, let us consider the case where the chain starts at . Assuming that and for any and some , we infer from (2.11) (control of the -norm of the dominating variables defined in (2.10)) and Propositions 5.1 and 5.3 that
[TABLE]
and
[TABLE]
for some constant depending only on . These inequalities are satisfactory, because if for (case ), we recover for the usual Marcinkiewicz-Zygmund inequalities (see [28]) for -norms of sums of independent random variables, and for the usual von Bahr-Esseen inequalities (see [26]). Note that, under the stronger condition than (1.2): (-contraction), and if , we obtain that if and if , which is exactly what we could expect for -norms of partial sums in a quasi-stationary regime.
Under more restrictive conditions on , one can also obtain some semi-exponential bounds for the deviation of . For the sake of simplicity, let us assume that (uniform contraction) and that there exist such that
[TABLE]
It is then easy to see that dominating variables defined in (2.10) also satisfy the uniform bound (1.4) (for the same and a different , say ). Hence, it follows from Proposition 4.2 that
[TABLE]
for any , where the positive constant depends only on , and
[TABLE]
In particular, we obtain from (1.5) the following moderate deviation behavior: for any , there exist such that
[TABLE]
Note that, for , this is in accordance with the best possible rate for large deviation of sums of martingale differences (see Theorem 2.1 in [15]).
2 Composition of random functions
Let be a probability space. Let and be two complete separable metric spaces. Let be a sequence of independent -valued random variables. Let be a -valued random variable independent of . We consider the Markov chain such that
[TABLE]
where is such that
[TABLE]
for some constant not depending on .
In the paper [10], the authors studied a class of homogeneous Markov chains (that is, with and a sequence of i.i.d. random variables) satisfying (2.8) and the condition
[TABLE]
for some positive constant . Under this additional constraint, they obtained very precise upper bounds for the deviation of separately Lipschitz functionals of the chain; this is possible, because in that case, the martingales differences from McDiarmid’s decomposition are bounded by a function of , which is then independent of the past -field of the chain.
However, condition (2.9) is quite restrictive, and is not satisfied for many natural models (a short list of such models is presented below). In the present paper, we shall not assume that (2.9) is satisfied. In this more general setting, the dominating random variables are
[TABLE]
(see Proposition 3.1 below). The main difference with [10] is that these dominating random variables are no longer independent from the past -field of the chain. Hence, the deviations bounds that we obtain are not as precise as in [10], but apply to a much larger class of (non homogeneous) Markov chains.
Remark 2.1*.*
Note that if (2.8) holds for the distance , then, for any , it also hold for the distance with instead of . This is elementary, but nevertheless important: it means that we can also obtain concentration inequalities for separately Lipschitz functions with respect to by controlling the behavior of (whose definition is as in (2.10) for the distance ). Note that separately Lipschitz functions with respect to are less and less regular as approaches 0.
Remark 2.2*.*
Let us quote an error in the paper [10]. The inequality (1.4) of that paper gives an upper bound for the quantity when is any increasing function from to . However this upper bound is not true in general under the assumption (1.2) of [10] (which is similar to our assumption (2.8)), but it holds under the much more restrictive assumption . The error comes from the fact that the first version of the paper [10] was written under this more restrictive assumption. Note that this wrong inequality was not used at any points in the proofs of the main results in [10], but only in Items 4 of Remarks 3.1 and 3.2 (which are therefore not correct).
2.1 Examples
In this subsection, we give a non exhaustive list of models satisfying condition (2.8), and we show how to control the moments of the dominating variables defined by (2.10). For the sake of simplicity, we shall only deal with the moments of order of , but similar computations may be done for exponential moments. We refer to [13] and [8] for more examples.
- •
ARCH-type models. For which
[TABLE]
Thus the non stationarity appears simply from changes in the parameter . In that case (2.8) is satisfied for provided for some .
For these models
[TABLE]
and the moments of order of satisfy
[TABLE]
Those models are easy to extend in an -valued framework. For instance, one can consider , where is a matrix and are -valued random variables. Let be a norm on , and be the associated matrix norm. Now, if , then the condition (2.8) is satisfied as soon as for some .
