Abstract

We apply the method of regions to the massive two-loop integrals appearing in the Higgs pair production cross section at the next-to-leading order, in the high energy limit. For the non-planar integrals, a subtle problem arises because of the indefinite sign of the second Symanzik polynomial. We solve this problem by performing an analytic continuation of the Mandelstam variables such that the second Symanzik polynomial has a definite sign. Furthermore, we formulate the procedure of applying the method of regions systematically. As a by-product of the analytic continuation of the Mandelstam variables, we obtain crossing relations between integrals in a simple and systematic way. In our formulation, a concept of “template integral” is introduced, which represents and controls the contribution of each region. All of the template integrals needed in the computation of the Higgs pair production at the next-to-leading order are given explicitly. We also develop techniques to solve Mellin-Barnes integrals, and show them in detail. Although most of the calculation is shown for the concrete example of the Higgs pair production process, the application to other similar processes is straightforward, and we anticipate that our method can be useful also for other cases.

Highlights

  • One of the most interesting problems in this field is higher order corrections to multiscale processes

  • We apply the method of regions to the massive two-loop integrals appearing in the Higgs pair production cross section at the next-to-leading order, in the high energy limit

  • For the non-planar integrals, a subtle problem arises because of the indefinite sign of the second Symanzik polynomial. We solve this problem by performing an analytic continuation of the Mandelstam variables such that the second Symanzik polynomial has a definite sign

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Summary

General idea of the method of regions

The procedure of the method of regions is the following [13, 35, 36, 40, 41]:. Step 1: Assign a hierarchy to the dimensionful parameters. The Step 2 is the crucial part of the method of regions, and an algorithm to reveal such scalings for a general integral is established based on the analysis of the convex hull [42, 43]. A new idea to reveal relevant scalings is proposed based on the technique of power geometry, which is implemented in the Mathematica package ASPIRE [44]. In this paper we use asy2.1.m. The practical bottleneck is Step 4, since the integration tends to be complicated even after the expansion if the original integral is very complicated. The practical bottleneck is Step 4, since the integration tends to be complicated even after the expansion if the original integral is very complicated This is one of the reasons why testing the method of regions is difficult. For all the representations mentioned above, one has to follow Step 1 to 5 for practical calculation

Conventions
Kinematics and high energy expansion
A First Example
Expansion in the top quark mass
Higher order terms in mt
Integrals with fewer lines
Template integrals for Regions 2 to 14
Analytic continuation
Solving the Mellin-Barnes integrals
Combining the results
Other master integrals
Summary
A Mellin-Barnes integrals
B Template integrals for the two-loop master integrals of Higgs pair production
C A corollary of the generalized Barnes lemma
Full Text
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