Skip to main content
Entropy logoLink to Entropy
. 2021 Mar 6;23(3):313. doi: 10.3390/e23030313

PAC-Bayes Bounds on Variational Tempered Posteriors for Markov Models

Imon Banerjee 1, Vinayak A Rao 1,*,, Harsha Honnappa 2,
Editor: Pierre Alquier
PMCID: PMC8000646  PMID: 33800820

Abstract

Datasets displaying temporal dependencies abound in science and engineering applications, with Markov models representing a simplified and popular view of the temporal dependence structure. In this paper, we consider Bayesian settings that place prior distributions over the parameters of the transition kernel of a Markov model, and seek to characterize the resulting, typically intractable, posterior distributions. We present a Probably Approximately Correct (PAC)-Bayesian analysis of variational Bayes (VB) approximations to tempered Bayesian posterior distributions, bounding the model risk of the VB approximations. Tempered posteriors are known to be robust to model misspecification, and their variational approximations do not suffer the usual problems of over confident approximations. Our results tie the risk bounds to the mixing and ergodic properties of the Markov data generating model. We illustrate the PAC-Bayes bounds through a number of example Markov models, and also consider the situation where the Markov model is misspecified.

Keywords: ergodicity, Markov chain, probably approximately correct, variational Bayes

1. Introduction

This paper presents probably approximately correct (PAC)-Bayesian bounds on variational Bayesian (VB) approximations of fractional or tempered posterior distributions for Markov data generation models. Exact computation of either standard or tempered posterior distributions is a hard problem that has, broadly speaking, spawned two classes of computational methods. The first, Markov chain Monte Carlo (MCMC), constructs ergodic Markov chains to approximately sample from the posterior distribution. MCMC is known to suffer from high variance and complex diagnostics, leading to the development of variational Bayesian (VB) [1] methods as an alternative in recent years. VB methods pose posterior computation as a variational optimization problem, approximating the posterior distribution of interest by the ‘closest’ element of an appropriately defined class of ‘simple’ probability measures. Typically, the measure of closeness used by VB methods is the Kullback–Leibler (KL) divergence. Excellent introductions to this so-called KL-VB method can be found in [2,3,4]. More recently, there has also been interest in alternative divergence measures, particularly the α-Rényi divergence [5,6,7], though in this paper, we focus on the KL-VB setting.

Theoretical properties of VB approximations, and in particular asymptotic frequentist consistency, have been studied extensively under the assumption of an independent and identically distributed (i.i.d.) data generation model [4,8,9]. On the other hand, the common setting where data sets display temporal dependencies presents unique challenges. In this paper, we focus on homogeneous Markov chains with parameterized transition kernels, representing a parsimonious class of data generation models with a wide range of applications. We work in the Bayesian framework, focusing on the posterior distribution over the unknown parameters of the transition kernel. Our theory develops PAC bounds that link the ergodic and mixing properties of the data generating Markov chain to the Bayes risk associated with approximate posterior distributions.

Frequentist consistency of Bayesian methods, in the sense of concentration of the posterior distribution around neighborhoods of the ‘true’ data generating distribution, have been established in significant generality, in both the i.i.d. [10,11,12] and in the non-i.i.d. data generation setting [13,14]. More recent work [14,15,16] has studied fractional or tempered posteriors, a class of generalized Bayesian posteriors obtained by combining the likelihood function raised to a fractional power with an appropriate prior distribution using Bayes’ theorem. Tempered posteriors are known to be robust against model misspecification: in the Markov setting we consider, the associated stationary distribution as well as mixing properties are sensitive to model parameterization. Further, tempered posteriors are known to be much simpler to analyze theoretically [14,16]. Therefore, following [14,15,16] we focus on tempered posterior distributions on the transition kernel parameters, and study the rate of concentration of variational approximations to the tempered posterior. Equivalently, as shown in [16] and discussed in Section 1.1, our results also apply to so-called α-variational approximations to standard posterior distributions over kernel parameters. The latter are modifications of the standard KL-VB algorithm to address the well-known problem of overconfident posterior approximations.

While there have been a number of recent papers studying the consistency of approximate variational posteriors [5,8,15] in the large sample limit, rates of convergence have received less attention. Exceptions include [9,15,17], where an i.i.d. data generation model is assumed. [15] establishes PAC-Bayes bounds on the convergence of a variational tempered posterior with fractional powers in the range [0, 1), while [9] considers the standard variational posterior case (where the fractional power equals 1). [17], on the other hand, establishes PAC-Bayes bounds for risk-sensitive Bayesian decision making problems in the standard variational posterior setting. The setting in [15] allows for model misspecification and the analysis is generally more straightforward than that in [9,17]. Our work extends [15] to the setting of a discrete-time Markov data generation model.

Our first results in Theorem 1 and Corollary 1 of Section 2 establish PAC-Bayes bounds for sequences with arbitrary temporal dependence. Our results generalize [15], [Theorem 2.4] to the non-i.i.d. data setting in a straightforward manner. Note that Theorem 1 also recovers ([16], [Theorem 3.3]), which is established under different ‘existence of test’ conditions. Our objective in this paper is to explicate how the ergodic and mixing properties of the Markov data generating process influences the PAC-Bayes bound. The sufficient conditions of our theorem, bounding the mean and variance of the log-likelihood ratio of the data, allows for developing this understanding, without the technicalities of proving the existence of test conditions intruding on the insights.

In Section 3, we study the setting where the data generating model is a stationary α-mixing Markov chain. Stationarity means that the Markov chain is initialized with the invariant distribution corresponding to the parameterized transition kernel, implying all subsequent states also follow this marginal distribution. The α-mixing condition ensures that the variance of the likelihood ratio of the Markov data does not grow faster than linear in the sample size. Our main results in this setting are applicable when the state space of the Markov chain is either continuous or discrete. The primary requirement on the class of data generating Markov models is for the log-likelihood ratio of the parameterized transition kernel and invariant distribution to satisfy a Lipschitz property. This condition implies a decoupling between the model parameters and the random samples, affording a straightforward verification of the mean and variance bounds. We highlight this main result by demonstrating that it is satisfied by a finite state Markov chain, a birth-death Markov chain on the positive integers, and a one-dimensional Gaussian linear model.

In practice, the assumption that the data generating model is stationary is unlikely to be satisfied. Typically, the initial distribution is arbitrary, with the state distribution of the Markov sequence converging weakly to the stationary distribution. In this setting, we must further assume that the class of data generating Markov chains are geometrically ergodic. We show that this implies the boundedness of the mean and variance of the log-likelihood ratio of the data generating Markov chain. Alternatively, in Theorem 4 we directly impose a drift condition on random variables that bound the log-likelihood ratio. Again, in this more general nonstationary setting, we illustrate the main results by showing that the PAC-Bayes bound is satisfied by a finite state Markov chain, a birth-death Markov chain on the positive integers, and a one-dimensional Gaussian linear model.

In preparation for our main technical results starting in Section 2 we first note relevant notations and definitions in the next section.

1.1. Notations and Definitions

We broadly adopt the notation in [15]. Let the sequence of random variables Xn=(X0,,Xn)Rm×(n+1) represent a dataset of n+1 observations drawn from a joint distribution Pθ0(n), where θ0ΘRd is the ‘true’ parameter underlying the data generation process. We assume the state space SRm of the random variables Xi is either discrete-valued or continuous, and write {x0,,xn} for a realization of the dataset. We also adopt the convention that 0log(0/0)=0.

For each θΘ, we will write pθ(n) as the probability density of Pθ(n) with respect to some measure Q(n), i.e., pθ(n):=dPθ(n)dQ(n), where Q(n) is either Lebesgue measure or the counting measure. Unless stated otherwise, all probabilities, expectations and variances, which we represent as P, E[X] and Var[X], are with respect to the true distribution Pθ0(n).

Let π(θ) be a prior distribution with support Θ. The αte-fractional posterior is defined as

πn,αte|Xn(dθ):=eαtern(θ,θ0)(Xn)π(dθ)eαtern(θ,θ0)(Xn)π(dθ), (1)

where, for θ0,θΘ, rn(θ,θ0)(·):=logpθ0(n)(·)pθ(n)(·), is the log-likelihood ratio of the corresponding density functions, and αte(0,) is a tempering coefficient. Setting αte=1 recovers the standard Bayesian posterior. Note that we will use superscripts to distinguish different quantities that are referred to just as α in the literature.

The Kullback–Leibler (KL) divergence between distributions P,Q is defined as

K(P,Q):=Xlogp(x)q(x)p(x)dx,

where p,q are the densities corresponding to P,Q on some sample space X. In particular, the KL divergence between the distributions parameterized by θ0 and θ is

K(Pθ0(n),Pθ(n)):=logpθ0(n)(x0,,xn)pθ(n)(x0,,xn)pθ0(n)(x0,,xn)dx0dxn=rn(θ,θ0)(x0,,xn)pθ0n(x0,,xn)dx0dxn. (2)

The αre-Rényi divergenceDαre(Pθ(n),Pθ0(n)) is defined as

Dαre(Pθ(n),Pθ0(n)):=1αre1logexpαrern(θ,θ0)(x0,,xn)pθ0(n)(x0,,xn)dx0dxn, (3)

where αre(0,1). As αre1, the αre-Rényi divergence recovers the KL divergence.

Let F be some class of distributions with support in Rd and such that any distribution P in F is absolutely continuous with respect to the tempered posterior: Pπn,αte|Xn.

Many choices of F exist; for instance (see also [15]), F can be the set of Gaussian measures, denoted FidΦ:

FidΦ={Φ(dθ;μ,Σ):μRd,Σd×dP.D.}, (4)

where P.D. references the class of positive definite matrices. Alternately, F can be the family of mean-field or factored distributions where the components θi of θ are independent of each other. Let π˜n,αte|Xn be the variational approximation to the tempered posterior, defined as

π˜n,αte|Xn:=argminρFK(ρ,πn,αte|Xn) (5)

It is easy to see that finding π˜n,αte|Xn in Equation (5) is equivalent to the following optimization problem:

π˜n,αte|Xn:=argmaxρFrn(θ,θ0)(x0,,xn)ρ(dθ)αte1K(ρ,π). (6)

Setting αte=1 again recovers the usual variational solution that seeks to approximate the posterior distribution with the closest element of F (the right-hand side above is called the evidence lower bound (ELBO)). Other settings of αte constitute αte-variational inference [16], which seeks to regularize the ‘overconfident’ approximate posteriors that standard variational methods tend to produce.

Our results in this paper focus on parametrized Markov chains. We term a Markov chain as ‘parameterized’ if the transition kernel pθ(·|·) is parametrized by some θΘRd. Let q(0)(·) be the initial density (defined with respect to the Lebesgue measure over Rm) or initial probability mass function. Then, the joint density is pθ(n)(x0,,xn)=q(0)(x0)i=0n1pθ(xi+1|xi); recall, this joint density pθ(n)(x0,,xn) corresponds to the walk probability of a time-homogeneous Markov chain. We assume that corresponding to each transition kernel pθ,θΘ, there exists an invariant distribution qθ()qθ that satisfies

qθ(x)=pθ(x|y)qθ(dy)xRm,θΘ.

We will also use qθ to designate the density of the invariant measure (as before, this is with respect to the Lebesgue or counting measure for continuous or discrete state spaces, respectively). A Markov chain is stationary if its initial distribution is the invariant probability distribution, that is, X0qθ.

Our results in the ensuing sections will be established under strong mixing conditions [18] on the Markov chain. Specifically, recall the definition of the α-mixing coefficients of a Markov chain {Xn}:

Definition 1

(α-mixing coefficient). Let Mij denote the σ-field generated by the Markov chain {Xk:ikj} parameterized by θΘ. Then, the α-mixing coefficient is defined as

αk=supt>0sup(A,B)Mt×Mt+kPθ(AB)Pθ(A)Pθ(B). (7)

Informally speaking, the α-mixing coefficients {αk} measure the dependence between any two events A (in the ‘history’ σ-algebra) and B (in the ‘future’ σ-algebra) with a time lag k. We note that we do not use superscripts to identify these α parameters, since they are the only ones with subscripts, and can be identified through this.

2. A Concentration Bound for the αre-Rényi Divergence

The object of analysis in what follows is the probability measure π˜n,αte|Xn(θ), the variational approximation to the tempered posterior. Our main result establishes a bound on the Bayes risk of this distribution; in particular, given a sequence of loss functions n(θ,θ0), we bound n(θ,θ0)π˜n,αte|Xn(θ)dθ. Following recent work in both the i.i.d. and dependent sequence settings [14,15,16], we will use n(θ,θ0)=Dαre(Pθ(n),Pθ0(n)), the αre-Rényi divergence between Pθ(n) and Pθ0(n) as our loss function. Unlike loss functions like Euclidean distance, Rényi divergence compares θ and θ0 through their effect on observed sequences, so that issues like parameter identifiability no longer arise. Our first result generalizes [15], [Theorem 2.1] to a general non-i.i.d. data setting.

Proposition 1.

