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Berry–Esseen Error Control Methods

Updated 30 January 2026
  • Berry–Esseen error control is a quantitative method that bounds the deviation between normalized sums and the Gaussian distribution using explicit moment-based rates.
  • It extends classical results to structured, high-dimensional, and dependent models, providing practical error rates for statistical inference and information theory applications.
  • The framework applies to conditioned random walks, U-statistics, and self-normalized sums, enabling finite-sample accuracy and rigorous performance guarantees.

Berry–Esseen error control refers to the quantitative bounding of the deviation between the distribution of a properly normalized sum (or functional) of random variables and its limiting law—typically Gaussian—via explicit rates and constants. This control is achieved through the Berry–Esseen theorem and its extensions, which quantify how close the distribution function of a sum of (possibly dependent or structured) random variables lies to the normal distribution, in terms of moments, dependence parameters, and model-specific quantities. Berry–Esseen-type bounds are central to both classical and modern probability, enabling non-asymptotic precision in hypothesis testing, information theory, statistical estimation, and applied stochastic models.

1. Classical Berry–Esseen Theorem and Extension to Structured Models

The classical Berry–Esseen theorem asserts that for independent, zero-mean, finite third-moment random variables i\ell_i, the normalized sum Sn=i=1niS_n = \sum_{i=1}^n \ell_i satisfies

P{Snnμ2<τ}Φ(τ)ωμ3μ2nμ2,\left|\mathbb{P}\left\{\frac{S_n}{\sqrt{n\,\mu_2}} < \tau\right\} - \Phi(\tau)\right| \leq \omega \frac{\mu_3}{\mu_2 \sqrt{n \mu_2}},

where μ2=1nE[i2]\mu_2 = \frac{1}{n} \sum E[\ell_i^2], μ3=1nE[i3]\mu_3 = \frac{1}{n} \sum E[|\ell_i|^3], Φ\Phi is the standard normal cdf, and ω0.5600\omega\leq 0.5600 is universal (Nakiboglu, 2019). This bound controls the approximation error to within O(n12)O(n^{-\frac{1}{2}}), and the leading constant depends on the ratio of third to second moments.

The approach extends to structured models—such as self-normalized sums, UU-statistics, Poisson functionals, permutation statistics, locally dependent or conditioned variables—by replacing classical independence and moment assumptions with appropriate generalized moments, exchangeable-pair frameworks, dependency graphs, or entropy/density controls. In each case, explicit Berry–Esseen bounds quantify how the error scales with system size, dimensionality, and model-specific complexity.

2. Berry–Esseen Error Control in Information Theory: Refined Sphere Packing Bound

The refined sphere-packing bound (RSPB) exemplifies Berry–Esseen error control in information theory (Nakiboglu, 2019). Given a channel family (e.g., Gaussian, Rényi-symmetric, DMC), it provides a tight converse for codeword error probability Pe(n)P_e^{(n)} as

Pe(n)Δ(R)n0.5(1Esp(R))exp(nEsp(R)),P_{e}^{(n)} \geq \Delta(R) n^{-0.5(1-E_{sp}'(R))} \exp(-n E_{sp}(R)),

where Esp(R)E_{sp}(R) is the sphere-packing exponent, Esp(R)E_{sp}'(R) is its derivative w.r.t. rate RR, and Δ(R)\Delta(R) is explicit via Berry–Esseen constants and channel/Augustin parameters. The key is to apply Berry–Esseen to the sum of log-likelihood increments i\ell_i under a tilted measure derived from the Augustin center. The symmetry hypothesis (Rényi-symmetry) ensures the increments are i.i.d. under tilt, allowing Lemma 2 (Berry–Esseen) to give the O(n12(1Esp(R)))O(n^{-\frac{1}{2}(1-E_{sp}'(R))}) prefactor in the exponential bound.

