Traitement du signalLe traitement du signal est la discipline qui développe et étudie les techniques de traitement, d'analyse et d' des . Parmi les types d'opérations possibles sur ces signaux, on peut dénoter le contrôle, le filtrage, la compression et la transmission de données, la réduction du bruit, la déconvolution, la prédiction, l'identification, la classification Bien que cette discipline trouve son origine dans les sciences de l'ingénieur (particulièrement l'électronique et l'automatique), elle fait aujourd'hui largement appel à de nombreux domaines des mathématiques, comme la , les processus stochastiques, les espaces vectoriels et l'algèbre linéaire et des mathématiques appliquées, notamment la théorie de l'information, l'optimisation ou encore l'analyse numérique.
Heteroskedasticity-consistent standard errorsThe topic of heteroskedasticity-consistent (HC) standard errors arises in statistics and econometrics in the context of linear regression and time series analysis. These are also known as heteroskedasticity-robust standard errors (or simply robust standard errors), Eicker–Huber–White standard errors (also Huber–White standard errors or White standard errors), to recognize the contributions of Friedhelm Eicker, Peter J. Huber, and Halbert White.
Type I and type II errorsIn statistical hypothesis testing, a type I error is the mistaken rejection of an actually true null hypothesis (also known as a "false positive" finding or conclusion; example: "an innocent person is convicted"), while a type II error is the failure to reject a null hypothesis that is actually false (also known as a "false negative" finding or conclusion; example: "a guilty person is not convicted").
Dimensional regularizationNOTOC In theoretical physics, dimensional regularization is a method introduced by Giambiagi and Bollini as well as – independently and more comprehensively – by 't Hooft and Veltman for regularizing integrals in the evaluation of Feynman diagrams; in other words, assigning values to them that are meromorphic functions of a complex parameter d, the analytic continuation of the number of spacetime dimensions. Dimensional regularization writes a Feynman integral as an integral depending on the spacetime dimension d and the squared distances (xi−xj)2 of the spacetime points xi, .