Let F be a subset of all probability distributions on Θ. For any αre(0,1), ϵ(0,1) and n1, the following probabilistic uniform upper bound on the expected αre-Rényi divergence holds:

PsupρFDαre(Pθ(n),Pθ0(n))ρ(dθ)αre1αrern(θ,θ0)ρ(dθ)+K(ρ,π)+log(1ϵ)1αre1ϵ. (8)

The proof of Proposition 1 follows easily from [15], and we include it in Appendix B.1.1 for completeness. Mirroring the comments in [15], when ρ=π˜n,αte this result is precisely [14, Theorem 3.4]. We also note from [14] that αre,β(0,1]αre-Rényi divergences are all equivalent through the following inequality αre(1β)β(1αre)DβDαreDβαreβ. Hence, for the subsequent results, we simplify by assuming that αte=αre. This probabilistic bound implies the following PAC-Bayesian concentration bound on the model risk computed with respect to the fractional variational posterior:

Theorem 1.

Let F be a subset of all probability distributions parameterized by Θ, and assume there exist ϵn>0 and ρnF such that

  • i. 

    K(Pθ0(n),Pθ(n))ρn(dθ)=E[rn(θ,θ0)]ρn(dθ)nϵn,

  • ii. 

    Varrn(θ,θ0)ρn(dθ)nϵn, and

  • iii. 

    K(ρn,π)nϵn.

Then, for any αre(0,1) and (ϵ,η)(0,1)×(0,1),

PDαre(Pθ(n),Pθ0(n))π˜n,αre(dθ|X(n))(αre+1)nϵn+αrenϵnηlog(ϵ)1αre1ϵη. (9)

The proof of Theorem 1 is a generalization of [15] (Theorem 2.4) to the non-i.i.d. setting, and a special case of [16] (Theorem 3.1), where the problem setting includes latent variables. We include a proof for completeness. As noted in [15], the sufficient conditions follow closely from [13] and we will show that they hold for a variety of Markov chain models.

A direct corollary of Theorem 1 follows by setting η=1nϵn, ϵ=enϵn and using the fact that enϵn1nϵn. Note that Equation (9) is vacuous if η+ϵ>1. Therefore, without loss of generality, we restrict ourselves to the condition 2nϵn<1.

Corollary 1.

Assume ϵn>0, ρnF such that the following conditions hold:

  • i. 

    K(Pθ0(n),Pθ(n))ρn(dθ)=E[rn(θ,θ0)]ρn(dθ)nϵn,

  • ii. 

    Varrn(θ,θ0)ρn(dθ)nϵn, and

  • iii. 

    K(ρn,π)nϵn.

Then, for any αre(0,1),

PDαre(Pθ(n),Pθ0(n))π˜n,αre(dθ|X(n))2(αre+1)ϵn1αre12nϵn. (10)

We observe that Theorem 1 and Corollary 1 place no assumptions on the nature of the statistical dependence between data points. However, verification of the sufficient conditions is quite hard, in general. One of our key contributions is to verify that under reasonable assumptions on the smoothness of the transition kernel, the sufficient conditions of Theorem 1 and Corollary 1 are satisfied by ergodic Markov chains.

Observe that the first two conditions in Corollary 1 ensure that the distribution ρn concentrates on parameters θΘ around the true parameter θ0, while the third condition requires that ρn not diverge from the prior π rapidly as a function of the sample size n. In general, verifying the first and third conditions is relatively straightforward. The second condition, on the other hand, is significantly more complicated in the current setting of dependent data, as the variance of rn(θ,θ0) includes correlations between the observations {X0,,Xn}. In the next section, we will make assumptions on the transition kernels (and corresponding invariant densities) that ’decouple’ the temporal correlations and the model parameters in the setting of strongly mixing and ergodic Markov chain models, and allow for the verification of the conditions in Corollary 1. Towards this, Propositions 2 and 3 below characterize the expectation and variance of the log-likelihood ratio rn(·,·) in terms of the one-step transition kernels of the Markov chain. First, consider the expectation of rn(·,·) in condition (i).

Proposition 2.

Fix θ1,θ2Θ and consider the parameterized Markov transition kernels pθ1 and pθ2, and initial distributions qθ1(0) and qθ2(0). Let pθ1(n) and pθ2(n) be the corresponding joint probability densities; that is,

pθj(n)(x0,,xn)=qθj(0)(x0)i=1npθi(xi|xi1) (11)

for j{1,2}. Then, for any n1, the log-likelihood ratio rn(θ2,θ1) satisfies

Eθ1rn(θ2,θ1)=i=1nEθ1logpθ1(Xi|Xi1)pθ2(Xi|Xi1)+Eθ1[Z0], (12)

where Z0:=logqθ1(0)(X0)qθ2(0)(X0). The expectation in the first term is with respect to the joint density function pθ1(y,x)=pθ1(y|x)qθ1(i1)(x) where the marginal density satisfies

qθ1(i1)(x)=pθ1(i1)(x0,,xi2,x)dx0dxi2fori>1,andqθ1(0)(x)fori=1.

If the Markov chain is also stationary under θ1, then Equation (12) simplifies to

Eθ1rn(θ2,θ1)=nEθ1logpθ1(X1|X0)pθ2(X1|X0)+Eθ1[Z0]. (13)

Notice that Eθ1rn(θ2,θ1) is precisely the KL divergence, K(Pθ1(n),Pθ2(n)). Next, the following proposition uses [19] (Lemma 1.3) to upper bound the variance of the log-likelihood ratio.

Proposition 3.

Fix θ1,θ2Θ and consider parameterized Markov transition kernels pθ1 and pθ2, with initial distributions qθ1(0) and qθ2(0). Let pθ1(n) and pθ2(n) be the corresponding joint probability densities of the sequence (x0,,xn), and qθj(i) the marginal density for i{1,,n} and j{1,2}. Fix δ>0 and, for each i{1,,n}, define

Cθ1,θ2(i):=logpθ1(xi|xi1)pθ2(xi|xi1)2+δpθ1(xi|xi1)qθ1(i1)(xi1)dxidxi1.

Similarly, define Z0:=logqθ1(0)(X0)qθ2(0)(X0), and D1,2:=Eθ1Z02+δ. Suppose the Markov chain corresponding to θ1 is α-mixing with coefficients {αk}. Then,

Varrn(θ1,θ2)<i,j=1n4n+2nδ/2(Cθ1,θ2(i)+Cθ1,θ2(j)+Cθ1,θ2(i)Cθ1,θ2(j))α|ij|1δ/(2+δ)(14)+i=1n4n+2nδ/2(Cθ1,θ2(i)+D1,2+Cθ1,θ2(i)D1,2)αi1δ/(2+δ)(15)+Cov(Z0,Z0).

Note that this result holds for any parameterized Markov chain. In particular, when the Markov chain is stationary, Cθ1,θ2(i)=Cθ1,θ2(1)i and θΘ, and Equation (14) simplifies to

Varrn(θ1,θ2)<n4n+6nδ/2Cθ1,θ2(1)k0αkδ/(2+δ)+4n+2nδ/2(Cθ1,θ2(1)+D1,2+Cθ1,θ2(1)D1,2)k1αkδ/(2+δ)+Cov(Z0,Z0). (16)

If the sum k0αkδ/(2+δ) is infinite, the bound is trivially true. For it to be finite, of course, the coefficients αk must decay to zero sufficiently quickly. For instance, Theorem A.1.2 shows that if the Markov chain is geometrically ergodic, then the α-mixing coefficients are geometrically decreasing. We will use this fact when the Markov chain is non-stationary, as in Section 4. In the next section, however, we first consider the simpler stationary Markov chain setting where geometric ergodic conditions are not explicitly imposed. We also note that unless only a finite number of αk are nonzero, the sum k0αkδ/(2+δ) is infinite when δ=0, and our results will typically require δ>0.

3. Stationary Markov Data-Generating Models

Observe that the PAC-Bayesian concentration bound in Corollary 1 specifically requires bounding the mean and variance of the log-likelihood ratio rn(θ,θ0). We ensure this by imposing regularity conditions on the log-ratio of the one-step transition kernels and the corresponding invariant densities. Specifically, we assume the following conditions that decouple the model parameters from the random samples, allowing us to verify the bounds in Corollary 1.

Assumption 1.

There exist positive functions Mk(1)(·,·) and Mk(2)(·), k{1,2,,m} such that for any parameters θ1,θ2Θ, the log of the ratio of one-step transition kernels and the log of the ratio of the invariant distributions satisfy, respectively,

|logpθ1(x1|x0)logpθ2(x1|x0)|k=1mMk(1)(x1,x0)|fk(1)(θ2,θ1)|(x0,x1),and (17)
|logqθ1(x)logqθ2(x)|k=1mMk(2)(x)|fk(2)(θ2,θ1)|x. (18)

We further assume that for some δ>0, the functions fk(1),fk(2) and Mk(1) satisfy the following:

  • i 

    there exist constants Ck(t) and measures ρnF such that |fk(t)(θ,θ0)|2+δρn(dθ)<Ck(t)n for t{1,2}, n1 and k{1,2,,m}, and

  • ii 

    there exists a constant B such that Mk(1)(x1,x0)2+δpθj(x1|x0)qθj(0)(x0)dx1dx0<B,k{1,,m} and j{1,2}.

The following examples illustrate Equations (17) and (18) for discrete and continuous state Markov chains.

Example 1.

Suppose {X0,,Xn} is generated by the birth-death chain with parameterized transition probability mass function,

pθ(j|i)=θifj=i1,1θifj=i+1.

In this example, the parameter θ denotes the probability of birth. We shall see that, m=3: M1(1)(X1,X0)=I[X1=X0+1], M2(1)(X1,X0)=I[X1=X01], and M3(1)(X1,X0)=1. We also define M1(2)(X0)=1, and set M2(2)(X0) and M3(2)(X0) both to X01. Let f1(1)(θ,θ0)=logθ0θ, f2(1)(θ,θ0)=log1θ01θ, f3(1)(θ,θ0)=0, f1(2)(θ,θ0)=f3(2)(θ,θ0)=log1θ01θ, and f2(2)(θ,θ0)=logθ0θ. The derivation of these terms and that they satisfy the conditions of Assumption 1 is provided in the proof of Proposition 6.

Example 2.

Suppose {X0,,Xn} is generated by the ‘simple linear’ Gauss–Markov model

Xn=θXn1+Wn,

where {Wn} is a sequence of i.i.d. standard Gaussian random variables. Then, m=2, with M1(1)(Xn,Xn1)=|XnXn1|, M2(1)(Xn,Xn1)=Xn2,M1(2)(x)=x22 and M2(2)(X)=0. Corresponding to these, we have f1(1)(θ,θ0)=(θθ0),f2(1)(θ,θ0)=(θ02θ2),f1(2)(θ0,θ0)=(θ02θ2) and f2(2)(θ0,θ0)=0. The derivation of these quantities and that these satisfy the conditions of Assumption 1 under appropriate choice of ρn is shown in the proof of Proposition 10.

Note that assuming the same number m of Mk(1) and Mk(2) involves no loss of generality, since these functions can be set to 0. Both Equations (17) and (18) can be viewed as generalized Lipschitz-smoothness conditions, recovering the usual Lipschitz-smoothness when m=1 and when fk(t) is Euclidean distance. Our generalized conditions are useful for distributions like the Gaussian, where Lipschitz smoothness does not apply. From Jensen’s inequality we have |fk(t)(θ,θ0)|ρn(dθ)||fk(t)(θ,θ0)|2+δρn(dθ)12+δ, and Assumption 1(i) above implies that for some constant C>0 and k{1,2,,m},t{1,2},

|fk(t)(θ,θ0)|ρn(dθ)Cn1/(2+δ)<Cn. (19)

Assumption 1(i) is satisfied in a variety of scenarios, for example, under mild assumptions on the partial derivatives of the functions fk(t). To illustrate this, we present the following proposition.

Proposition 4.

Let f(θ,θ0) be a function on a bounded domain with bounded partial derivatives with f(θ0,θ0)=0. Let {ρn(·)} be a sequence of probability densities on θ such that Eρn[θ]=θ0 and Varρn[θ]=σ2n for some σ>0. Then, for some C>0,

|f(θ,θ0)|2+δρn(dθ)<Cn. (20)

Proof. 

Define θf(θ,θ0):=f(θ,θ0)θ as the partial derivative of the function f. By the mean value theorem, |f(θ,θ0)|=|θθ0||θf(θ*,θ0)|, for some θ*[min{θ,θ0},max{θ,θ0}]. Since the partial derivatives are bounded, there exists LR such that θf(θ*,θ0)<L, and |f(θ,θ0)|2+δρn(dθ)<L2+δ|θθ0|2+δρn(dθ). Choose G>0 be such that |θ|<G, then θθ02G2+δ<θθ02G2. Therefore, |θθ0|2+δρn(dθ)<(2G)2+δVarθ2G<(2G)δσ2n. Now choosing (2G)δσ2 as C completes the proof. □

If θfk(t) is continuous and Θ is compact, then θfk(t) is always bounded. Furthermore, observe that if EMk(1)(X1,X0)2+δ<B, without loss of generality we can use Jensen’s inequality to conclude that, for all 0<a<2+δ, EMk(1)(X1,X0)a<Ba2+δ<B.

We can now state the main theorem of this section.

Theorem 2.

Let {X0,,Xn} be generated by a stationary, α-mixing Markov chain parametrized by θ0Θ. Suppose that Assumption 1 holds and that the α-mixing coefficients satisfy k1αkδ/(2+δ)<+. Furthermore, assume that K(ρn,π)nC for some constant C>0. Then, the conditions of Corollary 1 are satisfied with ϵn=Omax(1n,nδ/2n).

