The number of fiber intersections $ Y $ inside a bounded counting region of a two-dimensional random fiber web is a lattice-valued statistic whose finite-sample distribution can be asymmetric in a way that the recently established Gaussian limit cannot represent. That, together with the overdispersion of $ Y $ above a geometry-dependent fiber-count threshold and the mismatch between a continuous law and a lattice, motivates the negative binomial law matched to the exact finite-sample mean and variance of $ Y $. We first showed that the conditional intersection probability depends on a partner fiber's seeding region only through its expected truncated length, so the moment formulas keep their form under type-specific seeding; this settles a question left open by Chun and Jhong (2026). We then provided the exact finite-sample threshold beyond which the moment-matched fit exists—weaker in our configuration than the leading-order condition by a factor of about $ 63 $—and settled which negative binomial parameter must diverge for asymptotic normality: Not $ r_n $, for which we give a counterexample, but $ r_n(1-\theta_n) $. A large-scale simulation then compared the two approximations on a common lattice, using closed-form truncated-length moments. Two corrections proved essential: The Kolmogorov–Smirnov statistic must be evaluated for a lattice reference law, and the normal law must carry a half-count continuity correction, which alone is worth some $ 60\% $ of the apparent gain. The negative binomial's remaining advantage is real but not uniform: A factor of two in Kolmogorov distance at $ 150 $ equal-length fibers, the same at $ 300 $ on weaker evidence, not resolved from $ 500 $ onward, and reversed in one mixture configuration. On the Kolmogorov distance restricted to the outer $ 10\% $ of the distribution, it was ahead in every configuration we ran, though not in every individual tail cell; at $ 150 $ fibers and three standard deviations, the corrected Gaussian understated the upper tail by a factor of $ 2.2 $ and the negative binomial by $ 15\% $.
Citation: Heuiju Chun, Jae-Hwan Jhong. A moment-matched negative binomial approximation for fiber intersection counts in two-dimensional random webs[J]. AIMS Mathematics, 2026, 11(11): 36134-36162. doi: 10.3934/math.20261400
The number of fiber intersections $ Y $ inside a bounded counting region of a two-dimensional random fiber web is a lattice-valued statistic whose finite-sample distribution can be asymmetric in a way that the recently established Gaussian limit cannot represent. That, together with the overdispersion of $ Y $ above a geometry-dependent fiber-count threshold and the mismatch between a continuous law and a lattice, motivates the negative binomial law matched to the exact finite-sample mean and variance of $ Y $. We first showed that the conditional intersection probability depends on a partner fiber's seeding region only through its expected truncated length, so the moment formulas keep their form under type-specific seeding; this settles a question left open by Chun and Jhong (2026). We then provided the exact finite-sample threshold beyond which the moment-matched fit exists—weaker in our configuration than the leading-order condition by a factor of about $ 63 $—and settled which negative binomial parameter must diverge for asymptotic normality: Not $ r_n $, for which we give a counterexample, but $ r_n(1-\theta_n) $. A large-scale simulation then compared the two approximations on a common lattice, using closed-form truncated-length moments. Two corrections proved essential: The Kolmogorov–Smirnov statistic must be evaluated for a lattice reference law, and the normal law must carry a half-count continuity correction, which alone is worth some $ 60\% $ of the apparent gain. The negative binomial's remaining advantage is real but not uniform: A factor of two in Kolmogorov distance at $ 150 $ equal-length fibers, the same at $ 300 $ on weaker evidence, not resolved from $ 500 $ onward, and reversed in one mixture configuration. On the Kolmogorov distance restricted to the outer $ 10\% $ of the distribution, it was ahead in every configuration we ran, though not in every individual tail cell; at $ 150 $ fibers and three standard deviations, the corrected Gaussian understated the upper tail by a factor of $ 2.2 $ and the negative binomial by $ 15\% $.
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Difference between the simulated distribution function of $ Y $ and each approximation, against the standardized count. Both approximations are built from the same finite-$ n $ moments $ (m, v) $ and so differ only in shape
Relative error of the approximate upper-tail probability $ \mathbb{P}(Y\ge m+z\sqrt v) $ as a function of the cut-off $ z $, for two fiber counts, shown only as far out as the simulation resolves (at least $ 25 $ observed exceedances in the simulation). The shaded band is one estimated relative Monte Carlo standard error of the simulated tail probability, on either side of zero; it is not a confidence band for either approximation curve. The symmetric Gaussian approximation understates the upper tail increasingly severely as $ z $ grows. The negative binomial reduces that underestimation over the whole of the displayed range, by a factor of roughly two at the largest cut-offs, but does not remove it: Its own relative error is negative and growing at the edge of resolution
Two-length mixture model under type-specific seeding. Left: The simulated distribution of $ Y $ with the two lattice approximations overlaid. Right: The difference between the simulated distribution function and each approximation, as in Figure 1