Abstract

The three-loop QED mass-dependent contributions to the $g-2$ of each of the charged leptons with two internal closed fermion loops, sometimes called $A^{(6)}_3\left(\frac{m_1}{m_2}, \frac{m_1}{m_3}\right)$ in the $g-2$ literature, is revisited using the Mellin-Barnes (MB) representation technique. Results for the muon and $\tau$ lepton anomalous magnetic moments $A^{(6)}_{3,\mu}$ and $A^{(6)}_{3,\tau}$, which were known as series expansions in the lepton mass ratios up to the first few terms only, are extended to their exact expressions. The contribution to the anomalous magnetic moment of the electron $A^{(6)}_{3,e}$ is also explicitly given in closed form. In addition to this, we show that the different series representations derived from the MB representation collectively converge for all possible values of the masses. Such unexpected behavior is related to the fact that these series bring into play double hypergeometric series that belong to a class of Kamp\'e de F\'eriet series which we prove to have the same simple convergence and analytic continuation properties as the Appell $F_1$ double hypergeometric series.

Highlights

  • The Mellin-Barnes (MB) representation method, a well-known computational tool of perturbative quantum field theory, can be used to derive series representations of Feynman diagrams and related quantities in terms of multiple hypergeometric series

  • Such unexpected behavior is related to the fact that these series bring into play double hypergeometric series that belong to a class of Kampede Feriet series which we prove to have the same simple convergence and analytic continuation properties as the Appell F1 double hypergeometric series

  • Related quantities by revisiting what is possibly the simplest class of quantum electrodynamics (QED) contributions to the anomalous magnetic moment of each of the charged leptons that can be represented by a twofold MB integral. These threeloop QED mass-dependent contributions with two internal closed fermion loops, often denoted Að36Þðm1=m2; m1=m3Þ in the g − 2 literature, can involve at most double hypergeometric series, and we show that they have an unexpected behavior

Read more

Summary

INTRODUCTION

The Mellin-Barnes (MB) representation method, a well-known computational tool of perturbative quantum field theory, can be used to derive series representations of Feynman diagrams and related quantities in terms of multiple hypergeometric series. The analytic continuation properties that these g − 2 contributions satisfy are, surprisingly, the converse of what one faces when one deals with, for instance, the sunset diagram case because the MB representation of Að36Þðm1=m2; m1=m3Þ does not give rise to any white region This interesting result has encouraged us to probe what is special about the double hypergeometric series involved in our final expressions. We show that the latter and the former both belong to a class of Kampede Feriet series for which we prove, from their MB representation, the absence of white regions As another motivation for studying these particular g − 2 contributions it should be noted, and as emphasized in [4], that in contrast to all other three loop QED contributions to the muon anomalous magnetic moment, Að36;μÞðmμ=mτ; mμ=meÞ is the only one whose exact analytic form has not been derived so far. VI, where a short discussion of the results and future work are presented

SHORT QED LITERATURE REVIEW
THREE-LOOP QED CONTRIBUTIONS WITH TWO INTERNAL LOOPS
Convergence region
Exact result
Other cones
NUMERICAL ANALYSIS AND CHECKS
CONVERGENCE AND ANALYTIC CONTINUATION PROPERTIES OF KAMPÉ
CONCLUSION AND DISCUSSION
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call