Theorem 2 is satisfied by a large class of Markov chains, including chains with countable and continuous state spaces. In particular, if the Markov chain is geometrically ergodic, then it follows from Equation (A4) (in the appendix) that k1αkδ/(2+δ)<+. Observe that in order to achieve O(1n) convergence, we need δ1. Key to the proof of Theorem 2 is the fact that the variance of the log-likelihood ratio can be controlled via the application of Assumption 1 and Proposition 3. Note also that as δ decreases, satisfying the condition k1αkδ/(2+δ) requires the Markov chain to be faster mixing.

We now illustrate Theorem 2 for a number of Markov chain models. First, consider a birth-death Markov chain on a finite state space.

Proposition 5.

Suppose the data-generating process is a birth-death Markov chain, with one-step transition kernel parametrized by the birth probability θ0Θ. Let F be the set of all Beta distributions. We choose the prior to be a Beta distribution. Then, the conditions of Theorem 2 are satisfied and ϵn=O1n.

Proof. 

The proof of Proposition 5 follows from the more general Proposition 8, by fixing the initial distribution to the invariant distribution under θ0. Therefore it has been omitted. We simply refer to the proof of Proposition 8 under a more general setup in Appendix B.3. □

The birth-death chain on the finite state space is, of course, geometrically ergodic and the α-mixing coefficients αk decay geometrically. Note that the invariant distribution of this Markov chain is uniform over the state space, and consequently this is a particularly simple example. A more complicated and more realistic example is a birth-death Markov chain on the nonnegative integers. We note that if the probability of birth θ in a birth-death Markov chain on positive integers is greater than 0.5, then the Markov chain is transient, and consequently, not ergodic. Hence, our prior should be chosen to have support within (0,0.5). For that purpose, we define the class of scaled beta distributions.

Definition 2

(Scaled Beta). If X is a beta distribution on with parameters a and b, then Y is said to be a scaled beta distribution with same parameters on the interval (c,m+c) if

Y=mx+c;(m,c)R2

and in that case, the pdf of Y is obtained as

f(y)=1mBeta(a,b)ycma11ycmb1ify(c,m+c),0otherwise..

Here, E[Y]=maa+b+c and Var[Y]=m2ab(a+b)2(a+b+1). For the birth-death chain, we set m=0.5 and c=0 giving it support on (0,12). Setting m=2 and c=1 gives a beta distribution rescaled to have support on (1,1).

Proposition 6.

Suppose the data-generating process is a positive recurrent birth-death Markov chain on the positive integers parameterized by the birth probability θ0(0,12). Further let F be the set of all Beta distributions rescaled to have support (0,12). We choose the prior to be a scaled Beta distribution on (0,1/2) with parameters a and b. Then, the conditions of Theorem 2 are satisfied with ϵn=O1n.

Proof. 

The proof of Proposition 6 (for the stationary case) follows from the more general Proposition 9 (the nonstationary case) by fixing the initial distribution to the invariant distribution under θ0. We omit the proof and simply refer to the proof of Proposition 9 under a more general setup in Appendix B.3. □

Unlike with the finite state-space, the invariant distribution now depends on the parameter θΘ, and verification of the conditions of the proposition is more involved. In Appendix A.2, we prove that the class of scaled beta distributions satisfy the condition K(ρn,π)nϵn when the prior π is a beta or an uniform distribution. This fact will allow us to prove the above propositions.

Both Proposition 5 and Proposition 6 assume a discrete state space. The next example considers a strictly stationary simple linear model (as defined in Example 2), which has a continuous, unbounded state space.

Proposition 7.

Suppose the data-generating model is a stationary simple linear model:

Xn=θ0Xn1+Wn, (21)

where {Wn} are i.i.d. standard Gaussian random variables and |θ0|<1. Suppose that F is the class of all beta distributions rescaled to have the support (1,1). Then, the conditions of Theorem 2 are satisfied with ϵn=O1n.

Proof. 

This is a special case of the more general non-stationary simple linear model which is detailed in Proposition 10. Therefore, the proof of the fact that the simple linear model satisfies Assumption 1 when starting from stationarity is deferred to the proof of Proposition 10. The simple linear model with |θ0|<1 has geometrically decreasing (and therefore summable) α-mixing coefficients as a consequence of [20] (eq. (15.49)) and Theorem A.1.2. Combining these two facts, it follows that the conditions of Theorem 2 are satisfied. □

Observe that Theorem 1 (and Corollary 1) are general, and hold for any dependent data-generating process. Therefore, there can be Markov chains that satisfy these, but do not satisfy Assumption 1 which entails some loss of generality. However, as our examples demonstrate, common Markov chain models do indeed satisfy the latter assumption.

4. Non-Stationary, Ergodic Markov Data-Generating Models

We call a time-homogeneous Markov chain non-stationary if the initial distribution q(0) is not the invariant distribution. There are two sets of results in this setting: in Theorem 3 and Theorem 4 we explicitly impose the α-mixing condition, while in Theorem 5 we impose a f-geometric ergodicity condition (Definition A.1.2 in the appendix). As seen in Equation (A4) (in the appendix) if the Markov chain is also geometrically ergodic, then δ>0, αkδ/(2+δ)<. This condition can be relaxed, albeit at the risk of more complicated calculations that, nonetheless, mirror those in the geometrically ergodic setting. A common thread through these results is that we must impose some integrability or regularity conditions on the functions Mk(1).

First, in Theorem 3 we assume that the Mk(1) functions in Assumption 1 are uniformly bounded and that the α-mixing condition is satisfied. This result holds for both discrete and continuous state space settings.

Theorem 3.

Let {X0,,Xn} be generated by an α-mixing Markov chain parametrized by θ0Θ with transition probabilities satisfying Assumption 1 and with known initial distribution q(0). Let {αk} be the α-mixing coefficients under θ0, and assume that k1αkδ/(2+δ)<+. Suppose that there exists BR such that supx,y|Mk(1)(x,y)|<B for all k{1,2,,m} in Assumption 1. Furthermore, assume that there exists ρnF such that K(ρn,π)nC for some constant C>0. If the initial distribution q(0) satisfies Eq(0)|Mk(2)(X0)|2<+ for all k{1,2,,m}, then the conditions of Corollary 1 are satisfied with ϵn=Omax(1n,nδ/2n).

The following result in Proposition 8 illustrates Theorem 3 in the setting of a finite state birth-death Markov chain.

Proposition 8.

Suppose the data-generating process is a finite state birth-death Markov chain, with one-step transition kernel parametrized by the birth probability θ0. Let F be the set of all Beta distributions. We choose the prior on θ0 to be a Beta distribution. Then, the conditions of Theorem 3 are satisfied with ϵn=O1n for any initial distribution q(0).

Theorem 3 also applies to data generated by Markov chains with countably infinite state spaces, so long as the class of data-generating Markov chains is strongly ergodic and the initial distribution has finite second moments. The following example demonstrates this in the setting of a birth-death Markov chain on the positive integers, where the initial distribution is assumed to have finite second moments.

Proposition 9.

Suppose the data-generating process is a birth-death Markov chain on the non-negative integers, parameterized by the probability of birth θ0(0,12). Further let F be the set of all Beta distributions rescaled upon the support (0,12). Let q(0) be a probability mass function on non-negative integers such that i=1i2q(0)(i)<+. We choose the prior to be a scaled Beta distribution on (0,1/2) with parameters a and b. Then, the conditions of Theorem 3 are satisfied with ϵn=O1n.

Since continuous functions on a compact domain are bounded, we have the following (easy) corollary (stated without proof).

Corollary 2.

Let {X0,,Xn} be generated by an α-mixing Markov chain parametrized by θ0Θ on a compact state space, and with initial distribution q(0). Suppose the α-mixing coefficients satisfy k1αkδ/(2+δ)<+, and that Assumption 1 holds with continuous functions Mk(1)(·,·), k{1,2,,m}. Furthermore, assume that there exists ρn such that K(ρn,π)nC for some constant C. Then, Theorem 3 is satisfied with ϵn=Omax(1n,nδ/2n).

In general, the Mk(1) functions will not be uniformly bounded (consider the case of the Gauss–Markov simple linear model in Example 2), and stronger conditions must be imposed on the data-generating Markov chain itself. The following assumption imposes a ‘drift’ condition from [21]. Specifically, [21] (Theorem 2.3) shows that under the conditions of Assumption 2, the moment generating function of an aperiodic Markov chain {Xn} can be upper bounded by a function of the moment generating function of X0. Together with the α-mixing condition, Assumption 2 implies that this Markov data generating process satisfies Corollary 1.

Assumption 2.

Consider a Markov chain {Xn} parameterized by θ0Θ. Let Mn denote the σ-field generated by {X,,Xn1,Xn}. Denote the stochastic process {Mnk}:={Mk(1)(Xn,Xn1)}; recall Mk(1), for each k=1,,m1, are defined in Assumption 1. For each k=1,,m, assume the process {Mnk} satisfies the following conditions:

  • The drift condition holds for {Mnk}, i.e., EMnkMn1k|Mn1,Mn1k>aϵ for some ϵ,a>0.

  • For some λ>0 and D>0, Eeλ(MnkMn1k)|Mn1D.

Under this drift condition, the next theorem shows that Corollary 1 is satisfied.

Theorem 4.

Let {X0,,Xn} be generated by an aperiodic α-mixing Markov chain parametrized by θ0Θ and initial distribution q(0). Suppose that Assumption 1 and Assumption 2 hold, and that the α-mixing coefficients satisfy k1αkδ/(2+δ)<+. Furthermore, assume K(ρn,π)nC for some constant C>0. If eλMk(1)(y,x)pθ0(y|x)q1(0)(x)dx<+ for all k=1,,m1, then the conditions of Corollary 1 are satisfied with ϵn=Omax(1n,nδ/2n).

Verifying the conditions in Theorem 4 can be quite challenging. Instead, we suggest a different approach that requires f-geometric ergodicity. Unlike the drift condition in Assumption 2, f-geometric ergodicity additionally requires the existence of a petite set. As noted before, geometric ergodicity implies α-mixing with geometrically decaying mixing coefficients. As with Theorem 4, we assume for simplicity that the Markov chain is aperiodic.

Theorem 5.

Let {X0,,Xn} be generated by an aperiodic Markov chain parametrized by θ0Θ with known initial distribution q(0), and assumed to be V-geometrically ergodic for some V:Rm[1,). Suppose that Assumption 1 holds and Mk(1)(y,x)2+δpθ0(y|x)dy<V(x)k,xandsomeδ>0. Furthermore, assume that K(ρn,π)nC for some constant C>0. If the initial distribution q(0) satisfies Eq(0)[V(X0)]<+, then the conditions of Corollary 1 are satisfied with ϵn=Omax(1n,nδ/2n).

The following Proposition 10 shows, the simple linear model satisfies Theorem 5 when the parameter θ0 is suitably restricted.

Proposition 10.

Consider the simple linear model satisfying the equation

Xn=θ0Xn1+Wn, (22)

where {Wn} are i.i.d. standard Gaussian random variables and |θ0|<214+2δ1 for δ>0. Let F be the space of all scaled Beta distributions on (1,1) and suppose the prior π is a uniform distribution on (1,1). Then, the conditions of Theorem 5 are satisfied with ϵn=Omax(1n,nδ/2n), if the initial distribution q(0) satisfies Eq(0)[X04+2δ]<+.

5. Misspecified Models

We show next how our results can be extended to the misspecified model setting. Assume that the true data generating distribution is parametrized by θ0Θ. Let θn*:=argminθΘK(Pθ0(n),Pθ(n)) represent the closest parametrized distribution in the variational family to the data-generating distribution. Further, assume our usual conditions:

  • i. 

    E[rn(θ,θn*)]ρn(dθ)nϵn,

  • ii. 

    Varrn(θ,θn*)ρn(dθ)nϵn.

Now, since rn(θ,θ0)=rn(θ,θn*)+rn(θn*,θ0), we have

K(Pθ0(n),Pθ(n))ρn(dθ)E[rn(θ0,θn*)]+nϵn. (23)

Similarly, decomposing the variance it follows that

Var[rn(θ,θ0)]=Var[rn(θ,θn*)]+Var[rn(θn*,θ0)]+2Cov[rn(θ,θn*),rn(θn*,θ0)]. (24)

Using the fact that 2aba2+b2 on the covariance term 2Cov[rn(θ,θn*),rn(θn*,θ0)]=2Ern(θ,θn*)E[rn(θ,θn*)]rn(θn*,θ0)E[rn(θn*,θ0)], we have

Var[rn(θ,θ0)]2Var[rn(θ,θn*)]+2Var[rn(θn*,θ0)]. (25)

Integrating both sides with respect to ρn(dθ) we get

Var[rn(θ,θ0)]ρn(dθ)2Var[rn(θ,θn*)]ρn(dθ)+2Var[rn(θn*,θ0)]ρn(dθ)2nϵn+2Var[rn(θn*,θ0)]. (26)

Consequently, we arrive at the following result:

Theorem 6.

Let F be a subset of all probability distributions parameterized by Θ. Let θn*=argminθΘK(Pθ0(n),Pθ(n)) and assume there exist ϵn>0 and ρnF such that

  • i

    E[rn(θ,θn*)]ρn(dθ)nϵn,

  • ii

    Varrn(θ,θn*)ρn(dθ)nϵn, and

  • iii

    K(ρn,π)nϵn.

