Berry–Esseen theorem explained

In probability theory, the central limit theorem states that, under certain circumstances, the probability distribution of the scaled mean of a random sample converges to a normal distribution as the sample size increases to infinity. Under stronger assumptions, the Berry–Esseen theorem, or Berry–Esseen inequality, gives a more quantitative result, because it also specifies the rate at which this convergence takes place by giving a bound on the maximal error of approximation between the normal distribution and the true distribution of the scaled sample mean. The approximation is measured by the Kolmogorov–Smirnov distance. In the case of independent samples, the convergence rate is, where is the sample size, and the constant is estimated in terms of the third absolute normalized moment.

Statement of the theorem

Statements of the theorem vary, as it was independently discovered by two mathematicians, Andrew C. Berry (in 1941) and Carl-Gustav Esseen (1942), who then, along with other authors, refined it repeatedly over subsequent decades.

Identically distributed summands

One version, sacrificing generality somewhat for the sake of clarity, is the following:

There exists a positive constant C such that if X₁, X₂, ..., are i.i.d. random variables with E(X₁) = 0, E(X₁²) = σ² > 0, and E(|X₁|³) = ρ < ∞,^[1] and if we define

Y _{n} = {X _{1} + X _{2} + … + X _{n} \over n}

the sample mean, with F_n the cumulative distribution function of

{Y _{n} \sqrt{n} \over {\sigma}},

and Φ the cumulative distribution function of the standard normal distribution, then for all x and n,

\left|F _{n(x)} - \Phi(x)\right| \le {C \rho \over \sigma ^{3\sqrt{n}}. (1)}

That is: given a sequence of independent and identically distributed random variables, each having mean zero and positive variance, if additionally the third absolute moment is finite, then the cumulative distribution functions of the standardized sample mean and the standard normal distribution differ (vertically, on a graph) by no more than the specified amount. Note that the approximation error for all n (and hence the limiting rate of convergence for indefinite n sufficiently large) is bounded by the order of n^−1/2.

Calculated upper bounds on the constant C have decreased markedly over the years, from the original value of 7.59 by Esseen in 1942.^[2] The estimate C < 0.4748 follows from the inequality

\sup _{x\inR} \left|F _{n(x)} - \Phi(x)\right| \le { 0 . 33554 (\rho +0 . 415 \sigma ^{3)\over} \sigma ^{3\sqrt{n}},} since σ³ ≤ ρ and 0.33554 · 1.415 < 0.4748. However, if ρ ≥ 1.286σ³, then the estimate \sup _{x\inR} \left|F _{n(x)} - \Phi(x)\right| \le { 0 . 3328 (\rho +0 . 429 \sigma ^{3)\over} \sigma ^{3\sqrt{n}},} is even tighter.

proved that the constant also satisfies the lower bound

C\geq (\sqrt{ 10)/(+3 }{ 6 \sqrt{ 2 \pi}}) ≈ 0 . 40973 ≈ (1)/(\sqrt{ 2 \pi) } + 0.01079 .

Non-identically distributed summands

Let X₁, X₂, ..., be independent random variables with E(X_i) = 0, E(X_i²) = σ_i² > 0, and E(|X_i|³) = ρ_i < ∞. Also, let

S _{n} = {X _{1} + X _{2} + … + X _{n} \over \sqrt{\sigma ^{2 }} _{n} }

be the normalized n-th partial sum. Denote F_n the cdf of S_n, and Φ the cdf of the standard normal distribution. For the sake of convenience denote

\vec{\sigma} = (\sigma _{1,\ldots,\sigma} _{n), \vec{\rho}=(\rho} _{1,\ldots,\rho} _{n).}

In 1941, Andrew C. Berry proved that for all n there exists an absolute constant C₁ such that

\sup _{x\inR} \left|F _{n(x)} - \Phi(x)\right| \le C _{1 ⋅ \psi} _{1, (2)}

where

\psi _{1=\psi} _{1(\vec{\sigma},\vec{\rho})=({style\sum\limits} ^{2 } )} ^{i} ^{-1/2} ⋅ max _{1\le i\le} (\rho _{i})/(\sigma ^{2} _{i}) .

