Conveners
Session 3: Afternoon Session 1
- Alessandro Vicini (Università degli Studi e INFN Milano (IT))
Session 3: Afternoon Session 3
- Fernando Febres Cordero
Session 3: Afternoon Session 5
- Sally Dawson (BNL)
We present a calculation of the master integrals (MI's) required for the calculation of the Electroweak corrections to $gg\rightarrow \gamma\gamma$ production in which the process contains a light quark loop.
The integrals can be broken down into four categories based on the flow of the heavy vector bosons throughout the loop. Two of the families are planar, and two are non-planar. We...
I will present the computation of the NNLO double-virtual subleading-color corrections to the production of three photons at hadron colliders. I will briefly review the numerical generalized unitarity computation over finite fields performed with the C++ code Caravel, including updates that made this computation possible. I will then formulate the rational reconstruction problem for the finite...
In this talk I will present recent developments on the calculation of five-point scattering amplitudes in massless QCD beyond the leading-colour approximation.
I will discuss the methodology that we pursued to compute these highly non-trivial amplitudes. In this respect, I will argue that it is possible to tackle and tame the seemingly intractable algebraic complexity at each step of the...
We present the analytic result of three-point energy correlator in N=4 SYM and QCD. This is the first analytic computation of trijet event shape observables, which provides precise data for both theoretical analysis and phenomenological studies in jet substructure. The beauty of energy correlator allows us to rationalize all square roots and finish the full four-particle phase space integral....
In my talk, I will discuss the analytical results for a non-planar family of master integrals appearing in NNLO 2-loop diagrams of scattering amplitudes of diphoton and dijet production processes. We use the method of differential equations keeping the full dependence on the top quark's mass running in the loop to obtain the results for these master integrals up to O(\epsilon^4). The top...