Then, for any αre(0,1) and (ϵ,η)(0,1)×(0,1),

P[Dαre(Pθ(n),Pθ0(n))π˜n,αre(dθ|X(n))(αre+1)nϵn+E[rn(θ0,θn*)]+αre2nϵn+2Var[rn(θn*,θ0)]ηlog(ϵ)1αre]1ϵη. (27)

The proof of this theorem is straightforward and follows from the proof of Theorem 1 by plugging in the upper bounds for KL-divergence from Equation (23), and variance from Equation (26) to (A13). A sketch of the proof is presented in the appendix.

6. Conclusions

Concentration of the KL-VB model risk, in terms of the expected αre-Rényi divergence, is well established under the i.i.d. data generating model assumption. Here, we extended this to the setting of Markov data generating models, linking the concentration rate to the mixing and ergodic properties of the Markov model. Our results apply to both stationary and non-stationary Markov chains, as well as to the situation with misspecified models. There remain a number of open questions. An immediate one is to extend the current analysis to continuous-time Markov chains and Markov jump processes, possibly using uniformization of the continuous time model. Another direction is to extend this to the setting of non-homogeneous Markov chains, where analogues of notions such as stationarity are less straightforward. Further, as noted in the introduction, [14] establish PAC-Bayes bounds under slightly weaker ‘existence of test functions’ conditions, while our results are established under the stronger conditions used by [15] for the i.i.d. setting. Weakening the conditions in our analysis is important, but complicated. A possible path is to build on results from [22], who provides conditions form the existence of exponentially powerful test functions exist for distinguishing between two Markov chains. It is also known that there exists a likelihood ratio test separating any two ergodic measures [23]. However, leveraging these to establish the PAC-Bayes bounds for the KL-VB posterior is a challenging effort that we leave to future papers. Finally it is of interest to generalize our PAC-bounds to posterior approximations beyond KL-variational inference, such as αre-Rényi posterior approximations [6], and loss-calibrated posterior approximations [24,25].

Acknowledgments

Rao and Honnappa acknowledge support from NSF DMS-1812197. In addition, Rao acknowledges NSF IIS-1816499 for supporting this project.

Appendix A. Technical Desiderata

Appendix A.1. Definitions Related to Markov Chains

As noted before, ergodicity plays an acute role in establishing our results. We consolidate various definitions used throughout the paper in this appendix. Recall that we assume the parameterized Markov chain possesses an invariant probability density or mass function qθ under parameter θΘ. Our results in Section 4 also rely on the ergodic properties of the Markov chain, and we assume that the Markov chain is f-geometrically ergodic [20] (Chapter 15). First, refer to the definition of the functional norm ·f, from Definition A.1.1,

Definition A.1.1

(f-norm). The functional norm in f-metric of a measure v, or the f-norm of v is

vf=supg:|g|<fgdv, (A1)

where f and g are any two functions.

An immediate consequence of this definition is that if f1,f2 are two functions such that f1<f2 (i.e., for all points in the support of the functions), then

vf1vf2. (A2)

Now that we have defined the ·f norm, we can now define f-geometric ergodicity. In the following, we assume the Markov chain is positive Harris; see [20] for a definition. This is a mild and fairly standard assumption in Markov chain theory.

Definition A.1.2

(f-geometric ergodicity). For any function f, Markov chain {Xn} parameterized by θΘ is said to be f-geometrically ergodic if it is positive Harris and there exists a constant rf>1, that depends on f, such that for any AB(X),

n=1nrfnPθ(XnA|X0=x)Aqθ(y)dyf<. (A3)

It is straightforward to see that this is equivalent to

Pθ(XnA|X0=x)qθ(y)dyfCrfn

for an appropriate constant C (which may depend on the state x), that is, the Markov chain approaches steady state at a geometrically fast rate. If a Markov chain is f-geometrically ergodic for f1, then, it is simply termed as geometrically ergodic. It is straightforward to see (via Theorem A.1.2 in the Appendix) that a geometrically ergodic Markov chain is also α-mixing, with mixing coefficients satisfying

k0αkυ<υ>0, (A4)

showing that, under geometric ergodicity, the α-mixing coefficients raised to any positive power υ are finitely summable. We note here that the most standard procedure to establish f-geometric ergodicity for any Markov chain is through the verification of the drift condition. The drift condition is a sufficient condition for a Markov chain to be f-geometrically ergodic, as long as there exists a set (called petite set) towards which the Markov chain drifts to (see Assumption A.1.1 in the appendix). If a Markov chain is f-geometrically ergodic with fV, for some particular function V, then we call it V-geometrically ergodic.

We defined V-geometric ergodicity in the previous sections. In this section, we provide a sufficient condition for a Markov chain to be V-geometrically ergodic. First, we recall the definition of resolvent from [20] (Chapter 5).

Definition A.1.3

(Resolvent). Let n{0,1,2,} and qn be such that qn0n and n=1qn=1. Note that qn can be thought of being a probability mass function for a random variable "q" taking values on non-negative integers. Then, the resolvent of a Markov chain with respect to q is given by Kq(x,A) where,

Kq(x,A)=n=0qnP(XnA|X0=x). (A5)

Then, the definition of petite sets follows (see, for Reference, [20] (Chapter 5)).

Definition A.1.4

(Petite Sets). Let X0,,Xn be n samples from a Markov chain taking values on the state space X. Let C be a set. We shall call C to be vq petite if

Kq(x,B)υq(B)

for all xC and BB(X), and a non-trivial measure υq on B(X), and a probability mass function q on {1,2,3,}

Now, let ΔV(x):=E[V(Xn)|Xn1=x]V(x) for V:S[1,).

Assumption A.1.1

(Drift condition). [20] (Chapter 5) Suppose the chain {Xn} is, aperiodic and ψ-irreducible. Let there exists a petite set C, constants b<,β>0, and a non-trivial function V:S[1,) satisfying

ΔV(x)βV(x)+bIxCxS. (A6)

If a Markov chain drifts towards a petite set then it is V-geometrically ergodic. Suppose, for simplicity, that V(x)=|X|. Then, the drift condition becomes E[|XnXx1]|Xn1|=β|Xn|+bIXnC. The left hand side of this equation represents the change in the state of the Markov chain in one time epoch. Thus, the condition in Assumption A.1.1 essentially states that the Markov chain drifts towards a petite set C and then, once it reaches that set, moves to any point in the state space with at least some probability independent of C.

Theorem A.1.1

(Geometrically ergodic theorem). Suppose that {Xn} is satisfies Assumption A.1.1. Then, the set SV={x:V(x)<} is absorbing, i.e., Pθ(X1SV|X0=x)=1xSV, and full, i.e., ψ(SVc)=0. Furthermore, constantsr>1,R< such that, for any AB(S),

Pθ(XnA|X0=x)Aqθ(y)dyVRrnV(x). (A7)

Any aperiodic and ψ-irreducible Markov chain satisfying the drift condition is geometrically ergodic. A consequence of Equation (A2) is that if, {Xn} is V-geometrically ergodic, then for any other function U,suchthat|U|<V, it is also U-geometrically ergodic. In essence, a geometrically ergodic Markov chain is asymptotically uncorrelated in a precise sense. Recall ρ-mixing coefficients defined as follows. Let A be a sigma field and L2(A) be the set of square integrable, real valued, A measurable functions.

Definition A.1.5

(ρ-mixing coefficient). Let Mij denote the sigma field generated by the measures Xk,whereikj. Then,

ρk=supt>0sup(f,g)L2Mt×L2Mt+kCorr(f,g), (A8)

where Corr is the correlation function.

Theorem A.1.2.

If Xn is geometrically ergodic, then it is α-mixing. That is, there exists a constant c>0 such that αk=O(eck).

Proof. 

By [26] (Theorem 2) it follows that a geometrically ergodic Markov chain is asymptotically uncorrelated with ρ-mixing coefficients (see Definition A.1.5) that satisfy ρk=O(eck). Furthermore, it is well known that [18,26] αk14ρk, implying αk=O(eck). □

Appendix A.2. Bounding the KL-Divergence between Beta Distributions

The following results will be utilized in the proofs of Propositions 8–10.

Lemma A.2.1.

Let θ0(0,1). Let, ρn be a sequence of Beta distributions with parameters an=nθ0 and bn=n(1θ0). Let π denote an uniform distribution, U(0,1). Then, K(ρn,π)<C+12log(n), for some constant C>0.

Proof. 

Without loss of generality, we can assume an>1 and bn>1. The same form of the result can be obtained in all the other cases, by appropriate use of the bounds presented in the proof. We write the KL divergence K(ρn,π) as logρnπρn(dθ). Since π is uniform, π(θ)=1 whenever θ(0,1). Hence, the KL-divergence can be written as the negative of the entropy of ρn 01logρnθρn(dθ), which can be written as

K(ρn,π)=(an1)ψ(an)+(bn1)ψ(bn)(an+bn2)ψ(an+bn)logBeta(an,bn), (A9)

where ψ is the digamma function. Using Stirling’s approximation on Beta(an,bn) yields,

Beta(an,bn)=2πanan1/2bnbn1/2(an+bn)an+bn1/2(1+o(1)).

Hence, setting C1=log(2π), we can write logBeta(an,bn) as,

logBeta(an,bn)=C1(an12)log(an)(bn12)log(bn)+(an+bn12)log(an+bn)+log(1+o(1)).

From [27] we have that log(x)1x<ψ(x)<log(x)12xx>0. Since we assumed an>1 and bn>1, the fact that ψ(x)<log(x)12x implies

(an1)ψ(an)<(an1)log(an)an12anand,(bn1)ψ(bn)<(bn1)log(bn)bn12bn.

Finally, using the fact that log(x)1x<ψ(x), we get,

(an+bn2)ψ(an+bn)<(an+bn2)log(an+bn)+an+bn2an+bn.

Therefore, after much cancellation, the KL-divergence

(an1)ψ(an)+(bn1)ψ(bn)(an+bn2)ψ(an+bn)logBeta(an,bn)

can be upper bounded by

12log(an)12log(bn)+32log(an+bn)+an+bn2an+bnan12anbn12bn.

Now, plugging in the values of an and bn, we get Plugging in the values of an and bn, we get as upper bound for the KL-divergence as,

K(ρn,π)<12log(nθ0)12log(n(1θ0))+32log(n)+n2nnθ012nθ0n(1θ0)12n(1θ0)=12log(n)12log(θ0)+log(1θ0)+32n12nθ012n(1θ0)<C+12log(n),

for some large enough positive constant C. This completes our proof. □

Proposition A.2.1.

Let θ0(0,1). Let, ρn be a sequence of Beta distributions with parameters an=nθ0 and bn=n(1θ0). Let π denote an Beta distribution, with parameters (a,b). Then, K(ρn,π)<C+12log(n), for some constant C>0.

Proof. 

Without loss of generality, we assume a>1 and b>1. As mentioned in the proof of Lemma A.2.1, the other cases follows similarly. We write the KL-divergence between ρn and π as,

K(ρn,π)=logρnπρn(dθ)=logρnUρn(dθ)+logUπρn(dθ),

where, U is an uniform distribution on (0,1). We analyze the second term in the above expression. The second term can be written as,

logUπρn(dθ)=log11Beta(a,b)θa1(1θ)b1ρn(dθ)=C1(a1)log(θ)ρn(dθ)(b1)log(1θ)ρn(dθ),

where C1 is log(Beta(a,b)). Since, ρn follows a Beta distribution with parameters an=nθ0 and bn=n(1θ0), we get that,

logUπρn(dθ)=C1(a1)ψ(an)ψ(an+bn)(b1)ψ(bn)ψ(an+bn)

Since, log(x)1x<ψ(x)<log(x)12x, looking at the term ψ(an)ψ(an+bn), we get that,

ψ(an)ψ(an+bn)=ψ(nθ0)ψ(nθ0+n(1θ0))=ψ(nθ0)ψ(n).

Using the lower bound on ψ(nθ0) and the upper bound on ψ(n), we get

ψ(an)ψ(an+bn)<log(nθ0)+1nθ0+log(n)12n=log(θ0)+2θ02nθ0.

Furthermore, similarly, we get that,

ψ(bn)ψ(an+bn)<log(1θ0)+2(1θ0)2n(1θ0).

Therefore it follows that

max(a1)ψ(an)ψ(an+bn),(b1)ψ(bn)ψ(an+bn)<max(a1)log(θ0)+2θ02nθ0,(b1)log(1θ0)+2(1θ0)2n(1θ0)<C,

for a large positive constant C. Using the above bounds, we finally show that,

C1(a1)ψ(an)ψ(an+bn)(b1)ψ(bn)ψ(an+bn)<C1+2C,

which can be upper bounded by C for some large constant C. Finally, we upper bound logρnUρn(dθ) by Lemma A.2.1 thereby completing the proof. □

Appendix B. Proofs of Main Results

Appendix B.1. Proofs for A Concentration Bound for the αre-Rényi Divergence

Appendix B.1.1. Proof of Proposition 1

We start by recalling the variational formula of Donsker and Varadhan [28].

Lemma B.1.1

(Donsker-Varadhan)b. For any probability distribution function π on Θ, and for any measurable function h:ΘR, if ehdπ<, then

logehdπ=supρM+(Θ)hdρK(ρ,π) (A10)

Now, fix αre(0,1), and θΘ. First, observe that by the definition of the αre-Rényi divergence we have

Eθ0(n)[exp(αrern(θ,θ0))]=exp[(1αre)Dαre(Pθ(n),Pθ0(n))]

Multiplying both sides of the equation by exp[(1αre)Dαre(Pθ(n),Pθ0(n)) and integrating with respect to (w.r.t.) π(θ) it follows that

Eθ0(n)expαrern(θ,θ0)+(1αre)Dαre(Pθ(n),Pθ0(n))π(dθ)=1,or
Eθ0(n)expαrern(θ,θ0)+(1αre)Dαre(Pθ(n),Pθ0(n))π(dθ)=1.

