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Interaction Budgets for Gated Wavelet Denoising: An EMPR Theory of Operator- Versus Correlation-Induced Coupling
Ercan Gürvit
Posted: 20 July 2026
Assessing Area Under the Curve (AUC) with a Larger Number of Repeated Measures: A Simulated Mediation Analysis Comparing AUC Calculated with the Trapezoid-Rule and Definite Integrals with 30 and 100 Repeated Measures
Daniel Rodriguez
Posted: 20 July 2026
A Semiparametric Panel Generalized Additive Model for Forecasting GDP Growth and Inflation in African Economies
Ben Magabashele Malope
,Retius Chifurira
,Temesgen Zewotir
,Knowledge Chinhamu
Posted: 17 July 2026
Forest Fires in Sicily: Statistical Risk Analysis Based on 2010-2023 Data
Stefano Barone
,Santo Orlando
,Antonino Paladino
Posted: 13 July 2026
Tourist Profile Segmentation through Symmetric Asymmetric Multivariate Structures: Integrating Biplot, Co-Inertia Analysis and Neutrosophic Psychology
Harry Vite-Cevallos
,Omar Ruiz-Barzola
,Purificación Galindo-Villardón
Posted: 08 July 2026
Robust Unsupervised Spatial-Kinematic Coupling for Satellite Laser Ranging Signal Extraction
Yi Chen
,Rufeng Tang
,Yuqiang Li
,Niansheng Tang
Posted: 08 July 2026
A Note on the Background Driving Process Associated with Generalized Tempered Stable Distributions
A. Hilaire Nzokem
Posted: 03 July 2026
A Ranked Sparsity Extension to the Bayesian Information Criterion: A Tool for Selecting Variables from Multiple Data Modalities
Ryan A. Peterson
,Sarah M. Bird
,Logan M. Harris
,Patrick J. Breheny
,Joseph E. Cavanaugh
Posted: 03 July 2026
Comparative Efficacy of Statistical Learning and Ensemble Methods for Multivariate Obesity Condition Classification
Justice Yaw Effah
,Gifty Duah
,Eric Nyarko
,Miriam Appiah
,Natasha Adjoa Anderson
Posted: 30 June 2026
Bias Reduction for Moment Estimates and MLEs
C.S. Withers
Posted: 29 June 2026
Quantification of Statistical Evidence: P-Values, Likelihood Principle and Bayes Factors
Paul A. Quaye
,Andrew A. Neath
Posted: 29 June 2026
Stochastic Foundations of Atmospheric Thermodynamics: Deriving the Laws from Maximum Entropy and Implications for Earth’s Climate
Demetris Koutsoyiannis
Posted: 29 June 2026
Functional Moments and Functional Moment Generating Functions for Gaussian Random Variables: Theory, Inequalities, Numerical Analysis, and Applications
Sthitadhi Das
Posted: 29 June 2026
Modeling Healthcare Data with Logistic Quantile and Uniform Based Mixture Polynomial Distributions
Mohan D. Pant
,Aditya Chakraborty
,Jovanna A. Tracz
Posted: 23 June 2026
Stochastic First Passage to Institutional Distrust Under Informational Turbulence
Dimitri Volchenkov
Posted: 17 June 2026
Local-Time Sensitivity and Burst Instability for Threshold Functionals of One-Dimensional Diffusions
Tristan Guillaume
Let \(X = \left( X_{t} \right)_{0 \leq t \leq T}\) be a real-valued continuous process. For a threshold \(a\), the sub-threshold time set \[E_{T}(a) = \{ t \in \lbrack 0,T\rbrack:X_{t} \leq a\}\] encodes several different threshold observables. The most elementary one is the cumulative occupation time \[A_{T}(a) = \int_{0}^{T}\mathbf{1}_{\{ X_{t} \leq a\}}\, dt.\] For a regular one-dimensional diffusion, the classical occupation density formula gives \[A_{T}(a) = \int_{- \infty}^{a}\frac{L_{T}^{y}(X)}{\sigma^{2}(y)}\, dy,\] and hence \[\frac{\partial A_{T}}{\partial a}(a) = \frac{L_{T}^{a}(X)}{\sigma^{2}(a)}.\] Thus additive threshold occupation admits a local-time sensitivity calculus. In the terminology of barrier contracts, this additive clock is the cumulative, non-resetting Parisian clock, also called the Parasian clock. The purpose of this paper is to contrast this additive/Parasian regime with the behavior of resetting Parisian burst functionals. The connected components of \(E_{T}(a)\) represent sub-threshold episodes. We study in particular the longest burst \[M_{T}(a) = \sup\{|I|:I\text{ is a connected component of }E_{T}(a)\}.\] While \(A_{T}\) is locally controlled by local time, \(M_{T}\) is governed by the connectivity of the sub-threshold time set. We prove that \(M_{T}\) is monotone, that its supremum is attained, and that the weak-sublevel version is right-continuous with left limits, while the strict-sublevel version is its left-continuous regularization. The jump at a level is the increase in the maximal connected-component length produced by adjoining the level set. This gives a deterministic càdlàg/càglàd calculus for longest-burst profiles. For regular one-dimensional diffusions, this yields a sharp structural contrast. At deterministic levels which are almost surely not local-extreme values, the weak and strict longest bursts agree almost surely. Whenever the path has a unique interior maximum, the level-indexed longest-burst profile has a positive jump at the maximum level and is therefore not absolutely continuous. Brownian motion satisfies this criterion almost surely. We further identify the deterministic mechanism behind this instability: small threshold increases may fill short temporal bridges and merge large sub-threshold components. Finally, we show that the longest burst is exactly a one-sided continuous Parisian functional. This yields an exact Laplace-transform representation of its Brownian law through the Chesney--Jeanblanc-Picqué--Yor [1] Parisian transform, and an excursion-measure formulation in which local time enters only as the Itô excursion intensity. We also discuss smoothed burst statistics, moving thresholds, and diffusion examples. The paper is intended as a threshold-sensitivity comparison: local time controls cumulative Parasian occupation, whereas resetting Parisian burst observables are controlled by component mergers and excursion structure.