3. Conditional and Structured Berry–Esseen Bounds

For complex conditioning structures—such as random walks conditioned to stay positive, permutation statistics, sum-of-YY statistics given auxiliary constraints—Berry–Esseen error control must account for the delicate dependence relationships and altered limiting laws.

  • Conditioned random walks: For i.i.d. increments with EX1=0E X_1=0, Var(X1)=σ2Var(X_1)=\sigma^2, EX13<E|X_1|^3<\infty, the conditional law Snσn{τ>n}\frac{S_n}{\sigma \sqrt{n}} \mid \{\tau>n\} converges to Rayleigh, and the Berry–Esseen rate is O(n1/2)O(n^{-1/2}) with error constant depending on (EX13/σ3)3(E|X_1|^3/\sigma^3)^3 (Denisov et al., 2024). Exit-time decompositions, convolution remainder bounds, and density concentration control the error.
  • Stratified permutation statistics: Stein’s method via zero-bias coupling yields

suptP{Wt}Φ(t)c(k=1Ki,j[k]aijs3[k])1/2\sup_t |\mathbb{P}\{W \le t\} - \Phi(t)| \le c \left(\sum_{k=1}^K \sum_{i,j \in [k]} \frac{|a_{ij}^s|^3}{[k]}\right)^{1/2}

or, under sufficient stratum size and variance conditions, an optimal O(n1/2)O(n^{-1/2}) rate (Tian et al., 18 Mar 2025).

  • Conditional sum statistics: For Un=i=1NnYn,iXn,i=mnU_n = \sum_{i=1}^{N_n} Y_{n,i} \mid \sum X_{n,i} = m_n, the Berry–Esseen bound is O(Nn1/2)O(N_n^{-1/2}) under variance, third-moment, local limit, and smoothing conditions (Klein et al., 2019).

4. Berry–Esseen Bounds in High-Dimensional, Dependent, and Self-Normalized Settings

Error control extends to high-dimensional and dependent structures:

  • High-dimensional mm-dependent sums: For locally dependent XiRpX_i \in \R^p,

μ(Sn,Z)C(n/m)1/2polylog(n,p)\mu(S_n, Z) \leq C(n/m)^{-1/2} \mathrm{polylog}(n, p)

over all axis-parallel rectangles, provided uniform covariance lower bounds and third moments (Bong et al., 2022).

  • Self-normalized sums: For T=S/VT = S/V (Student statistic), explicit Berry–Esseen bounds of the form

$|\mathbb{P}\{T \le z\} - \Phi(z)| \le A_3\frac{_3}{_2^{3/2}} + A_4\frac{_4'^{1/2}}{_2} + A_6\frac{_6'}{_3^3 _2^{3/2}}$

hold with constants A3,A4,A6A_3, A_4, A_6 optimized for various distribution classes (Pinelis, 2011). For local dependency structures (m-dependence, graph dependency), the error rate is modulated by local parameters and truncation levels (Zhang, 2021).

  • Non-normal approximations and exchangeable pairs: The general exchangeable-pair bound is

supzP{Wz}Φ(z)E112λE[Δ2W]+1λEE[ΔΔW]+ER\sup_z |\mathbb{P}\{W \le z\} - \Phi(z)| \le E\left|1 - \frac{1}{2\lambda} E[\Delta^2 | W]\right| + \frac{1}{\lambda} E|E[\Delta \Delta^* | W]| + E|R|

where Δ=WW\Delta = W - W', λ\lambda is regression constant, and Δ\Delta^* is a majorant (Shao et al., 2017). This framework yields optimal rates under mild conditions even without bounded differences, extends to non-Gaussian targets, and applies to quadratic forms, Curie–Weiss models, graph colorings, and more.

