Convergence of measures

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In mathematics, more specifically measure theory, there are various notions of the convergence of measures. For an intuitive general sense of what is meant by convergence in measure, consider a sequence of measures μn on a space, sharing a common collection of measurable sets. Such a sequence might represent an attempt to construct 'better and better' approximations to a desired measure μ that is difficult to obtain directly. The meaning of 'better and better' is subject to all the usual caveats for taking limits; for any error tolerance ε > 0 we require there be N sufficiently large for nN to ensure the 'difference' between μn and μ is smaller than ε. Various notions of convergence specify precisely what the word 'difference' should mean in that description; these notions are not equivalent to one another, and vary in strength.

Three of the most common notions of convergence are described below.

Informal descriptions[edit]

This section attempts to provide a rough intuitive description of three notions of convergence, using terminology developed in calculus courses; this section is necessarily imprecise as well as inexact, and the reader should refer to the formal clarifications in subsequent sections. In particular, the descriptions here do not address the possibility that the measure of some sets could be infinite, or that the underlying space could exhibit pathological behavior, and additional technical assumptions are needed for some of the statements. The statements in this section are however all correct if \mu_n is a sequence of probability measures on a Polish space.

The various notions of convergence formalize the assertion that the 'average value' of each 'sufficiently nice' function should converge:

\int f\, d\mu_n \to \int f\, d\mu

To formalize this requires a careful specification of the set of functions under consideration and how uniform the convergence should be.

The notion of weak convergence requires this convergence to take place for every continuous bounded function f. This notion treats convergence for different functions f independently of one another, i.e. different functions f may require different values of Nn to be approximated equally well (thus, convergence is non-uniform in f).

The notion of strong convergence formalizes the assertion that the measure of each measurable set should converge:

\mu_n(A) \to \mu(A)

Again, no uniformity over the set A is required. Intuitively, considering integrals of 'nice' functions, this notion provides more uniformity than weak convergence. As a matter of fact, when considering sequences of measures with uniformly bounded variation on a Polish space, strong convergence implies the convergence \int f\, d\mu_n \to \int f\, d\mu for any bounded measurable function f. As before, this convergence is non-uniform in f

The notion of total variation convergence formalizes the assertion that the measure of all measurable sets should converge uniformly, i.e. for every \epsilon > 0 there exists N such that |\mu_n(A) - \mu(A)| < \epsilon for every n > N and for every measurable set A. As before, this implies convergence of integrals against bounded measurable functions, but this time convergence is uniform over all functions bounded by any fixed constant.

Total variation convergence of measures[edit]

This is the strongest notion of convergence shown on this page and is defined as follows. Let (X, \mathcal{F}) be a measurable space. The total variation distance between two (positive) measures μ and ν is then given by

 \left \|\mu- \nu \right \|_{TV} = \sup_f \left \{ \int_X fd\mu - \int_X fd\nu \right \}.

Here the supremum is taken over f ranging over the set of all measurable functions from X to [−1, 1]. This is in contrast, for example, to the Wasserstein metric, where the definition is of the same form, but the supremum is taken over f ranging over the set of measurable functions from X to [−1, 1] which have Lipschitz constant at most 1; and also in contrast to the Radon metric, where the supremum is taken over f ranging over the set of continuous functions from X to [−1, 1]. In the case where X is a Polish space, the total variation metric coincides with the Radon metric.

If μ and ν are both probability measures, then the total variation distance is also given by

\left \|\mu- \nu \right \|_{TV} = 2\cdot\sup_{A\in \mathcal{F}} | \mu (A) - \nu (A) |.

The equivalence between these two definitions can be seen as a particular case of the Monge-Kantorovich duality. From the two definitions above, it is clear that the total variation distance between probability measures is always between 0 and 2.

To illustrate the meaning of the total variation distance, consider the following thought experiment. Assume that we are given two probability measures μ and ν, as well as a random variable X. We know that X has law either μ or ν but we do not know which one of the two. Assume that these two measures have prior probabilities 0.5 each of being the true law of X. Assume now that we are given one single sample distributed according to the law of X and that we are then asked to guess which one of the two distributions describes that law. The quantity

{2+\|\mu-\nu\|_{TV} \over 4}

then provides a sharp upper bound on the prior probability that our guess will be correct.

Given the above definition of total variation distance, a sequence μn of measures defined on the same measure space is said to converge to a measure μ in total variation distance if for every ε > 0, there exists an N such that for all n > N, one has that[1]

\|\mu_n - \mu\|_{TV} < \epsilon.

