Abstract

We apply a recently suggested new strategy to solve differential equations for Feynman integrals. We develop this method further by analyzing asymptotic expansions of the integrals. We argue that this allows the systematic application of the differential equations to single-scale Feynman integrals. Moreover, the information about singular limits significantly simplifies finding boundary constants for the differential equations. To illustrate these points we consider two families of three-loop integrals. The first are form-factor integrals with two external legs on the light cone. We introduce one more scale by taking one more leg off-shell, $p_2^2\neq 0$. We analytically solve the differential equations for the master integrals in a Laurent expansion in dimensional regularization with $\epsilon=(4-D)/2$. Then we show how to obtain analytic results for the corresponding one-scale integrals in an algebraic way. An essential ingredient of our method is to match solutions of the differential equations in the limit of small $p_2^2$ to our results at $p_2^2\neq 0$ and to identify various terms in these solutions according to expansion by regions. The second family consists of four-point non-planar integrals with all four legs on the light cone. We evaluate, by differential equations, all the master integrals for the so-called $K_4$ graph consisting of four external vertices which are connected with each other by six lines. We show how the boundary constants can be fixed with the help of the knowledge of the singular limits. We present results in terms of harmonic polylogarithms for the corresponding seven master integrals with six propagators in a Laurent expansion in $\epsilon$ up to weight six.

Highlights

  • In this work, the finiteness of planar integrals in the u-channel as u = −s − t → 0 played a decisive role because these boundary conditions turned out to be very restrictive

  • We apply a recently suggested new strategy to solve differential equations for Feynman integrals. We develop this method further by analyzing asymptotic expansions of the integrals. We argue that this allows the systematic application of the differential equations to single-scale Feynman integrals

  • We show how the boundary constants can be fixed with the help of the knowledge of the singular limits

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Summary

Analyzing asymptotic behavior with differential equations

Let us first show how to use differential equations in order to determine the asymptotic behavior of Feynman integrals. We have normalized all integrals such that they are dimensionless functions, and so that their ǫ expansion starts at ǫ0 They cannot have branch cuts starting at x = 1, and this information will be useful when determining boundary constants for the integrals. For a few integrals we have used the limit x → ∞ These limits, together with simple analytic expressions for propagator-type integrals that are known in terms of gamma functions, completely determine the boundary constants, and allow us to obtain the full solution. The solution at any order ǫk is given by a linear combination (with rational coefficients) of harmonic polylogarithms Ha1,a2,...,an(x) [34] of weight k The latter are iterated integrals built from the alphabet of differential forms d log x, d log(1−x), d log(1+x).

Example
Evaluating K4 integrals
Asymptotic behavior and boundary conditions
Crossing symmetry
Further analytic and numerical checks
The choice of master integrals and differential equations
Determining the boundary conditions
Analytic solution and on-shell limit
Discussion and outlook
A Evaluating K4 integrals by Mellin-Barnes representation
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