In this talk, we discuss the question of Gibbs point processes in Rd with pairwise interactions that are not integrable at infinity. A standard example is the Riesz potential of the form φ(x)=1|x|s where s<d. This setting has a long history, notably because the case s=d−2 corresponds to the classical Coulomb potential, which arises from electrostatic theory. We will first address the existence of the process in the infinite volume regime when a neutralizing background is introduced (this model is known as Jellium in theoretical physics). Subsequently, we will discuss the rigidity of such point processes, specifically hyper-uniformity and number rigidity. We will provide a state-of-the-art review and present numerous conjectures and open problems.