$$ \newcommand{\st}{\text{ s.t. }} \newcommand{\and}{\text{ and }} \DeclareMathOperator*{\argmin}{arg\,min} \DeclareMathOperator*{\argmax}{arg\,max} \DeclareMathOperator*{\liminf}{lim\,inf} \DeclareMathOperator*{\limsup}{lim\,sup} \DeclareMathOperator*{\dom}{dom} \DeclareMathOperator*{\epi}{epi} \newcommand{\<}{\langle} \newcommand{\>}{\rangle} \newcommand{\R}{\mathbb{R}} \newcommand{\N}{\mathbb{N}} \newcommand{\O}{\mathcal{O}} \newcommand{\dist}{\text{dist}} \newcommand{\vec}[1]{\mathbf{#1}} \newcommand{\diag}{\mathrm{diag}} \newcommand{\d}{\mathrm{d}} \newcommand{\L}{\mathcal{L}} \newcommand{\H}{\mathcal{H}} \newcommand{\Tr}{\mathrm{\mathbf{Tr}}} \newcommand{\E}{\mathbb{E}} \newcommand{\Var}{\mathrm{Var}} \newcommand{\Cov}{\mathrm{Cov}} \newcommand{\indep}{\perp \!\!\! \perp} \newcommand{\KL}[2]{\mathrm{KL}(#1 \parallel #2)} \newcommand{\W}{\mathbf{W}} % Wasserstein distance \newcommand{\SW}{\mathbf{SW}} % Sliced-Wasserstein distance $$

Contrast

The perception of an image’s content changes little when an increasing function is applied to it. However, if the function is non-increasing, then the perception of the content changes completely. We are sensible to local rather than global changes of contrast. From now on, we are denoting $u \colon \Omega \to \mathbb{R}$ our image, where $\vert \Omega \vert = M \times N$ is a discrete rectangular grid. Also, we are assuming that $u$ takes discrete values $y_0 < \dots < y_{n - 1}$ (usually $0$ to $255$). ...

September 20, 2024 · 4 min · Felipe Vicentin

Image aquisition

The pinhole model The first very simple way to acquire images is with the pinhole model. Here, part of the light coming from the object passes through a small aperture $O$ and is projected onto the focal plane. We do this so that each point of the object is represented by a ray. Otherwise, the image would not be formed. The distance $f$ is called the focal length. Let’s suppose we have the following model to describe the pinhole: ...

September 16, 2024 · 3 min · Felipe Vicentin