Optimal i.i.d. Berry–Esseen constant
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Let \(\Phi\) be the standard normal distribution function. For i.i.d. real-valued random variables \(X_1,\ldots,X_n\), define
\[
C_{\mathrm{BE}}=\sup_{\substack{n\ge1,\ X_1,\ldots,X_n\ \mathrm{i.i.d.}\\ \mathbf E X_1=0,\ \mathbf E X_1^2=1,\ 0<\rho:=\mathbf E|X_1|^3<\infty}}
\frac{\sqrt n}{\rho}\sup_{x\in\mathbb R}\left|\mathbf P\!\left\{\frac{X_1+\cdots+X_n}{\sqrt n}\le x\right\}-\Phi(x)\right|.
\]
Determine \(C_{\mathrm{BE}}\) exactly.Notes
The Berry–Esseen theorem quantifies the central limit theorem: for i.i.d. random variables with mean zero, unit variance, and finite third absolute moment , the Kolmogorov distance between the law of the normalized sum and the standard normal distribution is at most for an absolute constant . The problem asks for the exact value of the optimal constant in this i.i.d. setting. It goes back to Esseen's 1942 analysis of the error in Liapounoff's limit theorem [Esseen1942Fourier].
The two sides of the question have advanced very unevenly. Esseen's two-point distributions show , but whether this bound is sharp is not known. In the other direction, successive refinements of the Fourier-analytic method have brought the general i.i.d. upper bound down to the commonly quoted value [Shevtsova2013Absolute]; related nonuniform versions of the inequality have been sharpened as well [Pinelis2017Nonuniform].
The problem remains open: a full solution requires closing the gap between and , identifying the exact constant, and describing all extremizing distributions.
References (3)
- [Esseen1942Fourier]
On the Liapounoff Limit of Error in the Theory of Probability
Esseen, Carl-Gustav · 1942 · article
- [Shevtsova2013Absolute]
On the Absolute Constants in the Berry–Esseen Inequality and Its Structural and Nonuniform Improvements
Open ↗Shevtsova, Irina G. · 2013 · article
- [Pinelis2017Nonuniform]
On the Nonuniform Berry–Esseen Bound
Open ↗Pinelis, Iosif · 2017 · incollection
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