Independently, in 1942, Carl-Gustav Esseen proved that for all n there exists an absolute constant C₀ such that

\sup _{x\inR} \left|F _{n(x)} - \Phi(x)\right| \le C _{0 ⋅ \psi} _{0,} ( 3 )

where

\psi _{0=\psi} _{0(\vec{\sigma},\vec{\rho})=({style\sum\limits} ^{2 } )} ^{i} ^{-3/2} ⋅ \sum\limits ^{n\rho} _{i.}

It is easy to make sure that ψ₀≤ψ₁. Due to this circumstance inequality (3) is conventionally called the Berry–Esseen inequality, and the quantity ψ₀ is called the Lyapunov fraction of the third order. Moreover, in the case where the summands X₁, ..., X_n have identical distributions

\psi _{0=\psi} ^{1= (\rho _{1})/(\sigma ^{3 \sqrt{n} _{1})} },and thus the bounds stated by inequalities (1), (2) and (3) coincide apart from the constant.

Regarding C₀, obviously, the lower bound established by remains valid:

C _{0 \geq (\sqrt{ 10)/(+3 }{ 6 \sqrt{ 2 \pi}})} = 0 . 4097 \ldots.

The lower bound is exactly reached only for certain Bernoulli distributions (see for their explicit expressions).

The upper bounds for C₀ were subsequently lowered from Esseen's original estimate 7.59 to 0.5600.^[3]

Multidimensional version

As with the multidimensional central limit theorem, there is a multidimensional version of the Berry–Esseen theorem.^[4]

Let

X _{1,...,X} _{n} be independent R ^{d} -valued random vectors each having mean zero. Write S _{n} = \sum ^{n} _{i =1} X _{i} and assume \Sigma _{n} = \operatorname{Cov}[S _{n]} is invertible. Let Z _{n\sim\operatorname{N}(0,{\Sigma} _{n})} be a d -dimensional Gaussian with the same mean and covariance matrix as S _{n} . Then for all convex sets U\subseteq R ^{d} ,| \Pr[S _{n\in} U] - \Pr[Z _{n\in} U] | \le C d ^{1/4} \gamma _{n} ,where C is a universal constant and \gamma _{n=\sum} ^{n} ^{i =1} \operatorname{E} [ \|\Sigma ^{-1 / 2} _{n} X _{i\|} ^{3 ]} ^{2} (the third power of the L² norm).

The dependency on

d ^{1/4} is conjectured to be optimal, but might not be.^[5]

See also

• Chernoff's inequality
• Edgeworth series
• List of inequalities
• List of mathematical theorems
• Concentration inequality

Notes

1. Since the random variables are identically distributed, X₂, X₃, ... all have the same moments as X₁.
2. . For improvements see,,,,,, . The detailed review can be found in the papers and .

3. ; ; ; ; ; .

4. Bentkus, Vidmantas. "A Lyapunov-type bound in R^d." Theory of Probability & Its Applications 49.2 (2005): 311–323.
5. Raič. Martin. 2019. A multivariate Berry--Esseen theorem with explicit constants. Bernoulli. 25. 4A. 2824–2853. 10.3150/18-BEJ1072. 1350-7265. 1802.06475. 119607520.

Bibliography

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• Durrett, Richard (1991). Probability: Theory and Examples. Pacific Grove, CA: Wadsworth & Brooks/Cole. .
• Esseen . Carl-Gustav . On the Liapunoff limit of error in the theory of probability . 1942 . Arkiv för Matematik, Astronomi och Fysik . 0365-4133 . A28 . 1–19 .
• Esseen . Carl-Gustav . A moment inequality with an application to the central limit theorem . 1956 . Skand. Aktuarietidskr. . 39 . 160–170 .
• Feller, William (1972). An Introduction to Probability Theory and Its Applications, Volume II (2nd ed.). New York: John Wiley & Sons. .
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• Serfling, Robert J. (1980). Approximation Theorems of Mathematical Statistics. New York: John Wiley & Sons. .
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• Shevtsova . Irina . An Improvement of Convergence Rate Estimates in the Lyapunov Theorem . 2010 . Doklady Mathematics . 82 . 3 . 862–864 . 10.1134/S1064562410060062 . 122973032 .
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• Tyurin . I.S. . An improvement of upper estimates of the constants in the Lyapunov theorem . 2010 . Russian Mathematical Surveys . 65 . 3(393) . 201–202 . 10.1070/RM2010v065n03ABEH004688 . 118771013 .
• van Beek . P. . An application of Fourier methods to the problem of sharpening the Berry–Esseen inequality . 1972 . Zeitschrift für Wahrscheinlichkeitstheorie und Verwandte Gebiete . 23 . 187–196 . 10.1007/BF00536558 . 3 . 121036017 . free .
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External links

• Gut, Allan & Holst Lars. Carl-Gustav Esseen, retrieved Mar. 15, 2004.