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Refined Discrepancy Estimates

Updated 19 November 2025
  • Refined discrepancy estimates are advanced quantitative bounds that improve classical worst-case measures by incorporating averaging techniques and structure-dependent criteria.
  • They enhance error bounds in quasi–Monte Carlo integration by employing Lp, BMO, and exponential Orlicz norms to precisely measure uniformity of point distributions.
  • Applications span high-dimensional random constructions, explicit sequence analysis, and acceptance–rejection sampling to optimize computational methods.

Refined discrepancy estimates are advanced quantitative bounds on the distributional irregularity, or "discrepancy," of finite and infinite point sets and sequences in multidimensional unit cubes or under various geometric or statistical transformations. These estimates go beyond classical worst-case (sup-norm) bounds to provide improved rates under averaging, moment, weighted, or structure-dependent criteria, frequently employing advanced techniques from harmonic analysis, probabilistic combinatorics, and Diophantine approximation.

1. Fundamental Notions and Discrepancy Functionals

Let PN={x1,,xN}[0,1)dP_N=\{x_1,\dots,x_N\}\subset [0,1)^d be a point set. The star discrepancy measures the largest deviation, over axis-parallel boxes anchored at the origin, between the empirical measure and Lebesgue measure: DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|. Associated functionals include LpL_p-discrepancy, BMO, and exponential Orlicz norms, as well as generalizations to half-space, L1L^1-averaged, and smooth-weighted settings. Uniformity in multidimensional distribution is crucial for numerical integration and quasi–Monte Carlo (QMC), where low discrepancy guarantees optimal error rates for bounded-variation integrands (Bilyk et al., 2014, Amirkhanyan et al., 2013, Kritzinger et al., 2015).

2. Polylogarithmic and Averaged Bounds: From Supremum to L1L^1 and LpL^p

Classical discrepancy theory gives lower bounds DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N (Roth, Schmidt) and, for optimal explicit constructions, DN=O((logN)d/N)D_N^* = O((\log N)^{d}/ N) (Larcher, 2014). Recent refined estimates focus on improved asymptotics under averaging:

  • L1L^1 Half-Space Discrepancy: For the cube [1,1]d[-1,1]^d, there exists a set DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.0 of DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.1 points such that

DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.2

where DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.3 is the half-space discrepancy and DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.4 is dimension-dependent (Chen et al., 2010). This generalizes Beck–Chen’s planar DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.5 bound and surpasses polynomial sup-norm bounds by exploiting DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.6 averaging.

  • DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.7-Discrepancy and Symmetrization: For symmetrized van der Corput sequence DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.8,

DN(PN)=supt[0,1]d1Ni=1N1[0,t)(xi)j=1dtj.D_N^*(P_N) = \sup_{t\in[0,1]^d}\left|\frac{1}{N}\sum_{i=1}^N \mathbf{1}_{[0,t)}(x_i) - \prod_{j=1}^d t_j\right|.9

optimal by Roth–Proinov theory, proven by precise Haar coefficient estimates and Littlewood–Paley theory (Kritzinger et al., 2015).

3. High-Dimensional and Randomized Bounds

Standard probabilistic constructions achieve

LpL_p0

for i.i.d. samples (HNWW). Refinements yield sharper constants and explicit probability-dependent bounds (Löbbe, 2014, Pasing et al., 2018):

  • For lacunary sequences LpL_p1 with LpL_p2 uniform,

LpL_p3

holds with explicit LpL_p4 and failure probability LpL_p5 (Löbbe, 2014).

  • The explicit constant in the high-dimensional random construction for LpL_p6 is now attainable via improved bracketing/covering number bounds (Pasing et al., 2018).

4. Orlicz, BMO, and Endpoint Discrepancy Spaces

Refined results probe discrepancy's integrability and tail behavior:

  • Exponential Orlicz Estimates: For LpL_p7-point sets LpL_p8,

LpL_p9

holds for Skriganov–Chen-style digital nets with random shift (Amirkhanyan et al., 2013). This rate is sharp and interpolates classical L1L^10 and sup-norms.