- •
Switching models. Many analogous models can be provided with a switching, e.g. for the first ARCH-model, such a parametric model is given with , , a parameter and
[TABLE]
Here is a sequence of independent random variables with values in . Using the notation , we see that condition (2.8) is satisfied as soon as
[TABLE]
for some .
Now, similar computations as for the first example lead to
[TABLE]
- •
Generalized -valued auto-regressive processes. We consider here the Model (1.1) presented in the introduction. Recall that is a random matrix and is an -valued random variable. Here are independent random variables, and is independent of the initial random variable . Model (1.1) is a composition of random functions as in (2.7), with
[TABLE]
Let be a norm on , and let as usual . The condition (2.8) is satisfied as soon as (1.2) holds.
For these models
[TABLE]
and the moments of order of satisfy
[TABLE]
- •
INAR() type models. In this case, let and , where is a sequence of i.i.d. integer valued random variables. The function is then given by
[TABLE]
Here, is an i.i.d. sequence distributed as . It is then easy to see that (2.8) is satisfied provided .
We shall now give some hints to control the moments of the dominating random variables . Let be distributed as and independent of . We then have that
[TABLE]
For the INAR(1) model, we have
[TABLE]
By contraction, we get that
[TABLE]
For , applying the Marcinkiewicz-Zygmund inequality given in [28], we get that
[TABLE]
For , applying the von-Bahr Essen inequality given in [26], we get that
[TABLE]
Note that non-stationary variants of this model can be obtained by considering independent (but non i.i.d.) ’s, with the constraint: .
- •
GLM-Poisson models. Besides the standard ARCH-models the simplest case is that of Poisson ARCH–models, where is a sequence of i.i.d. unit Poisson processes. Consider a sequence of functions and set
[TABLE]
where denotes a function. In that case, the condition (2.8) is satisfied if for any , any , and some .
For these models,
[TABLE]
where is a unit Poisson process independent of . By contraction, we get that
[TABLE]
where . Note that, when is an integer, denotes the Stirling polynomial defined through Stirling numbers (see the Lemma A-1 in [13] from [17]).
- •
GLM–GARCH Poisson models. One can give numerous extensions of the previous model. Keeping the same notations, one can consider , and
[TABLE]
where . Let . Then
[TABLE]
and (2.8) is true provided that and for some .
For these models,
[TABLE]
where is a unit Poisson process independent of . Hence, the moments of order of can be controlled exactly as in the previous example.
3 Separately Lipschitz functions of
Let be a separately Lipschitz function, such that
[TABLE]
Let
[TABLE]
We introduce the natural filtration of the chain, that is and for all , . Define
[TABLE]
and
[TABLE]
For all , let
[TABLE]
and notice that, by the definition of ’s, the functional introduced in (3.2) satisfies
[TABLE]
Thus is a martingale adapted to the natural filtration . This representation appears in Yurinskii [32] and in p. 33 of the monograph by Milman and Schechtman [24]. In the setting of separately Lipschitz functions of independent random variables (i.e. when ) it has been used by McDiarmid [23] to get an exponential bound on tail probabilities .
The following Proposition, similar to Proposition 2.1 in [10], collects some interesting properties of the function and of the martingale difference .
Proposition 3.1**.**
For all and any in , denote . Let be a Markov chain satisfying (2.7) for some functions satisfying (2.8). Let and be defined by (3.3) and (3.4) respectively.
The function is separately Lipschitz, and satisfies
[TABLE] 2. 2.
Denote by and the distribution of and the distribution of respectively. Let and be two functions defined as follows
[TABLE]
Then, the martingale difference satisfies
[TABLE]
Remark 3.1*.*
Assume moreover that satisfies
[TABLE]
for some function not depending on , and let be the function defined by
[TABLE]
Then and, consequently,
[TABLE]
Note that (3.5) is a non-uniform version of (2.9), which is satisfied for many examples (for instance the three first examples of Section 2). However, it seems quite difficult to check for INAR or GLM type models, while the moments of the dominating variables are easy to control for such models (see Section 2).
