We are developing NLO event generators for hadron collision interactions based on the limited leading-log (LLL) subtraction method. In this method, a boundary between non-radiative and radiative processes necessarily appears at the factorization scale ($\mu_{F}$). The radiation effects are simulated using a parton shower (PS) in non-radiative processes. It is therefore crucial in our method to apply a PS which well reproduces the radiation activities evaluated from the matrix-element (ME) calculations for radiative processes. The PS activity depends on the applied kinematics model. In this paper we introduce two models for our simple initial-state leading-log PS: a model similar to the "old" PYTHIA-PS and a $p_{T}$-prefixed model with a $p_...
We present a new approach to combine multiple NLO parton-level calculations matched to parton shower...
AbstractA new method of including NLO QCD corrections to the hard process in the LO Monte Carlo (MC)...
We present an algorithm to combine multiple matrix elements at LO and NLO with a parton shower. We b...
A new method to construct event-generators based on next-to-leading order QCD matrix-elements and le...
We present a next-to-leading order (NLO) calculation of t t ¯ $$ t\overline{t} $$ production in hadr...
The decade-old technique of combining NLO-corrected hard process with LO-level parton shower Monte C...
We present a new approach to combine multiple NLO parton-level calculations matched to parton shower...
We propose a scheme that could offer a convenient Monte Carlo sampling of next-to-leading-order matr...
We present a next-to-leading order (NLO) calculation of tt¯ production in hadronic collisions int...
We compare different procedures for combining fixed-order tree-level matrix-element generators with ...
We report on our exploration of matching matrix element calculations with the parton-shower models ...
The decade-old technique of combining NLO-corrected hard process with LO-level parton shower Monte C...
The accuracy of parton-shower simulations is often a limiting factor in the interpretation of data f...
In recent times the algorithms for the simulation of hadronic collisions have been subject to two su...
Comparisons of experimental data with theoretical predictions for collider processes containing hadr...
We present a new approach to combine multiple NLO parton-level calculations matched to parton shower...
AbstractA new method of including NLO QCD corrections to the hard process in the LO Monte Carlo (MC)...
We present an algorithm to combine multiple matrix elements at LO and NLO with a parton shower. We b...
A new method to construct event-generators based on next-to-leading order QCD matrix-elements and le...
We present a next-to-leading order (NLO) calculation of t t ¯ $$ t\overline{t} $$ production in hadr...
The decade-old technique of combining NLO-corrected hard process with LO-level parton shower Monte C...
We present a new approach to combine multiple NLO parton-level calculations matched to parton shower...
We propose a scheme that could offer a convenient Monte Carlo sampling of next-to-leading-order matr...
We present a next-to-leading order (NLO) calculation of tt¯ production in hadronic collisions int...
We compare different procedures for combining fixed-order tree-level matrix-element generators with ...
We report on our exploration of matching matrix element calculations with the parton-shower models ...
The decade-old technique of combining NLO-corrected hard process with LO-level parton shower Monte C...
The accuracy of parton-shower simulations is often a limiting factor in the interpretation of data f...
In recent times the algorithms for the simulation of hadronic collisions have been subject to two su...
Comparisons of experimental data with theoretical predictions for collider processes containing hadr...
We present a new approach to combine multiple NLO parton-level calculations matched to parton shower...
AbstractA new method of including NLO QCD corrections to the hard process in the LO Monte Carlo (MC)...
We present an algorithm to combine multiple matrix elements at LO and NLO with a parton shower. We b...