Speaker
Description
Hadrons are strongly interacting particles composed of quarks and gluons and described by Quantum Chromodynamics (QCD). Their internal structure can be described in terms of structure functions that encode, for example, the momentum and spin distributions of their constituents. Parton distribution functions (PDFs), for example, describe the quark and gluon momentum distributions inside a hadron. These distribution functions are, however, not easy to calculate, because they are defined on the light front, whereas most hadron calculations are performed in a Euclidean metric and yield, for instance, the hadron’s Bethe-Salpeter wave functions. The main problem is then to project these Bethe-Salpeter wave functions onto the light front.
We present a new method to compute the light-front wave functions using contour deformations, which we illustrate for a simple system of two interacting scalar particles of equal mass. After solving the two-body Bethe-Salpeter equation, the projection onto the light front is done through a combination of contour deformations and analytic continuation methods, and shown to be in agreement with the commonly used Nakanishi method. After showing that the contour deformation method can be used for particles of unequal masses and complex conjugate propagator poles, we explore the extension of this method to the calculation of more general parton distributions, such as transverse momentum distributions (TMDs) and generalized parton distributions (GPDs), from the projection of the hadron-hadron correlator, built from elementary n-point functions, such as the quark propagator and 4-point function.