Proof. The first point will be proved by recurrence in the backward sense. For the result is obvious due to . Suppose it is true at step , and let us prove it at step . By definition
[TABLE]
Then it is easy to see that
[TABLE]
Now, by assumption and condition (2.8),
[TABLE]
The point 1 follows from (3.6) and (3.7).
Next, we prove the point 2. First notice that
[TABLE]
Similarly, for all ,
[TABLE]
This completes the proof of Proposition 3.1. ∎
4 Deviation inequalities for the functional
Let be a Markov chain satisfying (2.7) for some functions satisfying (2.8). In this section, we apply inequalities for martingales to bound up the deviation of the functional defined by (3.2). Some of these inequalities are direct applications of known inequalities, and some deserve a short proof.
Denote by , and let be a sequence of positive numbers. Then, for any ,
[TABLE]
and note that the same bound is valid for by replacing the term by .
The term will be most of the time negligible, and represents the direct influence of the initial distribution of the chain. For instance, when the chain starts from a point , then and The main difficulty is to give an upper bound for , which is the purpose of the present paper.
4.1 A first exponential bound
Under a sub-Gaussian type condition, we obtain the following proposition.
Proposition 4.1**.**
Assume that there exists a positive constant such that, for any integer ,
[TABLE]
Then, for any ,
[TABLE]
where
[TABLE]
Remark 4.1*.*
Let us give some comments on Proposition 4.1.
Condition (4.2) is in fact a sub-Gaussian condition. On can check that it is satisfied provided
[TABLE]
and
[TABLE]
for some positive constant not depending on . 2. 2.
Assume that
[TABLE]
for some positive constant , and that
[TABLE]
Then, it follows from Proposition 4.1 that
[TABLE]
for some positive constant .
Proof. By Taylor’s expansion of and the fact that , we have, for all
[TABLE]
Using Rio’s inequality (see Theorem 2.1 of [28]): for any
[TABLE]
we get, for all
[TABLE]
Hence, by Hölder’s inequality, inequality (4.8) implies that, for all
[TABLE]
Applying the last inequality to (4.6), we obtain
[TABLE]
By points 2 of Proposition 3.1 and (4.2), we deduce that, for any integer ,
[TABLE]
Hence condition (4.2) implies that, for all ,
[TABLE]
By the inequality it follows that, for all ,
[TABLE]
Applying Markov’s inequality, it is then easy to see that, for all and
[TABLE]
Hence
[TABLE]
which gives (4.3). Using the inequality we get (4.4) from (4.3). ∎
4.2 Semi-exponential bounds
In the case where the variables have semi-exponential moments, the following proposition holds.
Proposition 4.2**.**
Let . Assume that there exists a constant such that, for any integer ,
[TABLE]
Then, for any ,
[TABLE]
where
[TABLE]
depends on only through the term .
Remark 4.2*.*
Let us comment on inequality (4.13). Assume moreover that
[TABLE]
for two positive constants . Then, it follows from (4.13) that
[TABLE]
for some positive constant . This rate is in accordance with the best possible rate for large deviation of partial sums of martingales differences, as proved in Theorem 2.1 of [15]. For partial sums of independent random variables, the rate (4.15) holds under weaker conditions on exponential moments, see Lanzinger and Stadtmüller [22].
Proof. From point 2 of Proposition 3.1 and condition (4.12), it is easy to see that, for any
[TABLE]
Applying Theorem 2.1 of Fan et al. [15] to the martingale sequence , we get, for any ,
[TABLE]
Combining the inequalities (4.1) and (4.17), we obtain the desired inequality. ∎
For the next proposition, let us introduce the random variables
[TABLE]
and note that
[TABLE]
According to Proposition 3.1, for any , .
Proposition 4.3**.**
Assume (3.5), and let . Assume that there exist two constants and such that, for any integer ,
[TABLE]
and
[TABLE]
Then, for all ,
[TABLE]
Remark 4.3*.*
According to Remark 4.2, under the conditions (4.19), (4.20) and (4.14), we have
[TABLE]
for some positive constant . This rate is in accordance with the best possible rate for large deviation of partial sums of martingales differences, as proved in Corollary 2.3 of [15]. Note that if , the condition (4.19) is true provided that
[TABLE]
For , the two conditions (4.23) and (4.20) are clearly less restrictive than (4.12), so Proposition 4.3 is more precise than Proposition 4.2 in the regime of large deviation. However, it does not allow to control moderate deviations for close to , which is possible via Proposition 4.2 (see for instance (1.6)).
