Abstract:During the last several years, remarkable progress has been made in numerical calculations of dimensionally regulated multi-loop Feynman diagrams using Mellin-Barnes (MB) representations. The bottlenecks were non-planar diagrams and Minkowskian kinematics. The method has been proved to work in a highly non-trivial physical application (two-loop electroweak bosonic corrections to the Z → bb decay), and cross-checked with the sector decomposition (SD) approach. In fact, both approaches have their pros and cons. … Show more
“…However, more advanced integration algorithms may help to improve the accuracy reached on a reasonable time scale even for such high dimensional MB integrals. For recent developments in that direction, see [14,15]. All numerical values also agree with independent results of the sector decomposition implementation FIESTA [31].…”
In this paper, we present a new approach to the construction of Mellin-Barnes representations for Feynman integrals inspired by the Method of Brackets. The novel technique is helpful to lower the dimensionality of MellinBarnes representations in complicated cases, some examples are given.
“…However, more advanced integration algorithms may help to improve the accuracy reached on a reasonable time scale even for such high dimensional MB integrals. For recent developments in that direction, see [14,15]. All numerical values also agree with independent results of the sector decomposition implementation FIESTA [31].…”
In this paper, we present a new approach to the construction of Mellin-Barnes representations for Feynman integrals inspired by the Method of Brackets. The novel technique is helpful to lower the dimensionality of MellinBarnes representations in complicated cases, some examples are given.
“…For crossed topologies, the situation is more complicated as one encounters cases in which the loop-by-loop approach yields polynomials in the Feynman parameters x i which are not positive definite, even in the absence of kinematic thresholds. Consequently, the MB integrals will be highly oscillating and hence their numerical evaluation will be difficult to handle, although steps in this direction have been undertaken [125][126][127][128].…”
The four-loop Sudakov form factor in maximal super Yang-Mills theory is analysed in detail. It is shown explicitly how to construct a basis of integrals that have a uniformly transcendental expansion in the dimensional regularisation parameter, further elucidating the number-theoretic properties of Feynman integrals. The physical form factor is expressed in this basis for arbitrary colour factor. In the nonplanar sector the required integrals are integrated numerically using a mix of sector-decomposition and Mellin-Barnes representation methods. Both the cusp as well as the collinear anomalous dimension are computed. The results show explicitly the violation of quadratic Casimir scaling at the four-loop order. A thorough analysis concerning the reliability of reported numerical uncertainties is carried out.
“…In the second step, a completely new software MBnumerics.m has been used [64]. In the next section some core ideas which made possible to calculate MB integrals in Minkowskian regions used in MBnumerics.m are given.…”
Section: Pos(ll2016)034mentioning
confidence: 99%
“…Automatic algorithms for finding the suitable shifts and contour deformations are implemented in MBnumerics.m [64]. At the moment an effective strategy is: Starting from original n−dimensional MB integrals, MBnumerics.m looks for well converging n − 1 and n − 2 integrals, and remaining n−dimensional integrals.…”
Mellin-Barnes (MB) techniques applied to integrals emerging in particle physics perturbative calculations are summarized. New versions of AMBRE packages which construct planar and nonplanar MB representations are shortly discussed. The numerical package MBnumerics.m is presented for the first time which is able to calculate with a high precision multidimensional MB integrals in Minkowskian regions. Examples are given for massive vertex integrals which include threshold effects and several scale parameters.
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