Abstract

We consider a set of two-loop sunrise master integrals with two different internal masses at pseudo-threshold kinematics and we solve it in terms of elliptic polylogarithms to all orders of the dimensional regulator.

Highlights

  • Progress in this direction has been made in [35], where eMPLs are defined on the complex plane, and their structure naturally adapts to representations of Feynman integrals commonly used in the physics literature (e.g. Feynman parameters)

  • Similar results exist for three-point and fourpoint two-loop Feynman diagrams in non-relativistic limits of Quantum Chromodynamics (NRQCD) kinematics (see ref. [56] for O(ε0) results and [112] for results to every order in ε in terms of s+1Fs-hypergeometric functions with s ≤ 7)

  • In this paper we studied a family of sunrise integrals with two different internal masses and pseudo-threshold kinematics in dimensional regularisation

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Summary

The sunrise integral

[71] we study the sunrise integral topology defined as, Ji1,i2,i3 (m2, M 2) =. This integral family has three master integrals, which can be chosen to be J1,1,1, J1,1,2, J1,2,2 and which can be solved in closed form in terms of hypergeometric functions [71] as, J1,2,2(m2, M 2) = −

Integral representations
All orders result in terms of elliptic polylogarithms
Elliptic polylogarithms
Regularisation
Elliptic polylogarithms and all orders result
Sunsets
Example
Conclusions
A Integral representations for the hypergeometric functions
C Improved representations
D Leading terms of the ε-expansion and one-fold integrals
E Definitions for elliptic polylogarithms
Full Text
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