Ericson fluctuations constitute one of the most characteristic features of quantum chaotic scattering in the regime of strongly overlapping resonances such as a compound nucleus. ^{[1] [2] [3]} These fluctuations were predicted in 1960 by Torleif Ericson in two seminal articles, ^{[4] [5] [6] [7]} further developed in 1963, ^[8] based on the same statistical assumptions as those used by E. Wigner, C. E. Porter and R. G. Thomas to describe generic properties of resonances in long-lived compound nuclear systems. ^{[9] [10] [11]} In the present case the fluctuations occur in the "continuum" regime for which a large number of such resonances overlap coherently, owing to the short lifetime of the compound nucleus. At the time it was believed that this would lead to a structure-less behavior. Ericson realized that the opposite was the case with strong, random fluctuations. ^{[12] [7]}

The Ericson fluctuations were first observed in 1964 by P. Von Brentano et al. ^[13] in nuclear physics giving rise to a vigorous theoretical and experimental programme. ^[3] They have the curious feature of being both reproducible and random at the same time. ^[14] The fluctuations are universal and have later been observed in many other areas such as photoionization of hydrogen, uni-molecular dissociation ( physical chemistry), ^[15] perturbed atomic and molecular systems and micro wave billiards. ^{[3] [16] [17]}

Present theoretical descriptions of chaotic quantum scattering confirm the predicted properties of the Ericson fluctuations. ^[9] The universality of the Ericson fluctuations are thus very well established. ^[3]