Define h(θ):=αrern(θ,θ0)+(1αre)Dαre(Pθ(n),Pθ0(n)). Then, applying Lemma B.1.1 to the integrand on the left hand side (l.h.s.) above, it follows that

Eθ0(n)expsupρM+(Θ)h(θ)ρ(dθ)K(ρ,π)=1.

Multiply both sides of this equation by ϵ>0 to obtain

Eθ0(n)expsupρM+(Θ)h(θ)ρ(dθ)K(ρ,π)+log(ϵ)=ϵ.

Now, by Markov’s inequality, we have

Pθ0(n)supρM+(Θ)(αrern(θ,θ0)+(1αre)Dαre(Pθ(n),Pθ0(n)))ρ(dθ)K(ρ,π)+log(ϵ)0ϵ. (A11)

Thus, it follows via complementation that

Pθ0(n)[ρF(Θ)Dαre(Pθ(n),Pθ0(n))ρ(dθ)αre(1αre)rn(θ,θ0)ρ(dθ)+K(ρ,π)log(ϵ)1αre]1ϵ,

thereby completing the proof.

Appendix B.1.2. Proof of Theorem 1

Recall the definition of the fractional posterior and the VB approximation,

πn,αre|Xn=expαrern(θ,θ0)(Xn)π(dθ)expαrern(γ,θ0)(Xn)π(dγ),π˜n,αre|Xn=argminρFK(ρ,πn,αre|X(n)).

It follows by definition of the KL divergence that

π˜n,αre|Xn=argminρFαrern(θ,θ0)ρ(dθ)+K(ρ,π), (A12)

where π is the prior distribution. Following Proposition 1 it follows that for any ϵ>0

Dαre(Pθ(n),Pθ0(n))π˜(dθ|Xn)αre(1αre)rn(θ,θ0)ρ(dθ)+K(ρ,π)log(ϵ)1αre,

with probability 1ϵ. We fix an η(0,1). Using Chebychev’s inequality, we have

Pθ0(n)[αre1αrern(θ,θ0)ρn(dθ)αre1αreE[rn(θ,θ0)]ρn(dθ)+αre1αreVar[rn(θ,θ0)ρn(dθ)]η+K(ρn,π)1αre]=Pθ0(n)[αre1αrern(θ,θ0)ρn(dθ)αre1αreE[rn(θ,θ0)]ρn(dθ)K(ρn,π)1αreαre1αreVar[rn(θ,θ0)ρn(dθ)]η]Varαre1αrern(θ,θ0)ρn(dθ)αre1αreE[rn(θ,θ0)]ρn(dθ)K(ρn,π)1αreαre21αre2Var[rn(θ,θ0)ρn(dθ)]η.

Note that αre1αreE(rn(θ,θ0))ρn(dθ) and K(ρn,π)1αre are constants with respect to the data, implying

Var[αre1αrern(θ,θ0)ρn(dθ)αre1αreE[rn(θ,θ0)]ρn(dθ)K(ρn,π)1αre]=αre2(1αre)2Varrn(θ,θ0)ρn(dθ).

Therefore, we have

Pθ0(n)[αre1αrern(θ,θ0)ρn(dθ)αre1αreE[rn(θ,θ0)]ρn(dθ)+αre1αreVar[rn(θ,θ0)ρn(dθ)]η+K(ρn,π)1α]η.

From Proposition 1, with probability 1ϵ the following holds

Dαre(Pθ(n),Pθ0(n))π˜n,αre|Xn(dθ)αrern(θ,θ0)ρn(dθ)+K(ρn,π)log(ϵ)1αre.

Therefore, with probability 1ηϵ the following statement holds

Dαre(Pθ(n),Pθ0(n))π˜n,αre|Xn(dθ)αre1αreK(Pθ0(n),Pθ(n))ρn(dθ)+αre1αreVar[rn(θ,θ0)ρn(dθ)]η+K(ρn,π)log(ϵ)1αre. (A13)

Next, we observe that

Varrn(θ,θ0)ρn(dθ)=Eθ0(n)rn(θ,θ0)ρn(dθ)Ern(θ,θ0)ρn(dθ)2Var[rn(θ,θ0)]ρn(dθ),

by a straightforward application of Jensen’s inequality to the inner integral on the left hand side. Finally, following the hypotheses (i), (ii) and (iii), we have,

Dαre(Pθ(n),Pθ0(n))π˜n,αre|Xn(dθ)αre1αreK(Pθ0(n),Pθ(n))+Var[rn(θ,θ0)]ρn(dθ)ηρn(dθ)+1αreK(ρn,π)log(ϵ)αre(ϵn+nϵnη)1αre+nϵnlog(ϵ)1αre,

thereby concluding the proof. □

Appendix B.1.3. Proof of Proposition 2

We define Yi:=logpθ1(Xi|Xi1)pθ2(Xi|Xi1) for i=1,,n, and Z0=logq1(0)(X0)q2(0)(X0). Then, using the Markov property we can see that the Kullback–Leibler divergence between the joint distributions Pθ1(n) and Pθ2(n) satisfies KPθ1(n),Pθ2(n)=i=1nEθ1Yi+Eθ1[Z0]. If the Markov chain {Xi} is stationary under θ1, so is {Yi}. Hence Yi=dY1 and the above equation reduces to,

KPθ1(n),Pθ2(n)=nEθ1Y1+Eθ1[Z0]. (A14)

Appendix B.1.4. Proof of Proposition 3

First, recall the following result from [19].

Lemma B.1.2.

[19] (Lemma 1.2) Let X,,X1,X2, be an α-mixing Markov chain with α-mixing coefficients given by αk. Let Mab be the sigma-field generated by the subsequence (Xa,Xa+1,,Xb). Let ηtMt and τtMt+k be adapted random variables such that |ηt|1,|τt|1. Then,

suptsupηt,τt|E[ηtτt]E[ηt]E[τt]|4αk. (A15)

This lemma provides an upper bound on the covariance of events ηandτ, as shown next.

Lemma B.1.3.

Let ηMtτMt+k be such that, E|η|2+δC1,E|τ|2+δC2forsomeδ>0. Then, for a fixed n<+, we have

|EητEηEτ|4n+2nδ/2(C1+C2)+2nδ/2C1C2αk2δ/(2+δ). (A16)
Proof. 

Let N<+ be a fixed number. We get from the triangle inequality that

|EητEηEτ||EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|+|EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|+|EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|+|EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|. (A17)

Multiplying and dividing the first term by N2 and applying Lemma B.1.2, we get |EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|4N2αk. For the second term, if |τ|N, then τN and τN. Plugging this in the second term we get,

(A18)|EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|NEηI[|η|N+NEηI[|η|N](A19)=2N|EηI[|η|N]|.

Since |η|N, we have 1|η|1+δN1+δ. Following this,

(A20)|2NEηI[|η|N]|2NE|η|2+δN1+δI[|η|N](A21)2N1N1+δ|Eη2+δ|2C1Nδ.

Similarly, we can also write for the third term, |EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|2C2Nδ. Finally, for the last term we get that by Cauchy-Schwarz inequality,

|EητI[|η|N,|τ|N]EηI[|η|N]EτI[|τ|N]|VarηI[|η|N]VarτI[|τ|N] (A22)
<2VarηI[|η|N]VarτI[|τ|N] (A23)
2Eη2I[|η|N]Eτ2I[|τ|N]. (A24)

Since |η|>N, 1<|η|δNδ. Similarly, 1<|τ|δNδ. Plugging these in the previous equation, we get,

Eη2I[|η|N]Eτ2I[|τ|N]1N2δE|η|2+δI[|η|N]E|τ|2+δI[|τ|N] (A25)
1NδC1C2. (A26)

Combining the four upper bounds above, we get,

|EητEηEτ|4N2αk+2Nδ(C1+C2)+2NδC1C2. (A27)

Now, in particular, setting N=n1/2αk1/(2+δ) it follows that

|EητEηEτ|4nαkδ/(2+δ)+2nδ/2αkδ/(2+δ)(C1+C2)+2nδ/2αkδ/(2+δ)C1C2 (A28)
=4n+2nδ/2(C1+C2)+2nδ/2C1C2αkδ/(2+δ). (A29)

Lemma B.1.4.

Let {Xt} be an α-mixing Markov chain with mixing coefficient αk. Further assume that E|Xt|2+δC1andE|Xt+k|2+δC2 for some δ>0. Then, for any t and any n>0

|Cov(Xt,Xt+k)|4n+2nδ/2(C1+C2)+2nδ/2C1C2αkδ/(2+δ). (A30)
Proof. 

Set η=Xt,τ=Xt+k Lemma B.1.3. □

We also need to establish the following technical lemma.

Lemma B.1.5.

Let {Xt} be an α-mixing Markov Chain with mixing coefficients {αt}. Then the process {Yt} where Yt:=logpθ0(Xt|Xt1)pθ(Xt|Xt1) is also α-mixing with mixing coefficients {α˜t} where α˜t=αt1.

Proof. 

By Zi denote the paired random measure (Xi,Xi1). Let Mij denote the sigma field generated by the measures Xk,whereikj. By Gij denote the sigma field generated by the measures Zk,whereikj. Let CMi1j. Then, C can be expressed as (Ci1×Ci××Cj). for Ci1Mi1i1,CiMii and so on. Now, consider a map. Tij:(Ci1×Ci××Cj)(Ci1×Ci×Ci××Cj1×Cj1×Cj). Note that, Tij(C)Gij. It is easy to see that Gij=Tij(Mi1j)Mi1*j, where Tij(Mi1j) is obtained by applying the map Tij to each element of Mi1j. If we assume this latter set to be the range and Mi1j to be the domain, then, by construction, Tij is a bijection. Furthermore, the two classes are made of disjoint sets, i.e., if ATij(Mi1j)andA*Mi1*j, then AA*=ϕ. Furthermore, note that Mi1j* is made of impossible sets. i.e., P(A*)=0A*Mi1j*. Now consider the α-mixing coefficients for Zi. By definition, it is given by

αkz=supisupAGi,BGi+k|P(AB)P(A)P(B)|=supisupAGi,BGi+k|P((AoA*)(BoB*))P((AoA*))P((BoB*))|.

where,

A=(AoA*) B=(BoB*)
AoTi(Mi) A*M*i
BoTi+k1(Mj+k1) B*Mj+k1*.

Then, the expression for the α-mixing coefficient can be reduced into

αkz=supisupAoTi(Mi),BoTi+k1(Mi+k1)|P(AoBo)P(Ao)P(Bo)|.

Note that, by bijection property of Tij, we can find AMi and BMi+k1 such that

αkz=supisupAMi,BMi+k1|P(Ti(A)Ti+k1(B))P(Ti(A))P(Ti+k1(B))|.=αk1.

Now, logpθ0(Xn|Xn1)pθ(Xn|Xn1) is just a function of the paired Markov chain Zi, therefore it has α-mixing coefficient αk1. □

We now proceed to the proof of Proposition 3. Let {Xk} be a stationary α-mixing Markov chain under θ1 with mixing coefficients {αk}. Observe that the log-likelihood can be expressed as

rn(θ2,θ1)=i=1nlogpθ1(Xi|Xi1)pθ2(Xi|Xi1)+logq1(0)(X0)q2(0)(X0)i=1nYi+Z0.

Therefore, the variance of the log-likelihood ratio is simply

Varθ1rn(θ2,θ1)=Varθ1i=1nYi+Z0=i,j=1nCovθ1(Yi,Yj)+i,j=1nCovθ1(Yi,Z0)+Covθ1(Z0,Z0).

It follows from Lemma B.1.5 that {Yk} is a stochastic process with α-mixing coefficients αk1. Therefore, using Lemma B.1.4 we have

|Covθ1(Yi,Yj)|=|Eθ1YiYjEθ1YiEθ1Yj|<(4n+2nδ/2(Eθ1|Yi|2+δ+Eθ1|Yj|2+δ+Eθ1|Yi|2+δEθ1|Yj|2+δ))α|ji|1δ/(2+δ)=4n+2nδ/2(Cθ1,θ2(i)+Cθ1,θ2(j)+Cθ1,θ2(i)Cθ1,θ2(j))α|ji|1δ/(2+δ).

Similarly, as above we can also say

|Covθ1(Yi,Z0)|<4n+2nδ/2(Cθ1,θ2(i)+D1,2+Cθ1,θ2(i)D1,2)αi1δ/(2+δ)

Combining, the two upper bounds above, we get the first result:

Varθ1rn(θ2,θ1)<i,j=1n4n+2nδ/2(Cθ1,θ2(i)+Cθ1,θ2(j)+Cθ1,θ2(i)Cθ1,θ2(j))α|ij|1δ/(2+δ)+i=1n4n2+2nδ/2(Cθ1,θ2(i)+D1,2+Cθ1,θ2(i)D1,2)αi1δ/(2+δ)+Var[Z0,Z0].

