A self-consistent calculation of non-spherical Bose-Einstein correlation functions with Coulomb final-state interaction
Márton I. Nagy, Dániel Kincses, Máté Csanád
TL;DR
The paper tackles the challenge of accurately modeling Bose-Einstein correlations with Coulomb final-state interactions for non-spherical, Lévy-stable sources in heavy-ion collisions. It develops a self-consistent 3D framework by reformulating the Coulomb integral in Fourier space, deriving semi-analytic expressions for the Coulomb-corrected correlator via functionals $\mathcal{A}_1$ and $\mathcal{A}_2$, and providing a public software package for fully 3D computations. The authors apply the method to elliptically contoured Lévy sources and compare full 3D results with traditional spherical approximations, illustrating when the latter are adequate and when the full treatment is necessary, with emphasis on frame transformations between PCMS and LCMS. This work enables more precise femtoscopy analyses for high-statistics heavy-ion data and offers practical guidance for systematic uncertainties in experimental analyses.
Abstract
Particle correlations and femtoscopy are a rich subfield of high-energy physics. As the experimental data become more precise, there is an increasing need for the theoretical calculations to provide better and more general descriptions of the measurements. One of the important new directions is the investigation of the precise shape of the Bose-Einstein correlation functions utilizing Lévy-stable distributions. This work is a direct follow-up to our previous study, in which we developed a novel method for calculating Bose-Einstein correlation functions including the Coulomb final-state interaction. In this paper, we present a self-consistent generalization of the previous approach to non-spherical source functions and investigate the validity of the previously applied approximations assuming spherical symmetry. We present a software package that includes the calculation of a fully three-dimensional correlation function including the Coulomb interaction.
