One can use more than one scale variable to specify the family of surfaces in the space of parton splitting parameters that define the evolution of a parton shower. Considering $e^+e^-$ annihilation, we use two variables, with shower evolution following a special path in this two dimensional space. In addition, we treat in a special way the part of the splitting function that has a soft emission singularity but no collinear singularity. This leads to certain advantages compared to the usual shower formulation with only one scale variable
Abstract We present a parton shower which implements the DGLAP evolution of parton densities and fra...
It is useful to describe a leading order parton shower as the solution of a linear equation that spe...
We present a method to match the multi-parton states generated by the High Energy Jets Monte Carlo w...
One can use more than one scale variable to specify the family of surfaces in the space of parton sp...
One can use more than one scale variable to define the family of surfaces in the space of parton spl...
When the initial state evolution of a parton shower is organized according to the standard “backward...
Initial state evolution in parton shower event generators involves parton distribution functions. We...
We introduce a general framework to construct multi-emission kernels for parton branching algorithms...
Away from the strictly soft and collinear limit of QCD radiation the choice of evolution scale in a ...
We propose a simple scheme to start a parton-shower evolution description from a given jet configura...
We present a formulation for a parton shower at an arbitrary order of perturbation theory, with the ...
In this note we outline the Monte Carlo project {\tt KrkMC}. The goal of this project is to construc...
We present a simple parton-shower model that replaces the explicit angular ordering of the coherent ...
We present a model that includes the production of arbitrarily many jets in lepton-hadron events, us...
Programs that calculate observables in quantum chromodynamics at next-to-leading order typically suf...
Abstract We present a parton shower which implements the DGLAP evolution of parton densities and fra...
It is useful to describe a leading order parton shower as the solution of a linear equation that spe...
We present a method to match the multi-parton states generated by the High Energy Jets Monte Carlo w...
One can use more than one scale variable to specify the family of surfaces in the space of parton sp...
One can use more than one scale variable to define the family of surfaces in the space of parton spl...
When the initial state evolution of a parton shower is organized according to the standard “backward...
Initial state evolution in parton shower event generators involves parton distribution functions. We...
We introduce a general framework to construct multi-emission kernels for parton branching algorithms...
Away from the strictly soft and collinear limit of QCD radiation the choice of evolution scale in a ...
We propose a simple scheme to start a parton-shower evolution description from a given jet configura...
We present a formulation for a parton shower at an arbitrary order of perturbation theory, with the ...
In this note we outline the Monte Carlo project {\tt KrkMC}. The goal of this project is to construc...
We present a simple parton-shower model that replaces the explicit angular ordering of the coherent ...
We present a model that includes the production of arbitrarily many jets in lepton-hadron events, us...
Programs that calculate observables in quantum chromodynamics at next-to-leading order typically suf...
Abstract We present a parton shower which implements the DGLAP evolution of parton densities and fra...
It is useful to describe a leading order parton shower as the solution of a linear equation that spe...
We present a method to match the multi-parton states generated by the High Energy Jets Monte Carlo w...