FEYNMAN DIAGRAMS AND DIFFERENTIAL EQUATIONS
By M. Argeri, Pierpaolo Mastrolia. 2007
205 citations recorded by the source corpus.
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.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/a9c3a034cd6fe1bc1bf39156f223ee6a1aeab7c2
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Astronomy and Astrophysics
- L. Tancredi
- Erik Panzer
- Stefan Weinzierl
- Christian Bogner
- Luise Adams
- Pierpaolo Mastrolia
- P. Baikov
- E. Mirabella
In Nuclear and High Energy Physics
- Erik Panzer
- L. Tancredi
- E. Mirabella
- Pierpaolo Mastrolia
- Johannes Schlenk
- Luise Adams
- Stefan Weinzierl
- Christian Bogner
Citations in the corpus
- The two-loop sunrise graph with arbitrary masses (2013, background): “We expect that a solution can be obtained along the lines of [9, 26].”
- Algorithms for the symbolic integration of hyperlogarithms with applications to Feynman integrals (2014, methodology): “Also within the method of differential equations [21], boundary conditions occur that must be obtained separately, e.”
- Four Loop Massless Propagators: an Algebraic Evaluation of All Master Integrals (2010, background): “For its modern status and further references, see the review [97].”
- The full four-loop cusp anomalous dimension in N\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{N} $$\end{do (2019, unknown): “We find that the differential equations (for reviews, see [63, 64]) for this basis takes the form”
- Lectures on differential equations for Feynman integrals (2014, unknown): “Earlier reviews include [8].”
- Magnus and Dyson series for Master Integrals (2014, methodology): “[4, 5], is one of the most effective techniques for computing dimensionally regulated multi-loop integrals and has led to significant achievements in the context of multi-loop corrections.”
- Feynman integrals and hyperlogarithms (2015, methodology): “The method of differential equations [10, 98] generates a system of linear, first-order partial differential equations in terms of Feynman integrals in the family of the initial graph.”