Let \(X = \left( X_{t} \right)_{0 \leq t \leq T}\) be a real-valued continuous process. For a threshold \(a\), the sub-threshold time set \[E_{T}(a) = \{ t \in \lbrack 0,T\rbrack:X_{t} \leq a\}\] encodes several different threshold observables. The most elementary one is the cumulative occupation time \[A_{T}(a) = \int_{0}^{T}\mathbf{1}_{\{ X_{t} \leq a\}}\, dt.\] For a regular one-dimensional diffusion, the classical occupation density formula gives \[A_{T}(a) = \int_{- \infty}^{a}\frac{L_{T}^{y}(X)}{\sigma^{2}(y)}\, dy,\] and hence \[\frac{\partial A_{T}}{\partial a}(a) = \frac{L_{T}^{a}(X)}{\sigma^{2}(a)}.\] Thus additive threshold occupation admits a local-time sensitivity calculus. In the terminology of barrier contracts, this additive clock is the cumulative, non-resetting Parisian clock, also called the Parasian clock. The purpose of this paper is to contrast this additive/Parasian regime with the behavior of resetting Parisian burst functionals. The connected components of \(E_{T}(a)\) represent sub-threshold episodes. We study in particular the longest burst \[M_{T}(a) = \sup\{|I|:I\text{ is a connected component of }E_{T}(a)\}.\] While \(A_{T}\) is locally controlled by local time, \(M_{T}\) is governed by the connectivity of the sub-threshold time set. We prove that \(M_{T}\) is monotone, that its supremum is attained, and that the weak-sublevel version is right-continuous with left limits, while the strict-sublevel version is its left-continuous regularization. The jump at a level is the increase in the maximal connected-component length produced by adjoining the level set. This gives a deterministic càdlàg/càglàd calculus for longest-burst profiles. For regular one-dimensional diffusions, this yields a sharp structural contrast. At deterministic levels which are almost surely not local-extreme values, the weak and strict longest bursts agree almost surely. Whenever the path has a unique interior maximum, the level-indexed longest-burst profile has a positive jump at the maximum level and is therefore not absolutely continuous. Brownian motion satisfies this criterion almost surely. We further identify the deterministic mechanism behind this instability: small threshold increases may fill short temporal bridges and merge large sub-threshold components. Finally, we show that the longest burst is exactly a one-sided continuous Parisian functional. This yields an exact Laplace-transform representation of its Brownian law through the Chesney--Jeanblanc-Picqué--Yor [1] Parisian transform, and an excursion-measure formulation in which local time enters only as the Itô excursion intensity. We also discuss smoothed burst statistics, moving thresholds, and diffusion examples. The paper is intended as a threshold-sensitivity comparison: local time controls cumulative Parasian occupation, whereas resetting Parisian burst observables are controlled by component mergers and excursion structure.
Posted: 15 June 2026
E-CVWMD and E-CVWMD-Pairwise: Novel Joint
Performance Metrics for Mixed-Type Multivariate
Hydroclimatic Models
David Arango-Londoño
,Delia Ortega-Lenis
,Mauricio A. Mazo-Lopera
,Paula Moraga
Posted: 15 June 2026
Development of a Four-Parameter Statistical Neutrosophic Nadarajah-Haghighi Distribution: Estimation, Simulation, and Application to Neutrosophic Monthly Temperature Data
Rihab Ahmed Abed
,Wafaa A. Ashour
,Nooruldeen A. Noori
Posted: 05 June 2026
On Minimax Robust Estimation Problem for Stochastic Sequences with Harmonizable Stable Increments
Maksym Luz
,Mikhail Moklyachuk
Posted: 04 June 2026
A Probability Generating Function Based Goodness-of-Fit Test for the Poisson–Three-Parameter Lindley Distribution
Francisco Novoa-Muñoz
Posted: 03 June 2026
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