If {Xi} is stationary under θ1, so is {Yi}. Therefore, Eθ1|Yi|2+δ=Eθ1|Y1|2+δ=Cθ1,θ2(1)i, and

i,j=1nCovθ1(Yi,Yj)i,j=1n4n+6nδ/2Cθ1,θ2(1)α|ji|1δ/(2+δ)n4n+6nδ/2Cθ1,θ2(1)h1αh1δ/(2+δ). (A31)

Again, using Lemma B.1.4 on Covθ1(Yi,Z0), yields

i=1nCovθ1(Yi,Z0)4n+2nδ/2(Cθ+D1,2+CθD1,2)h1αhδ/(2+δ). (A32)

Finally, using Equations (A31) and (A32) we have

Varθ1rn(θ2,θ1)n4n+6nδ/2Cθ1,θ2(1)h1αh1δ/(2+δ)+4n+2nδ/2(Cθ1,θ2(1)+D1,2+Cθ1,θ2(1)D1,2)h1αhδ/(2+δ)+Covθ1(Z0,Z0).

Appendix B.2. Proofs for Stationary Markov Data-Generating Models

Proof of Theorem 2

Part 1: Verifying condition (i) of Corollary 1.

We substitute the true parameter θ0 for θ1 and θ for θ2. We also set q1(0) to be the invariant distribution of the Markov chain under θ0, q0, and q2(0) as the invariant distribution of the Markov chain under θ, qθ. Applying the fact that these Markov chains are stationary to Proposition 2, we have

K(Pθ0(n),Pθ(n))=nElogpθ0(X1|X0)pθ(X1|X0)+E[Z0],nj=1mEMj(1)(X1,X0)|fj(1)(θ,θ0)|+k=1mE[Mk(2)(X0)]|fk(2)(θ,θ0)|, (A33)

where the inequality follows from Assumption 1. Therefore, it follows that

K(Pθ0(n),Pθ(n))ρn(dθ)nj=1mEMj(1)(X1,X0)|fj(1)(θ,θ0)|ρn(dθ)+k=1mE[Mk(2)(X0)]|fk(2)(θ,θ0)|ρn(dθ).

By Assumption 1(i), it follows that

K(Pθ0(n),Pθ(n))ρn(dθ)nj=1mEMj(1)(X1,X0)Cn+k=1mE[Mk(2)(X0)]Cnnϵn(1),

where ϵn(1)=O1n.

Part 2: Verifying condition (ii) of 1. Again, using Proposition 3 along with the fact that the Markov chain is stationary we have

Var[rn(θ,θ0)]n4n+6nδ/2Cθ0,θ(1)k0αkδ/(2+δ)+4n2+2nδ/2(Cθ0,θ(1)+Dθ0,θ+Cθ0,θ(1)Dθ0,θ)k1αkδ/(2+δ)+Var[Z0].

It then follows that

Var[rn(θ,θ0)]ρn(dθ)n4n+6nδ/2Cθ0,θ(1)ρn(dθ)k1αk1δ/(2+δ)+Var[Z0]ρn(dθ)+(4n2+2nδ/2(Cθ0,θ(1)ρn(dθ)+Dθ0,θρn(dθ)+Cθ0,θ(1)Dθ0,θρn(dθ)))k1αkδ/(2+δ).

First, consider the term Cθ0,θ(1)ρn(θ), and observe that

Cθ0,θ(1)ρn(dθ)=Elogpθ0(X1|X0)pθ(X1|X0)2+δρn(dθ).

By Assumption 1, we have

Elogpθ0(X1|X0)pθ(X1|X0)2+δρn(dθ)Ej=1mMj(1)(X1,X0)|fk(1)(θ,θ0)|2+δρn(dθ).

Since the function xx2+δ is convex, we can apply Jensen’s inequality to obtain,

j=1mMj(1)(X1,X0)|fk(1)(θ,θ0)|2+δm1+δk=1mMj(1)(X1,X0)2+δ|fk(1)(θ,θ0)|2+δ.

Therefore, it follows that

Elogpθ0(X1|X0)pθ(X1|X0)2+δρn(dθ)m1+δk=1mE[Mk(1)(X1,X0)2+δ]×|fk(1)(θ,θ0)|2+δρn(dθ).

By Assumption 1, |fk(θ,θ0)|2+δρn(dθ)<Cn and E[Mk(1)(X1,X0)2+δ]<B, implying that

Cθ0,θ(1)ρn(dθ)m1+δk=1mBCn=m2+δBCn.

Since k0αkδ/(2+δ)<, it follows that 4n+6nδ/2Cθ0,θ(1)ρn(dθ)k1αk1δ/(2+δ)=O(nδ/2n). Similarly, we can show that Dθ0,θρn(dθ)=O(1n), and Var[Z0]ρn(dθ)=O(1n).

For the final term Cθ0,θ(1)Dθ0,θρn(dθ), use the Cauchy-Schwarz inequality to obtain the upper bound Cθ0,θ(1)ρn(dθ)Dθ0,θρn(dθ)1/2 which is also of order O(1n). Combining all of these together we have

Var[rn(θ,θ0)]ρn(dθ)nϵn(2),

for some ϵn(2)=O(nδ/2n).

Since K(ρn,π)<nC=nCn, it follows that K(ρn,π)<nϵn(3), where ϵn(3)=O(1/n) as before. Finally, by choosing ϵn=max(ϵn(1),ϵn(2),ϵn(3)), our theorem is proved. □

Appendix B.3. Proofs for Non-Stationary, Ergodic Markov Data-Generating Models

Appendix B.3.1. Proof of Theorem 3

Part 1: Verifying condition (i) of Corollary 1: As in the proof of Theorem 2 substitute the true parameter θ0 for θ1 and θ for θ2 in. We also set q1(0) and q2(0) to the distribution q(0). Applying Proposition 2 to the corresponding transition kernels and initial distribution we have,

K(Pθ0(n),Pθ(n))=i=1nElogpθ0(Xi|Xi1)pθ(Xi|Xi1)+ElogD(X0)D(X0)=i=1nElogpθ0(Xi|Xi1)pθ(Xi|Xi1). (A34)

Now, applying Assumption 1, we can bound the previous equation as follows,

K(Pθ0(n),Pθ(n))i=1nEk=1mMk(1)(Xi,Xi1)|fk(1)(θ,θ0)|=i=1nk=1mEMk(1)(Xi,Xi1)|fk(1)(θ,θ0)|. (A35)

Since Mk(1)’s are bounded there exists a constant Q so that,

K(Pθ0(n),Pθ(n))ρn(dθ)Qi=1nk=1m|fk(1)(θ,θ0)|ρn(dθ)=Qnk=1m|fk(1)(θ,θ0)|ρn(dθ).

By Assumption 19 in Assumption 1, it follows that

K(Pθ0(n),Pθ(n))ρn(dθ)Qnk=1mCn=nmQCn=nϵn(1),

for some ϵn(1)=O(1n).

Part 2: Verifying condition (ii) of Corollary 1: As in the previous part, Z0=0, implying that Dθ,θ0. Applying Proposition 3 and integrating with respect to ρn, we obtain

Varrn(θ,θ0)ρn(dθ)i=1n4n+2nδ/2Cθ0,θ(i)ρn(dθ)αi1δ/(2+δ)+i,j=1n4n+2nδ/2(Cθ0,θ(i)ρn(dθ)+Cθ0,θ(j)ρn(dθ)+Cθ0,θ(i)Cθ0,θ(j)ρn(dθ))×α|ij|1δ/(2+δ). (A36)

First, consider the term Cθ0,θ(i)ρn(dθ). Using Assumption 1, we can upper bound Cθ0,θ(i) as,

Cθ0,θ(i)Ek=1mMk(1)(Xi,Xi1)|fk(1)(θ,θ0)|2+δk=1mm1+δEMk(1)(Xi,Xi1)|fk(1)(θ,θ0)|2+δ(byJensensinequality)=k=1mm1+δEMk(1)(Xi,Xi1)2+δ|fk(1)(θ,θ0)|2+δ.

Since Mk(1)’s are upper bounded by Q, it follows from the previous expression that, Cθ0,θ(i)k=1mm1+δQ2+δ|fk(1)(θ,θ0)|2+δ.

Hence, from Assumption 1, we get,

Cθ0,θ(i)ρn(dθ)k=1mm1+δQ2+δ|fk(1)(θ,θ0)|2+δρn(dθ)(mQ)2+δCn.

Using the upper bound above, we can say for an L large enough, Cθ0,θ(i)ρn(dθ)Ln. Next, by the Cauchy-Schwarz inequality, we have that Cθ0,θ(i)Cθ0,θ(j)ρn(dθ))<Cθ0,θ(i)ρn(dθ)Cθ0,θ(j)ρn(dθ))Ln. Thus, we have the following upper bound.

Varrn(θ,θ0)ρn(dθ)i=1n4n+2nδ/2Lnαi1δ/(2+δ)+i,j=1n4n+2nδ/2(Ln+Ln+Ln)α|ij|1δ/(2+δ)=4n+2nδ/2Lni=1nαi1δ/(2+δ)+4n+6nδ/2Lni,j=1nα|ij|1δ/(2+δ).

Since i,j=1nα|ij|1δ/(2+δ)<nk1αk1δ/(2+δ)<, we have that for some ϵn(2)=O(nδ/2n),

Varrn(θ,θ0)ρn(dθ)<nϵn(2).

Since K(ρn,π)nC, following the concluding argument in Theorem 2 completes the proof. □

Appendix B.3.2. Proof of Proposition 8

We verify Assumption 1 and the proof follows from Theorem 3. For i{1,2,,K1},

pθ(j|i)=θifj=i1,1θifj=i+1.

If i=0 or i=K, then the Markov chain goes back to 1 or K1, respectively, with probability 1. With the convention log00=0, the log ratio of the transition probabilities becomes,

|logpθ0(X1|X0)logpθ(X1|X0)|=I[X1=X0+1]logθ0θ+I[X1=X01]log1θ01θ.

In this case, m=2. M1(1)(X1,X0)=I[X1=X0+1] and M2(1)(X1,X0)=I[X1=X01], both of which are bounded. Let f1(1)(θ,θ0):=logθ0θ suppose f2(1)(θ,θ0):=log1θ01θ.

The stationary distribution qθ(i)=1Ki1,2,,K. Hence the log of the ratio of the invariant distribution becomes

logq0(x)logqθ(x)=0, (A37)

and we can set Mi(2)(·):=1 and fi(2)(·,·):=0 for i{1,2}. Thus, to prove the concentration bound for this Markov chain it is enough to assume that δ=1 and show that [f1(1)(θ,θ0)]3ρn(dθ)<Cn and [f2(1)(θ,θ0)]3ρn(dθ)<Cn for some constant C>0.

As given, {ρn} is a sequence of beta probability distribution functions, with parameters an,bn that satisfy the constraint anan+bn=θ0. Specifically, we choose an=nθ0 and (therefore) bn=n(1θ0). Thus, we get the following,

|f1(1)(θ,θ0)|3ρn(dθ)=logθ0θ3ρn(dθ)<θ0θ13ρn(dθ)=1Beta(an,bn)01θ0θθ3θan1(1θ)bn1dθ.

Since θ0,θ(0,1), so is |θ0θ|2, giving |θ0θ|3<2(θ0θ)2. We use that fact to arrive at

|f1(1)(θ,θ0)|3ρn(dθ)2Beta(an,bn)01(θ0θ)2θan4(1θ)bn1dθ=2Beta(an3,bn)Beta(an,bn)(an3)(bn)(an+bn3)2(an+bn2).

From our choice of an and bn, 2Beta(an3,bn)Beta(an,bn)=O(1), and plugging the values of an and bn into (an3)(bn)(an+bn3)2(an+bn2), we get (an3)(bn)(an+bn3)2(an+bn2)=1n(θ03n)(1θ0)(13n)2(12n), which is upper bounded by C1n for some constant C1>0. Hence,

|f1(1)(θ,θ0)|3ρn(dθ)<C1n.

Similarly, we can also show that,

|f2(1)(θ,θ0)|3ρn(dθ)<C2n.

Finally, from Proposition A.2.1, we get that K(ρn,π)<C+12log(n) for some large constant C. Hence, K(ρn,π)<C3n for some constant C3>0. Choosing C=max(C1,C2,C3), we satisfy all the conditions of Assumption 1 and Theorem 3. □

Appendix B.3.3. Proof of Proposition 9

For the purpose of this proof, we choose ρn’s with scaled Beta distribution with parameters an=n(θ0/2) and bn=n(1θ0/2). Since, ρn is a scaled Beta distribution with the scaling factors m=0.5 and c=0, the pdf of ρn is given by

ρn(θ)=2Beta(an,bn)2θan12θbn

Since this is a scaled distribution, Eρn[θ]=2anan+bn=θ0 and there exists a constant σ>0, Varρn[θ]=σ2n. Now, we analyse the transition probabilities. For i{1,2,}, the Birth-Death process has transition probabilities

pθ(j|i)=θifj=i1,1θifj=i+1.

If i=0, then the Markov chain goes to 1 with probability 1. Hence with the convention log00=0 the ratio of the log of the transition probabilities becomes,

|logpθ0(X1|X0)logpθ(X1|X0)|=I[X1=X0+1]logθ0θ+I[X1=X01]log1θ01θ.

In this case, m=3. M1(1)(X1,X0)=I[X1=X0+1] and M2(1)(X1,X0)=I[X1=X01]. Define M3(1)(X1,X0):=1. All these random variables are bounded. Define f1(1)(θ,θ0):=logθ0θ,f2(1)(θ,θ0):=log1θ01θ and f3(1)(θ,θ0):=0. Similarly as in the proof on Proposition 8,

[f1(1)(θ,θ0)]3ρn(dθ)<C1n,and[f2(1)(θ,θ0)]3ρn(dθ)<C2n.