5. Berry–Esseen Control in Non-Classical, Multivariate, and Functional Settings

For expansions, local limit theorems, high-dimensional and functional approximations:

  • Non-uniform Berry–Esseen: Smoothing inequalities and filters yield bounds that scale optimally in the moderate-deviation regime, achieving smaller constants for nonuniform bounds (Pinelis, 2013).
  • Entropic and total variation bounds: When summands possess finite entropic distance, Berry–Esseen error control extends to total variation and relative entropy: FnΦTVC(D)L3,D(SnZ)C(D)L4\|F_n - \Phi\|_{TV} \le C(D) L_3,\quad D(S_n \| Z) \le C'(D) L_4 with C(D)C(D) exponential in single-summand entropies (Bobkov et al., 2011).
  • Multivariate and geometric bounds: Berry–Esseen-type bounds are established for multivariate sums and central limit theorems for dynamical systems, with rates O(N1/2)O(N^{-1/2}) under covariance linear growth, explicit smoothing via Bentkus’s lemma, and control over non-stationarity/expansion parameters (Leppänen, 2024). For densities, local limit Berry–Esseen analogues provide

supxpn(x)φ(x)CL3+CdM2ecnmin(σ2/L32,1)\sup_x |p_n(x) - \varphi(x)| \le C L_3 + C_d M^2 e^{-c n \min(\sigma^2 / L_3^2, 1)}

with L3L_3 as Lyapunov ratio, MM maximal density, and exponential smoothing (Bobkov et al., 2024).

  • Higher-order and bootstrap accuracy: If KKth-moment matching is enforced, higher-order Berry–Esseen bounds yield sharper rates, e.g.

supBballP(SnB)P(S~nB)CK[Cz,LKE(XiK+YiK)]1/(K+1)nK/[2(K+1)]\sup_{B\,\text{ball}} |P(S_n \in B) - P(\tilde S_n \in B)| \le C_K [C_{z,L}^K \sum E(\|X_i\|^K + \|Y_i\|^K)]^{1/(K+1)} n^{-K/[2(K+1)]}

which directly improves bootstrap quantile approximation and normal approximation in high dimensions (Zhilova, 2016).

6. Applications and Domain-Specific Instantiations

Error control via Berry–Esseen bounds is now embedded in a range of applied probabilistic and statistical areas:

  • Information theory: Determination of non-asymptotic converse bounds for channel coding under symmetry—AWGN, DMC, and Rényi-symmetric channels (Nakiboglu, 2019).
  • Combinatorics: Precise normal approximation for subgraph counts in random graphs and permutations; kernel-based goodness-of-fit tests using deterministic U-statistics designs (Zhang, 2021, Miglioli et al., 23 Oct 2025).
  • Poisson processes: Berry–Esseen rates for avoidance functionals (e.g., volume of union of balls, quantization error) via Malliavin–Stein calculus (Barrio, 2015).
  • Dynamical systems: Central limit theorem error control in time-dependent non-stationary compositions of expanding maps, with explicit dependence on metric and expansion parameters (Leppänen, 2024).
  • Edgeworth expansions: Sharp transition criteria between Berry–Esseen bounds and Edgeworth expansions via the Berry–Esseen characteristic and integrated tail-mass; necessary and sufficient conditions for second-order expansions in stationary weakly dependent processes (Jirak et al., 2020).

7. Interpretation, Optimality, and Directions

Berry–Esseen error control is fundamentally governed by Lyapunov-type ratios of the largest relevant moment, symmetries or exchangeability, density/concentration bounds, and detailed model structure (dependency, conditioning, normalization). Sharp constants and rates O(n1/2)O(n^{-1/2}), O(n1)O(n^{-1}), or precise moderate-deviation quantification are available under appropriate conditions; improved rates with moment matching, careful design, or symmetry are possible in modern formulations. The control facilitates finite-sample inference, sharp converses, and robust quantile calibration, often with rigorous optimality. The ongoing development concerns extensions to local limit forms, high dimensions, dependency graphs, functional data, non-normal targets, and more nuanced metrics (total variation, entropy, Wasserstein, Zolotarev distances).


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