Proof. From point 2 of Proposition 3.1 and condition (4.20), it is easy to see that, for any
[TABLE]
For any
[TABLE]
Thus
[TABLE]
Using Theorem 2.2 of Fan et al. [15], we have
[TABLE]
From the last inequality, we deduce that
[TABLE]
Using the exponential Markov inequality and the condition (4.19), we get, for all ,
[TABLE]
Taking , we have, for all ,
[TABLE]
Combining the last inequality and (4.1), we obtain the desired inequality. ∎
4.3 Fuk-Nagaev type bound
We now consider the case where the random variables have only a weak moment of order . For any real-valued random variable and any , define the weak moment of order by
[TABLE]
The following proposition is a Fuk-Nagaev type inequality (cf. Fuk [19] and Nagaev [25]; see also Fan et al. [16] and Rio [29] for martingales).
Proposition 4.4**.**
Let and , and consider the variables defined in (4.18). Assume that there exist two constants and such that, for any integer ,
[TABLE]
and
[TABLE]
Then, for all ,
[TABLE]
Remark 4.4*.*
Let us comment on Proposition 4.4.
If there exists a constant such that
[TABLE]
then, for any ,
[TABLE]
Thus under conditions (4.26), (4.27) and (4.29), we have
[TABLE] 2. 2.
Assume moreover that satisfies (3.5). Then, according to Remark 3.1, Proposition 4.4 remains valid when is replaced by Since and are independent, we easily see that
[TABLE]
and
[TABLE]
Thus if
[TABLE]
then condition (4.27) is satisfied with Of course, the same computations may be done by interchanging and . Hence, if
[TABLE]
then condition (4.27) still holds with
Proof. To prove Proposition 4.4, we need the following inequality whose proof can be found in Fan et al. [14] (cf. Corollary 2.3 and Remark 2.1 therein).
Lemma 4.1**.**
Assume that are square integrable martingale differences, and let and . Then, for all ,
[TABLE]
By Lemma 4.1 and Markov’s inequality, it follows that, for all ,
[TABLE]
It is easy to see that, for all ,
[TABLE]
and that, for all ,
[TABLE]
Thus, for all ,
[TABLE]
Taking and in the last inequality, we obtain, for all ,
[TABLE]
Combining the last inequality and (4.1), we obtain the desired inequality. ∎
4.4 von Bahr-Esseen’s inequality, weak form
We now consider the case where the variables and have only a weak moment of order .
Proposition 4.5**.**
Let . Assume that there exists positive constants such that, for any ,
[TABLE]
Then, for any
[TABLE]
where
[TABLE]
and
[TABLE]
Remark 4.5*.*
Let us comment on Proposition 4.5.
Contrary to the previous inequalities of Section 4, this inequality is truly non-stationary, in the sense that it is expressed in terms of the weak moments , without assuming a uniform bound (in ) on these moments. This will also be the case of the moment inequalities of Section 5. 2. 2.
Assume moreover that satisfies (3.5). Then, according to Remark 3.1, Proposition 4.4 remains true if condition (4.32) is replaced by
[TABLE]
In particular, if either
[TABLE]
or
[TABLE]
hold, then condition (4.34) is satisfied with . 3. 3.
Assume that and that , then
[TABLE]
Proof. By Proposition 3.3 of Cuny et al. [7], we have, for any
[TABLE]
From point 2 of Proposition 3.1 and condition (4.32), it follows that, for any
[TABLE]
Combining (4.35) and (4.36), we obtain the desired inequality. ∎
5 Moment inequalities
In this section, we shall control the -norm of the functional , for . The upper bounds will be expressed in terms of the moments of order of the dominating random variables . Let us emphasize that all the inequalities of these section are completely non-stationary, in the sense that we shall not assume a uniform bound (in ) on .