The stationary distribution is given by qθ(i)=(θ1θ)i1qθ(1)i1,2,, so that qθ(i)=(1θ)(θ1θ)i1 Hence the log of the ratio of the invariant distribution becomes

logq0(i)logqθ(i)=log1θ01θ+(i1)logθ0θ(i1)log1θ01θ (A38)

We define M1(2)(X0):=1, and M2(2)(X0)=M3(2)(X0):=X01. We can write Eq(0)[M2(2)(X0)]2=i=1(i1)2q(0)(i)<i=1i2q(0)(i). We have chosen q(0) such that i=1i2q(0)(i) is bounded. Hence, Eq(0)[M2(2)(X0)]2<. To verify Assumption i define, f1(2)(θ,θ0)=f3(2)(θ,θ0):=log1θ01θ, and define f2(2)(θ,θ0):=logθ0θ. Therefore following the proof of Proposition 8,

|f1(2)(θ,θ0)|3ρn(dθ)=|f3(2)(θ,θ0)|3ρn(dθ)=|f2(1)(θ,θ0)|3ρn(dθ)<C2n,and,|f2(2)(θ,θ0)|3ρn(dθ)=|f1(1)(θ,θ0)|3ρn(dθ)<C1n.

Finally, we take the KL-divergence K(ρn,π). ρn follows a scaled Beta distribution on (0,1/2) with parameters an=n(θ0/2) and bn=n(1θ0/2), while π follows a scaled Beta distribution on (0,1/2) with parameters a and b. Thus,

K(ρn,π)=012logρn(θ)π(θ)ρn(dθ),

which, by substituting t=2θ, we get,

K(ρn,π)=201logρn(t)π(t)ρn(dt).

01logρn(t)π(t)ρn(dt) is the KL-divergence between a Beta distribution with parameters an and bn and a Beta distribution with parameters a and b. An application of Proposition A.2.1 gives us for a constant C1>0,

01logρn(t)π(t)ρn(dt)<C1+12log(n).

Hence we can say, K(ρn,π)<2C1+12log(n). Thus, we now get that for some constant C3>0,

K(ρn,π)<C3n.

Choosing C=max(C1,C2,C3) we satisfy all of the conditions of Assumption 1 and thus by Theorem 3, we are complete the proof. □

Appendix B.3.4. Proof of Theorem 4

Part 1: Verifying condition (i) of Corollary 1 As in the proof of Theorem 2 substitute the true parameter θ0 for θ1 and θ for θ2. We also set our initial distributions q1(0) and q2(0) to the known initial distribution q(0). A method similar to Equation (A35), yields

K(Pθ0(n),Pθ(n))i=1nk=1mEMk(1)(Xi,Xi1)|fk(1)(θ,θ0)|.

Because Mk(1)s satisfy Assumption 2, it follows by the application of Theorem 2.3, [21] that λ>0 such that for any 0<κλ, and for some ζ(0,1) possibly depending upon λ,

EeκMk(1)(Xi,Xi1)X1,X0]ζi1eκMk(1)(X1,X0)+1ζi1ζDeκaforalli>1.

We rewrite EMk(1)(Xi,Xi1)|X1,X0 as follows:

EMk(1)(Xi,Xi1)|X1,X0=E[κMk(1)(Xi,Xi1)|X1,X0]κE[eκMk(1)(Xi,Xi1)|X1,X0]κ.

Therefore, i=1nEMk(1)(Xi,Xi1) can be upper bounded as,

i=1nEMk(1)(Xi,Xi1)=i=1nEκMk(1)(Xi,Xi1)|X1,X0κ1i=1nζi1EeκMk(1)(X1,X0)+1ζi1ζDeκaκ1.

Since, ζ(0,1), ζi<1. Hence, we can write that,

i=1nζi1EeκMk(1)(X1,X0)+1ζi1ζDeκaκ1i=1nζi1EeκMk(1)(X1,X0)+11ζDeκaκ1=1ζn1ζEeκMk(1)(X1,X0)+n1ζDeκaκ1nL,

for a large constant L. Therefore K(Pθ0(n),Pθ(n))ρn(dθ) can be upper bounded as follows,

K(Pθ0(n),Pθ(n))ρn(dθ)k=1mnL|fk(1)(θ,θ0)|ρn(dθ)=k=1mnL|fk(1)(θ,θ0)|ρn(dθ).

By Assumption 1, |fk(1)(θ,θ0)|ρn(dθ)<Cn, hence,

K(Pθ0(n),Pθ(n))ρn(dθ)nLCn.

Hence, for some ϵn(1)=O(1n), we have obtained that, K(Pθ0(n),Pθ(n))ρn(dθ)nϵn(1).

Part 2: Verifying condition (ii) of Corollary 1: Similar to as in the proof of Theorem 3, we upper bound Varrn(θ,θ0)ρn(dθ) by

Varrn(θ,θ0)ρn(dθ)i,j=1n(4n+2nδ/2(Cθ0,θ(i)ρn(dθ)+Cθ0,θ(j)ρn(dθ) (A39)
+Cθ0,θ(i)Cθ0,θ(j)ρn(dθ)))α|ij|1δ/(2+δ)+i=1n4n+2nδ/2Cθ0,θ(i)ρn(dθ)αi1δ/(2+δ), (A40)

where Cθ0,θ is upper bounded as

Cθ0,θ(i)k=1mm1+δEMk(1)(Xi,Xi1)2+δ|fk(1)(θ,θ0)|2+δ.

There exists a constant Cδ depending upon δ such that,

[Mk(1)]2+δ(Xi,Xi1)=κ2+δ[Mk(1)]2+δ(Xi,Xi1)2+δκ2+δeκMk(1)(Xi,Xi1)+Cδκ2+δ.

By expressing EMk(1)(Xi,Xi1)2+δ=EEMk(1)(Xi,Xi1)2+δ|X1,X0 and following a method similar to the previous part, we get,

EMk(1)(Xi,Xi1)2+δζiEeκMk(1)(X1,X0)+1ζi1ζDeκa+Cδκ2+δ.

The fact that 0<ζ<1 implies that 0<ζi<ζ. This gives us the following,

EMk(1)(Xi,Xi1)2+δζEeκMk(1)(X1,X0)+11ζDeκa+Cδκ2+δ.

Since κ<λ, by the application of Jensen’s inequality, we get

EMk(1)(Xi,Xi1)2+δζEeλMk(1)(X1,X0)+11ζDeκa+Cδκ2+δ=ζeλMk(1)(x1,x0)pθ0(x1|x0)D(x0)dx1dx0+11ζDeκa+Cδκ2+δ.

We know that |fk(1)(θ,θ0)|2+δρn(dθ)<Cn. Thus, following Assumption 1 we can say that, for a large constant L, Cθ0,θ(i)ρn(dθ)Ln. The rest of the proof follows similarly as in the proof of Theorem 3, and we obtain an ϵn(2)=O(nδ/2n), such that,

Var[rn(θ,θ0)]ρn(dθ)<nϵn(2).

Since, K(ρn,π)nC, similar arguments as in the proof of Theorem 2 holds. The theorem is thus proved.

Appendix B.3.5. Proof of Theorem 5

Part 1: Verifying condition (i) of Corollary 1 As in the proof of Theorem 2 substitute the true parameter θ0 for θ1 and θ for θ2. We also set q1(0) and q2(0) to the known initial distribution q(0). Similar to the steps leading to Equation (A35), we get

K(Pθ0(n),Pθ(n))i=1nk=1mEMk(1)(Xi,Xi1)|fk(1)(θ,θ0)|.

Consider the term EMk(1)(Xi,Xi1). With qθ0(i1) the marginal distribution of Xi1, we have

EMk(1)(Xi,Xi1)=Mk(1)(xi,xi1)pθ0(xi|xi1)qθ0(i1)(xi1)dxidxi1.EMk(1)(Xi,Xi1)=Mk(1)(xi,xi1)pθ0(xi|xi1)pθ0i1(xi1|x0)qθ0(0)(x0)dx0dxidxi1

Recall that the marginal density satisfies qθ0(i1)(xi1)=pθ0i1(xi1|x0)qθ0(0)(x0)d(x0), where pθ0i(·|x0) is the i-step transition probability. Then

EMk(1)(Xi,Xi1)=EMk(1)(Xi,xi1)|xi1pθ0i1(xi1|x0)qθ0(0)(x0)dx0dxi1.

Since the Markov chain {Xn} satisfies Assumption A.1.1, we know by the application of Theorem A.1.1 that {Xn} is V-geometrically ergodic. Hence, τ<1, R< such that |f|<V

|f(xi1)pθ0i1(xi1|x0)dxi1f(xi1)qθ0(xi1)dxi1|<RV(x0)τi1,

where qθ0 is the stationary distribution, implying that

f(xi1)pθ0i1(xi1|x0)dxi1<f(xi1)qθ0(xi1)dxi1+RV(x0)τi1.

By the application of Jensen’s inequality we get EMk(1)(Xi,Xi1)|Xi12+δEMk(1)(Xi,Xi1)2+δ|Xi1<V(Xi1). Since V(·)1, it follows from the previous expression that EMk(1)(Xi,Xi1)|Xi1<V(Xi1)1/(2+δ)V(Xi1). Thus, setting f(x)=EMk(1)(Xi,Xi1)|Xi1=x, we obtain

EMk(1)(Xi,Xi1)<EMk(1)(Xi,Xi1)|Xi1qθ0(xi)dxi1+RV(x0)τi1q(0)(x0)dx0=E[Mk(1)(X1,X0)]+τi1RV(x0)q(0)(x0)dx0.

Summing from i=1 to n, we get

i=1nEMk(1)(xi,xi1)<nE[Mk(1)(X1,X0)]+i=1nτi1RV(x0)q(0)(x0)dx0
=nE[Mk(1)(X1,X0)]+1τn1τRV(x0)q(0)(x0)dx0.

This gives us the following bound on K(Pθ0(n),Pθ(n))ρn(dθ):

K(Pθ0(n),Pθ(n))ρn(dθ)k=1mnE[Mk(1)(X1,X0)]+1τn1τRV(x0)D(x0)dx0×|fk(1)(θ,θ0)|ρn(dθ).

By Assumption 1, |fk(1)(θ,θ0)|ρn(dθ)<Cn. Hence, we can rewrite the previous expression as

K(Pθ0(n),Pθ(n))ρn(dθ)k=1mnE[Mk(1)(X1,X0)]+1τn1τRV(x1)D(x1)dx1Cn=nmE[Mk(1)(X1,X0)]+1τnn(1τ)RV(x0)D(x0)dx0Cn.

Since, τ<1, 0<1τn<1, and we rewrite the previous equation as,

K(Pθ0(n),Pθ(n))ρn(dθ)nmE[Mk(1)(X1,X0)]+1n(1τ)RV(x0)D(x0)dx0Cn.

Hence, there exists an ϵn(1)=O(1n) such that K(Pθ0(n),Pθ(n))ρn(dθ)nϵn(1).

Part 2: Verifying condition (ii) of Corollary 1: Similar to as in the proof of Theorem 3, we upper bound Varrn(θ,θ0)ρn(dθ) by

Varrn(θ,θ0)ρn(dθ)i,j=1n(4n+2nδ/2(Cθ0,θ(i)ρn(dθ)+Cθ0,θ(j)ρn(dθ) (A41)
+Cθ0,θ(i)Cθ0,θ(j)ρn(dθ)))α|ij|1δ/(2+δ)+i=1n4n+2nδ/2Cθ0,θ(i)ρn(dθ)αi1δ/(2+δ), (A42)

where Cθ0,θ is upper bounded as

Cθ0,θ(i)k=1mm1+δEMk(1)(Xi,Xi1)2+δ|fk(1)(θ,θ0)|2+δ.

Since EMk(1)(Xi,Xi1)2+δ|Xi1<V(Xi1), by a similar application of V-geometric ergodicity, we can say that, 0<τ<1, such that

EMk(1)(Xi,Xi1)2+δnE[Mk(1)(X1,X0)]2+δ+τi1RV(x0)D(x0)dx0,

which, by the fact that τi1<τ, gives us,

EMk(1)(Xi,Xi1)2+δE[Mk(1)(X1,X0)]2+δ+τRV(x0)D(x0)dx0.

By Assumption 1, we know that, |fk(1)(θ,θ0)|2+δρn(dθ)<Cn. Hence, for a large constant L, Cθ0,θ(i)ρn(dθ)Ln. We also see that since the chain is geometrically ergodic, by the application of Equation (A4), k1αkδ/(2+δ)<+. The rest of the proof follows similarly as in the proof of Theorem 3, and we obtain an ϵn(2)=O(nδ/2n), such that,

Var[rn(θ,θ0)]ρn(dθ)<nϵn(2).

Since, K(ρn,π)nC, similar arguments as in the proof of Theorem 2 holds. The theorem is thus proved. □

Appendix B.3.6. Proof of Proposition 10

For the purpose of the proof, we choose ρn’s with scaled Beta distribution with parameters an=n1+θ02 and bn=n1θ02. Since, ρn is a scaled Beta distribution with the scaling factors m=2 and c=1, the pdf of ρn is given by

ρn(θ)=12Beta(an,bn)1+θ2an1θ2bn

Since this is a scaled distribution, Eρn[θ]=2anan+bn1=θ0 and there exists a constant σ>0, Varρn[θ]=σ2n. We now analyse the log-ratio of the transition probabilities for the Markov chain,

logpθ0(Xn|Xn1)logpθ(Xn|Xn1)=2XnXn1(θθ0)+Xn12(θ02θ2).

