activity
20002016
most citedFeynman Rules for the Rational Part of the QCD 1-loop amplitudes

141 citations · 465 across the 19 of their papers we have counts for

collaborators

20 papers

hep-ph2016★ 1 cited

Attacking One-loop Multi-leg Feynman Integrals with the Loop-Tree Duality

Grigorios Chachamis, Sebastian Buchta, Petros Draggiotis +1

We discuss briefly the first numerical implementation of the Loop-Tree Duality (LTD) method. We apply the LTD method in order to calculate ultraviolet and infrared finite multi-leg…

hep-ph2015★ 1 cited

First Numerical Implementation of the Loop-Tree Duality Method

Sebastian Buchta

The Loop-Tree Duality (LTD) is a novel perturbative method in QFT that establishes a relation between loop-level and tree-level amplitudes, which gives rise to the idea of treating…

hep-ph2015★ 11 cited

Numerical implementation of the Loop-Tree Duality method

Sebastian Buchta, Grigorios Chachamis, Petros Draggiotis +1

We present a first numerical implementation of the Loop-Tree Duality (LTD) method for the direct numerical computation of multi-leg one-loop Feynman integrals. We discuss in detail…

hep-ph2015

Towards a Numerical Implementation of the Loop-Tree Duality Method

Sebastian Buchta, Grigorios Chachamis, Petros Draggiotis +2

We review the recent progress on the numerical implementation of the Loop-Tree Duality Method (LTDM) for the calculation of scattering amplitudes. A central point is the analysis o…

hep-ph2014★ 3 cited

The loop-tree duality at work

Sebastian Buchta, Grigorios Chachamis, Ioannis Malamos +3

We review the recent developments of the loop-tree duality method, focussing our discussion on analysing the singular behaviour of the loop integrand of the dual representation of…

hep-ph2014★ 56 cited

On the singular behaviour of scattering amplitudes in quantum field theory

Sebastian Buchta, Grigorios Chachamis, Petros Draggiotis +2

We analyse the singular behaviour of one-loop integrals and scattering amplitudes in the framework of the loop--tree duality approach. We show that there is a partial cancellation…