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Feynman Diagrams and Differential Equations (0707.4037v1)

Published 27 Jul 2007 in hep-ph

Abstract: We review in a pedagogical way the method of differential equations for the evaluation of D-dimensionally regulated Feynman integrals. After dealing with the general features of the technique, we discuss its application in the context of one- and two-loop corrections to the photon propagator in QED, by computing the Vacuum Polarization tensor exactly in D. Finally, we treat two cases of less trivial differential equations, respectively associated to a two-loop three-point, and a four-loop two-point integral. These two examples are the playgrounds for showing more technical aspects about: Laurent expansion of the differential equations in D (around D=4); the choice of the boundary conditions; and the link among differential and difference equations for Feynman integrals.

Citations (199)

Summary

Analysis of Feynman Diagrams and Differential Equations

The paper by Mario Argeri and Pierpaolo Mastrolia provides a comprehensive examination of the application of differential equations to the evaluation of D-dimensionally regulated Feynman integrals. The authors aim to illuminate the process of tackling integrals essential to quantum field theory calculations, particularly in scenarios where more traditional direct integration techniques become computationally intensive or infeasible.

The discussion begins with a pedagogical exploration of Feynman diagrams' role within the perturbative framework of quantum electrodynamics (QED), emphasizing photon propagator corrections. By employing the method of integration-by-parts (IBP) identities combined with Lorentz invariance and symmetry relations, the paper delineates how one may systematically reduce the complexity of these calculations. The IBP relations, alongside these symmetries, facilitate the expression of Feynman integrals in terms of a minimal set of fundamental integrals, known as Master Integrals (MIs).

One of the significant contributions of the paper is the elaboration on the systematic reduction of higher-order loop integrals to these MIs, thereby simplifying calculations previously requiring the evaluation of numerous complex integrals. The paper introduces differential equations tailored specifically for these MIs, allowing for their computation through techniques like Euler's variation of constants. This methodology is extended through examples of both analytic and numeric solutions, showcasing its adaptability and power in various situational contexts.

Particularly notable is the application of example cases, such as the two-loop vacuum polarization in QED. These practical examinations highlight the technical nuances encountered when solving systems of differential equations and dealing with their boundary conditions. The paper also considers applications in more complex scenarios, such as multi-loop corrections essential for the precision calculations in the Standard Model predictions, including heavy-quark and Higgs boson physics.

The authors do not only focus on presenting this method in great detail but also speculate on its broader implications. The method's ability to separate algebraic complexity from analytic issues presents a strategic advantage in tackling perturbative calculations beyond Feynman integrals, potentially informing developments in computational methodologies in theoretical physics.

This paper stands as a detailed resource for researchers dealing with perturbative calculations at higher-loop orders. It not only refines the mathematical toolkit available to physicists but also underscores the interdisciplinary potential of techniques bridging algebraic and analytic mechanics within theoretical physics. The authors propose that while a unified analytical strategy for Feynman integrals is not yet available, the method of differential equations presented offers a promising tool, opening avenues for more efficient and accurate computational approaches in quantum field theory. Future work might explore crafting bespoke differential equations for even more challenging Feynman integrals, perhaps offering new strategies in tackling the inherent complexities of gauge theories and beyond.

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