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Vertex diagrams for the QED form factors at the 2-loop level

R. Bonciani, P. Mastrolia, E. Remiddi

TL;DR

The paper delivers a comprehensive reduction and analytic evaluation of all 2-loop QED electron-vertex integrals in continuous dimensional regularization for on-shell electrons with finite mass. By reducing to 16 Master Integrals using IBP, Lorentz invariance, and symmetry relations, and then solving a system of differential equations in $Q^2$ with an $\epsilon$-expansion, the authors express all MI coefficients in closed harmonic polylogarithmic form. The work provides explicit results for topologies with 3–6 denominators, including reducible diagrams, and furnishes high- and low-$Q^2$ expansions, laying the groundwork for the complete real and imaginary parts of the QED form factors at two loops. The methods combine bottom-up IBP, differential equations, and Euler’s variation of constants to achieve compact, analytic results suitable for numerical implementation and SEO-friendly indexing.

Abstract

We carry out a systematic investigation of all the 2-loop integrals occurring in the electron vertex in QED in the continuous $D$-dimensional regularization scheme, for on-shell electrons, momentum transfer $t=-Q^2$ and finite squared electron mass $m_e^2=a$. We identify all the Master Integrals (MI's) of the problem and write the differential equations in $Q^2$ which they satisfy. The equations are expanded in powers of $ε= (4-D)/2$ and solved by the Euler's method of the variation of the constants. As a result, we obtain the coefficients of the Laurent expansion in $ε$ of the MI's up to zeroth order expressed in close analytic form in terms of Harmonic Polylogarithms.

Vertex diagrams for the QED form factors at the 2-loop level

TL;DR

The paper delivers a comprehensive reduction and analytic evaluation of all 2-loop QED electron-vertex integrals in continuous dimensional regularization for on-shell electrons with finite mass. By reducing to 16 Master Integrals using IBP, Lorentz invariance, and symmetry relations, and then solving a system of differential equations in with an -expansion, the authors express all MI coefficients in closed harmonic polylogarithmic form. The work provides explicit results for topologies with 3–6 denominators, including reducible diagrams, and furnishes high- and low- expansions, laying the groundwork for the complete real and imaginary parts of the QED form factors at two loops. The methods combine bottom-up IBP, differential equations, and Euler’s variation of constants to achieve compact, analytic results suitable for numerical implementation and SEO-friendly indexing.

Abstract

We carry out a systematic investigation of all the 2-loop integrals occurring in the electron vertex in QED in the continuous -dimensional regularization scheme, for on-shell electrons, momentum transfer and finite squared electron mass . We identify all the Master Integrals (MI's) of the problem and write the differential equations in which they satisfy. The equations are expanded in powers of and solved by the Euler's method of the variation of the constants. As a result, we obtain the coefficients of the Laurent expansion in of the MI's up to zeroth order expressed in close analytic form in terms of Harmonic Polylogarithms.

Paper Structure

This paper contains 30 sections, 152 equations, 7 figures.

Figures (7)

  • Figure 1: 2-loop vertex diagrams for the QED form factor. The fermionic external lines are on the mass-shell $p_{1}^{2}=p_{2}^{2}=-a$, while the wavy line on the r.h.s. has momentum $Q=p_{1}+p_{2}$, with $Q^{2}=-s$.
  • Figure 2: A 4-denominator topology.
  • Figure 3: The set of 3 independent 6-denominator topologies present in the graphs of Fig.(\ref{['fig1']}).
  • Figure 4: The set of 8 independent 5-denominator topologies contained in the graphs of Fig.(\ref{['fig1']}). External fermion lines are put on the mass-shell $p_{1}^{2}=p_{2}^{2}=-a$, while external wavy lines carry an off-shell momentum $Q=p_{1}+p_{2}$. The topology (g) is evaluated on the mass-shell.
  • Figure 5: The set of 12 independent 4-denominator (sub)topologies coming from the 5-denominator topologies of Fig.(\ref{['fig2']}).
  • ...and 2 more figures