Observe that in this setting, M1(1)(Xn,Xn1)=|XnXn1| and M2(1)(Xn,Xn1)=Xn2. Next, using the fact that

E[|Xn|2+δ|Xn1]=E[|Xnθ0Xn1+θ0Xn1|2+δ|Xn1],

and by an application of triangle inequality, we obtain

E[|Xn|2+δ|Xn1]E|Xnθ0Xn1|+|θ0Xn1|2+δ|Xn1=E2|Xnθ0Xn1|+|θ0Xn1|22+δ|Xn1=E22+δ|Xnθ0Xn1|+|θ0Xn1|22+δ|Xn1.

Now by using Jensen’s inequality we get,

E[|Xn|2+δ|Xn1]E22+δ|Xnθ0Xn1|2+δ+|θ0Xn1|2+δ2|Xn1=21+δE|Xnθ0Xn1|2+δ|Xn1+21+δ|θ0Xn1|.

We know if YN(μ,σ2), then E|Yμ|p=σp2p2Γ(p+12)π. Consequently,

E[|Xn|2+δ|Xn1]21+δ22+δ2Γ(3+δ2)π+21+δ|θ0Xn1|2+δ. (A43)

It follows that,

E[M1(1)(Xn,Xn1)2+δ|Xn1]21+δ22+δ2Γ(3+δ2)π|Xn1|2+δ+21+δ|θ0|2+δ|Xn1|4+2δ21+δ22+δ2Γ(3+δ2)π+21+δ|θ0|2+δ(|Xn1|4+2δ+1).

Since θ0<1, we can say,

E[M1(1)(Xn,Xn1)2+δ|Xn1]21+δ22+δ2Γ(3+δ2)π+21+δ(|Xn1|4+2δ+1).

Define a constant Cδ:=21+δ22+δ2Γ(3+δ2)π+21+δ. The above term then becomes,

E[M1(1)(Xn,Xn1)2+δ|Xn1]Cδ(|Xn1|4+2δ+1).

Next we analyse the term M2(1)(Xn,Xn1).

EM2(1)(Xn,Xn1)2+δ|Xn1=E[Xn14+2δ|Xn1]=Xn14+2δCδ(Xn14+2δ+1).

Then, defining V(x):=Cδ(x4+2δ+1) it follows that,

EV(Xn)|Xn1=ECδ(Xn4+2δ+1)|Xn1.

Using a technique similar to Equation (A43) we get,

ECδ(Xn4+2δ+1)|Xn1Cδ(23+2δ24+2δ2Γ(5+2δ2)π+23+2δ|θ0Xn1|4+2δ+1).

Define another constant Cδ:=Cδ23+2δ24+2δ2Γ(5+2δ2)π23+2δ|θ0|4+2δ+1. Since δ>0, 24+2δ2Γ(5+2δ2)π>1. Furthermore, since |θ0|<1, so is |θ0|4+2δ. Hence,

23+2δ24+2δ2Γ(5+2δ2)π23+2δ|θ0|4+2δ>0.

Hence, we have shown that,

EV(Xn)|Xn1(23+2δ|θ0|4+2δ)Cδ(Xn14+2δ+1)+Cδ.

Since |θ0|<214+2δ1, 23+2δ|θ0|4+2δ<1, and we can express the above equation as,

EV(Xn)|Xn1V(Xn1)+Cδ.

Define the set C(m):={x:|x|4+2δ+1m}. From Proposition 11.4.2, [20], for a large enough m, C(m) forms a petite set. Thus, we have proved that V(x) as defined in this example satisfies Assumption A.1.1, and {Xn} is V-geometrically ergodic. The fj(1)’s corresponding to Assumption 1 are given by f1(1)(θ,θ0)=(θθ0) and f2(1)(θ,θ0)=(θ02θ2). Therefore, it follows that,

θf1(1)=1,θf2(1)=2θand2<2θ<2.

Since f1(1)(θ0,θ0)=f2(1)(θ0,θ0)=0, We just showed that they also have bounded partial derivatives. We also know that |θ|<1. Hence, by Proposition 4fj(1)’s satisfy the conditions of Assumption 1.

The invariant distribution for the simple linear model Markov-chain under parameter θ is given by a gaussian distribution with mean 0 and variance 11θ2. In other words,

qθ(x)=12πe1θ22x2.

Analyzing the log likelihood yields,

logq0(x)logqθ(x)=x22(1θ02)+x22(1θ2)=x22(θ02θ2).

Let f1(2)(θ0,θ0)=(θ02θ2) and f1(2)(θ0,θ0)=0. Since f1(2)(θ0,θ0)=f2(1)(θ0,θ0), by following arguments similar as before, can conclude that f1(2)(θ0,θ0) also satisfies the requirements of Assumption 1. Let M1(2)(x)=x22 and define M2(2)(x):=1. Let X0q1(0). As long as x4+2δq1(0)(x)dx<, we satisfy all the conditions required for Theorem 5. Finally we need to verify the condition that K(ρn,π)<Cn for some constant C>0. The KL-divergence logρn(θ)π(θ)ρn(dθ) becomes,

K(ρn,π)=11log12Beta(an,bn)1+θ2an1θ2bn×12Beta(an,bn)1+θ2an1θ2bndθ.

Substituting, y=1+θ2, we get,

K(ρn,π)=01log12Beta(an,bn)yan1ybn12Beta(an,bn)yan1ybndy=01log121Beta(an,bn)yan1ybndy+01log1Beta(an,bn)yan1ybn1Beta(an,bn)yan1ybn.

The first term integrates up to log(1/2). The second term is the KL-divergence between a Uniform and Beta distribution with parameters an=n1+θ02 and bn=n(11+θ02) and support [0,1]. Following Lemma A.2.1 it follows that K(ρn,π) is upper bounded by,

K(ρn,π)<log(1/2)+C1+12log(n)<Cn,

for some large constant C. This completes the proof. □

Appendix B.4. Proofs for Misspecified Models

Proof of Theorem 6

As in the proof of Theorem 1, following Equation (A13), we note that,

Dαre(Pθ(n),Pθ0(n))π˜n,αre|Xn(dθ)αre1αreK(Pθ0(n),Pθ(n))ρn(dθ)+αre1αreVar[rn(θ,θ0)ρn(dθ)]η+K(ρn,π)log(ϵ)1αre. (A44)

Following from Equations (23) and (26), we get that,

K(Pθ0(n),Pθ(n))ρn(dθ)E[rn(θ0,θn*)]+nϵn,

and

Var[rn(θ,θ0)]ρn(dθ)2nϵn+2Var[rn(θn*,θ0)].

Plugging these into Equation (A44), we are done. □

Author Contributions

Formal analysis, I.B.; Investigation, I.B.; Methodology, I.B., V.A.R. and H.H.; Resources, V.A.R. and H.H.; Validation, V.A.R. and H.H. All authors have read and agreed to the published version of the manuscript.

Funding

National Science Foundation: IIS-1816499; DMS-1812197.

Conflicts of Interest

The authors declare no conflict of interest.

Footnotes

Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

References

  • 1.Wainwright M.J., Jordan M.I. Introduction to Variational Methods for Graphical Models. Found. Trends Mach. Learn. 2008;1:1–103. doi: 10.1561/2200000001. [DOI] [Google Scholar]
  • 2.Bishop C.M. Pattern Recognition and Machine Learning. Springer; Berlin, Germany: 2006. [Google Scholar]
  • 3.Ormerod J.T., Wand M.P. Explaining variational approximations. Am. Stat. 2010;64:140–153. doi: 10.1198/tast.2010.09058. [DOI] [Google Scholar]
  • 4.Blei D.M., Kucukelbir A., McAuliffe J.D. Variational inference: A review for statisticians. J. Am. Stat. Assoc. 2017;112:859–877. doi: 10.1080/01621459.2017.1285773. [DOI] [Google Scholar]
  • 5.Jaiswal P., Rao V., Honnappa H. Asymptotic Consistency of α-Rényi-Approximate Posteriors. J. Mach. Learn. Res. 2020;21:1–42. [Google Scholar]
  • 6.Li Y., Turner R.E. Rényi divergence variational inference; Proceedings of the 30th Annual Conference on Neural Information Processing Systems; Barcelona, Spain. 5–10 December 2016; pp. 1073–1081. [Google Scholar]
  • 7.Dieng A.B., Tran D., Ranganath R., Paisley J., Blei D. Variational Inference via χ Upper Bound Minimization; Proceedings of the 31th Annual Conference on Neural Information Processing Systems; Long Beach, CA, USA. 4–9 December 2017. [Google Scholar]
  • 8.Wang Y., Blei D.M. Frequentist consistency of variational Bayes. J. Am. Stat. Assoc. 2019;114:1147–1161. doi: 10.1080/01621459.2018.1473776. [DOI] [Google Scholar]
  • 9.Zhang F., Gao C. Convergence rates of variational posterior distributions. Ann. Stat. 2020;48:2180–2207. doi: 10.1214/19-AOS1883. [DOI] [Google Scholar]
  • 10.Ghosal S., Ghosh J.K., Van Der Vaart A.W. Convergence rates of posterior distributions. Ann. Stat. 2000;28:500–531. doi: 10.1214/aos/1016218228. [DOI] [Google Scholar]
  • 11.Shen X., Wasserman L. Rates of convergence of posterior distributions. Ann. Stat. 2001;29:687–714. [Google Scholar]
  • 12.Rousseau J. On the frequentist properties of Bayesian nonparametric methods. Annu. Rev. Stat. Its Appl. 2016;3:211–231. doi: 10.1146/annurev-statistics-041715-033523. [DOI] [Google Scholar]
  • 13.Ghosal S., Van Der Vaart A.W. Entropies and rates of convergence for maximum likelihood and Bayes estimation for mixtures of Normal densities. Ann. Stat. 2001:1233–1263. [Google Scholar]
  • 14.Bhattacharya A., Pati D., Yang Y. Bayesian fractional posteriors. Ann. Stat. 2019;47:39–66. doi: 10.1214/18-AOS1712. [DOI] [Google Scholar]
  • 15.Alquier P., Ridgway J. Concentration of tempered posteriors and of their variational approximations. Ann. Stat. 2020;48:1475–1497. doi: 10.1214/19-AOS1855. [DOI] [Google Scholar]
  • 16.Yang Y., Pati D., Bhattacharya A. α-variational inference with statistical guarantees. Ann. Stat. 2020;48:886–905. doi: 10.1214/19-AOS1827. [DOI] [Google Scholar]
  • 17.Jaiswal P., Honnappa H., Rao V.A. Risk-sensitive variational Bayes: Formulations and bounds. arXiv. 20191903.05220 [Google Scholar]
  • 18.Bradley R.C. Basic Properties of Strong Mixing Conditions. A Survey and Some Open Questions. Probab. Surv. 2005;2:107–144. doi: 10.1214/154957805100000104. [DOI] [Google Scholar]
  • 19.Ibragimov I.A. Some limit theorems for stationary processes. Theory Probab Appl. 1962;7:349–382. doi: 10.1137/1107036. [DOI] [Google Scholar]
  • 20.Meyn S.P., Tweedie R.L. Markov Chains and Stochastic Stability. Springer; Berlin, Germany: 2012. [Google Scholar]
  • 21.Hajek B. Hitting-time and occupation-time bounds implied by drift analysis with applications. Adv. Appl. Probab. 1982:502–525. doi: 10.2307/1426671. [DOI] [Google Scholar]
  • 22.Birgé L. Specifying Statistical Models. Springer; Berlin, Germany: 1983. Robust testing for independent non identically distributed variables and Markov chains; pp. 134–162. [Google Scholar]
  • 23.Ryabko D. Testing statistical hypotheses about ergodic processes; Proceedings of the IEEE Region 8 International Conference on Computational Technologies in Electrical and Electronics Engineering; Novosibirsk, Russia. 21–25 July 2008. [Google Scholar]
  • 24.Lacoste-Julien S., Huszár F., Ghahramani Z. Approximate inference for the loss-calibrated Bayesian; Proceedings of the International Conference on Artificial Intelligence and Statistics; Ft. Lauderdale, FL, USA. 11–13 April 2011. [Google Scholar]
  • 25.Jaiswal P., Honnappa H., Rao V.A. Asymptotic consistency of loss-calibrated variational Bayes. Stat. 2020;9:e258. doi: 10.1002/sta4.258. [DOI] [Google Scholar]
  • 26.Jones G.L. On the Markov chain central limit theorem. Probab. Survey. 2004;1:299–320. doi: 10.1214/154957804100000051. [DOI] [Google Scholar]
  • 27.Alzer H. On some inequalities for the gamma and psi functions. Math. Comput. 1997;66:373–389. doi: 10.1090/S0025-5718-97-00807-7. [DOI] [Google Scholar]
  • 28.Donsker M.D., Varadhan S.S. Asymptotic evaluation of certain Markov process expectations for large time, I. Commun. Pure Appl. Math. 1975;28:1–47. doi: 10.1002/cpa.3160280102. [DOI] [Google Scholar]

Articles from Entropy are provided here courtesy of Multidisciplinary Digital Publishing Institute (MDPI)

RESOURCES