5.1 Marcinkiewicz-Zygmund type inequality
We assume in this subsection that the dominating random variables and have a moment of order .
Proposition 5.1**.**
Let . Assume that there exist positive constants such that
[TABLE]
Then
[TABLE]
where
[TABLE]
Remark 5.1*.*
Assume moreover that satisfies (3.5). Then, according to Remark 3.1, inequality (5.38) remains true if the second condition of (5.37) is replaced by
[TABLE]
Proof. Applying Theorem 2.1 of Rio [28], we get
[TABLE]
By Proposition 3.1 and condition (5.37), it follows that
[TABLE]
which gives the desired inequality. ∎
5.2 Rosenthal’s inequality
Under the same assumptions as in the previous subsection, one can prove the following Rosenthal-type inequality.
Proposition 5.2**.**
Let , and consider the variables defined in (4.18). If (5.37) holds, then there exists a constant depending only on such that
[TABLE]
Remark 5.2*.*
Assume that satisfies (3.5). Then, according to Remark 3.1, it follows from the proof of Proposition 5.2 that inequality (5.40) remains true if the second condition of (5.37) is replaced by (5.39).
Proof. From point 2 of Proposition 3.1, it is easy to see that
[TABLE]
and that
[TABLE]
The desired inequality is then a direct consequence of Rosenthal’s inequality for martingales (see for instance Theorem 2.12 of Hall and Heyde [20]). ∎
5.3 von Bahr-Esseen’s inequality
In this subsection, we assume that the dominating random variables and have a moment of order .
Proposition 5.3**.**
Let , and assume that (5.37) holds. Then
[TABLE]
where
[TABLE]
Remark 5.3*.*
Assume that satisfies (3.5). Then, according to Remark 3.1, it follows from the proof of Proposition 5.3 that inequality (5.41) remains true if the second condition of (5.37) is replaced by (5.39)
Proof. Using an improvement of the von Bahr-Esseen inequality (see inequality (1.11) in Pinelis [26]), we have
[TABLE]
where the constant is described in Proposition 1.8 of Pinelis [26], and is such that for any . By Proposition 3.1, it follows that
[TABLE]
which is the desired inequality. ∎
Aknowledgements
P. Doukhan wants to thank Tianjin University for its hospitality. His work has been developed within the MME-DII center of excellence (ANR-11-LABEX-0023-01) & PAI-CONICYT MEC No 80170072. X. Fan has been partially supported by the National Natural Science Foundation of China (Grant no. 11601375).
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] Adamczak, R., 2008. A tail inequality for suprema of unbounded empirical processes with applications to Markov chains. Electron. J. Probab. 13: 1000–1034.
- 2[2] Alquier, P., Doukhan, P., 2011. Sparsity considerations for dependent variables. Electron. J. Statist. 5: 750–774.
- 3[3] Bickel, P. J., Ritov, Y., Tsybakov, A., 2009. Simultaneous analysis of lasso and Dantzig selector. Ann. Statist. 37: 1705–1732.
- 4[4] Bardet, J.-M., Doukhan, P., 2018. Non-parametric estimation of time varying AR(1)–processes with local stationarity and periodicity. Electron. J. Statist. 12: 2323–2354.
- 5[5] Brockwell, P.J., Davis, R.A., 1987. Time series: theory and methods. Springer Science & Business Media.
- 6[6] Cox, P.M., Betts, R.A., Jones, C.D., Spall, S.A., Totterdell, I.J., 2000. Acceleration of global warming due to carbon-cycle feedbacks in a coupled climate model. Nature 408: 184–187.
- 7[7] Cuny, C., Dedecker, J., Merlevède, F., 2017. Large and moderate deviations for the left random walk on G L d ( ℝ ) 𝐺 subscript 𝐿 𝑑 ℝ GL_{d}(\mathbb{R}) . ALEA, Lat. Am. J. Probab. Math. Stat. 14: 503–527.
- 8[8] Dahlhaus, R., Richter, S., Wu, W.B., 2019. Towards a general theory for non-linear locally stationary processes. Bernoulli 25(2): 1013-1044.
