Перейти к основному содержанию
AkademIndex

Продукты

Для разработчиков

AkademBaseОткрытый API экосистемы
Статья

Combining higher-order resummation with multiple NLO calculations and parton showers in GENEVA

Simone AlioliUniversity of CaliforniaC. BauerErnest Orlando Lawrence Berkeley National Laboratory, University of California, Berkeley, CA, 94720, U.S.ACalvin BerggrenErnest Orlando Lawrence Berkeley National Laboratory, University of California, Berkeley, CA, 94720, U.S.AAndrew HornigDepartment of Physics, University of Washington, Seattle, WA, 98195, U.S.AFrank J. TackmannTheory Group, Deutsches Elektronen-Synchrotron (DESY), D-22607, Hamburg, GermanyChristopher K. VermilionErnest Orlando Lawrence Berkeley National Laboratory, University of California, Berkeley, CA, 94720, U.S.AJonathan R. WalshErnest Orlando Lawrence Berkeley National Laboratory, University of California, Berkeley, CA, 94720, U.S.ASaba ZuberiErnest Orlando Lawrence Berkeley National Laboratory, University of California, Berkeley, CA, 94720, U.S.A
2013en
ABI

Аннотация

A bstract We extend the lowest-order matching of tree-level matrix elements with parton showers to give a complete description at the next higher perturbative accuracy in α s at both small and large jet resolutions, which has not been achieved so far. This requires the combination of the higher-order resummation of large Sudakov logarithms at small values of the jet resolution variable with the full next-to-leading-order (NLO) matrix-element corrections at large values. As a by-product, this combination naturally leads to a smooth connection of the NLO calculations for different jet multiplicities. In this paper, we focus on the general construction of our method and discuss its application to e + e − and pp collisions. We present first results of the implementation in the Geneva Monte Carlo framework. We employ N -jettiness as the jet resolution variable, combining its next-to-next-to-leading logarithmic resummation with fully exclusive NLO matrix elements, and Pythia 8 as the backend for further parton showering and hadronization. For hadronic collisions, we take Drell-Yan production as an example to apply our construction. For e + e − → jets, taking α s ( m Z ) = 0.1135 from fits to LEP thrust data, together with the Pythia 8 hadronization model, we obtain good agreement with LEP data for a variety of 2-jet observables.

Перевод пока недоступен

Идентификаторы

Цитирования и источники

Цитирований: 2Использованных источников: 0