  • BMO and Product-Orlicz in L1L^11: Order-2 digital nets L1L^12 satisfy

L1L^13

which lies precisely at the critical endpoint between L1L^14 and L1L^15 (Bilyk et al., 2014).

These results are central to understanding tail decay of the discrepancy function and its role in QMC integration, particularly for function classes at the boundary of L1L^16.

5. Refined Estimates for Structured, Indexed, and Hybrid Sequences

  • Explicit Sequences with Sharp Rates: The concatenated inverse-prime sequence L1L^17 defined by blockwise inverses modulo primes satisfies

L1L^18

and this is best possible for the construction (Lind, 2021).

  • Index-Transformed Sequences: For sequences indexed by sum-of-digits or smooth functions,

L1L^19

these bounds quantify the uniformity loss under irregular indexing and generalize to multidimensional and digital settings (Kritzer et al., 2014).

  • Hybrid and Metrological Constructions: Metrical or average-case theorems establish that for almost all parameters in Kronecker, digital, or hybrid sequences, discrepancy can be reduced to

L1L^10

with lower bounds matching up to a L1L^11 factor (Larcher, 2014).

6. Discrepancy Beyond Axis-Aligned Boxes and Halfspaces

  • Acceptance–Rejection and Stratified Sampling: Acceptance–rejection samples using stratified (or net-based) drivers admit improved discrepancy rates:

L1L^12

and, for driver nets with boundary cover number L1L^13,

L1L^14

with exponents optimized by smoothness or geometric complexity of the acceptance region (Zhu et al., 2014).

  • Markov Chain Quasi–Monte Carlo: For variance-bounding chains and suitable deterministic drivers, star-discrepancy decays as L1L^15, approaching L1L^16 with the anywhere-to-anywhere property (Dick et al., 2013).

7. Smooth Discrepancy and Diophantine Approximation

Recent advances in "smooth discrepancy" investigate weighted test functions of high regularity. For the L1L^17-dimensional Kronecker sequence: L1L^18 where L1L^19 encodes Diophantine properties of LpL^p0 and LpL^p1 (Chow et al., 2024). In LpL^p2 and LpL^p3, for suitably badly approximable LpL^p4, the smooth discrepancy is bounded or grows only logarithmically, but for LpL^p5, the problem is tied to Littlewood's conjecture: unbounded smooth discrepancy would imply the conjecture holds in that dimension.

Table: Key Refined Discrepancy Estimates

Setting Refined Discrepancy Rate Reference
LpL^p6 half-space (cube in LpL^p7) LpL^p8 (Chen et al., 2010)
High-dim random star (LpL^p9) DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N0, DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N1 (Pasing et al., 2018)
Symmetrized van der Corput DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N2 (DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N3, DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N4) (Kritzinger et al., 2015)
Exponential Orlicz/BMO (DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N5) DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N6 (Amirkhanyan et al., 2013, Bilyk et al., 2014)
Stratified acceptance-rej. DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N7 (Zhu et al., 2014)
Indexed sequences DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N8 or DN(logN)d/2/ND_N^*\gtrsim (\log N)^{d/2}/N9 (Kritzer et al., 2014)
Smooth Kronecker DN=O((logN)d/N)D_N^* = O((\log N)^{d}/ N)0 (Diophantine-dependent) (Chow et al., 2024)
Explicit DN=O((logN)d/N)D_N^* = O((\log N)^{d}/ N)1-dim seq. (inv-primes) DN=O((logN)d/N)D_N^* = O((\log N)^{d}/ N)2 (Lind, 2021)

These advances collectively demonstrate that, by exploiting averaging, functional-analytic, combinatorial, and arithmetic structures, refined discrepancy estimates can dramatically improve the theoretical and practical bounds on uniformity of point sets in high-dimensional computational and analytic settings.

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