Strong convergence of measures[edit]

For (X, \mathcal{F}) a measurable space, a sequence μn is said to converge strongly to a limit μ if

 \lim_{n \to \infty} \mu_n(A) = \mu(A)

for every set A\in\mathcal{F}.

For example, as a consequence of the Riemann–Lebesgue lemma, the sequence μn of measures on the interval [−1, 1] given by μn(dx) = (1+ sin(nx))dx converges strongly to Lebesgue measure, but it does not converge in total variation.

Weak convergence of measures[edit]

In mathematics and statistics, weak convergence (also known as narrow convergence or weak-* convergence, which is a more appropriate name from the point of view of functional analysis, but less frequently used) is one of many types of convergence relating to the convergence of measures. It depends on a topology on the underlying space and thus is not a purely measure theoretic notion.

There are several equivalent definitions of weak convergence of a sequence of measures, some of which are (apparently) more general than others. The equivalence of these conditions is sometimes known as the portemanteau theorem.[2]

Definition. Let S be a metric space with its Borel σ-algebra Σ. We say that a bounded sequence of positive finite measures Pn on (S, Σ), n = 1, 2, ..., converges weakly to the finite positive measure P, and write

P_n\Rightarrow P

if any of the following equivalent conditions is true (here En denotes expectation or the L1 norm with respect to Pn while E denotes expectation or the L1 norm with respect to P):

In the case S = R with its usual topology, if Fn, F denote the cumulative distribution functions of the measures Pn, P respectively, then Pn converges weakly to P if and only if limn→∞ Fn(x) = F(x) for all points xR at which F is continuous.

For example, the sequence where Pn is the Dirac measure located at 1/n converges weakly to the Dirac measure located at 0 (if we view these as measures on R with the usual topology), but it does not converge strongly. This is intuitively clear: we only know that 1/n is "close" to 0 because of the topology of R.

This definition of weak convergence can be extended for S any metrizable topological space. It also defines a weak topology on P(S), the set of all probability measures defined on (S, Σ). The weak topology is generated by the following basis of open sets:

\left\{ U_{\phi, x, \delta} \left| \begin{array}{c} \phi \colon S \to \mathbf{R} \text{ is bounded and continuous,} \\ x \in \mathbf{R} \text{ and } \delta > 0 \end{array} \right. \right\},

where

U_{\phi, x, \delta} := \left\{ \mu \in \boldsymbol{P}(S) \left| \left| \int_{S} \phi \mathrm{d} \mu - x \right| < \delta \right. \right\}.

If S is also separable, then P(S) is metrizable and separable, for example by the Lévy–Prokhorov metric, if S is also compact or Polish, so is P(S).

If S is separable, it naturally embeds into P(S) as the (closed) set of dirac measures, and its convex hull is dense.

There are many "arrow notations" for this kind of convergence: the most frequently used are P_{n} \Rightarrow P, P_{n} \rightharpoonup P and P_{n} \xrightarrow{\mathcal{D}} P..

Weak convergence of random variables[edit]

Let (\Omega, \mathcal{F}, \mathbb{P}) be a probability space and X be a metric space. If Xn, X: Ω → X is a sequence of random variables then Xn is said to converge weakly (or in distribution or in law) to X as n → ∞ if the sequence of pushforward measures (Xn)(P) converges weakly to X(P) in the sense of weak convergence of measures on X, as defined above.

References[edit]

  1. ^ Madras, Neil; Sezer, Deniz (25 Feb 2011). "Quantitative bounds for Markov chain convergence: Wasserstein and total variation distances". arxiv. Retrieved 21 July 2012. 
  2. ^ Klenke, Achim (2006). Probability Theory. Springer-Verlag. ISBN 978-1-84800-047-6. 
  • Ambrosio, L., Gigli, N. & Savaré, G. (2005). Gradient Flows in Metric Spaces and in the Space of Probability Measures. Basel: ETH Zürich, Birkhäuser Verlag. ISBN 3-7643-2428-7. 
  • Billingsley, Patrick (1995). Probability and Measure. New York, NY: John Wiley & Sons, Inc. ISBN 0-471-00710-2. 
  • Billingsley, Patrick (1999). Convergence of Probability Measures. New York, NY: John Wiley & Sons, Inc. ISBN 0-471-19745-9. 

See also[edit]