524 research outputs found
New Approach to Parton Shower MC's for Precision QCD Theory: HERWIRI1.0(31)
By implementing the new IR-improved
Dokshitzer-Gribov-Lipatov-Altarelli-Parisi-Callan-Symanzik (DGLAP-CS) kernels
recently developed by one of us in the HERWIG6.5 environment we generate a new
MC, HERWIRI1.0(31), for hadron-hadron scattering at high energies. We use MC
data to illustrate the comparison between the parton shower generated by the
standard DGLAP-CS kernels and that generated by the new IR-improved DGLAP-CS
kernels. The interface to MC@NLO, MC@NLO/HERWIRI, is illustrated. Comparisons
with FNAL data and some discussion of possible implications for LHC
phenomenology are also presented.Comment: 24 pages, 10 figures; published versio
Interplay of IR-Improved DGLAP-CS Theory and NLO Parton Shower MC Precision
We present the interplay between the new IR-improved DGLAP-CS theory and the
precision of NLO parton shower/ME matched MC`s as it is realized by the new MC
Herwiri1.031 in interface to MC@NLO. We discuss phenomenological implications
using comparisons with recent LHC data on single heavy gauge boson production.Comment: 8 pages, 4 figures; presented by BFLW at ICHEP 201
QCD Corrections to Resonant Slepton Production in Hadron Colliders
We consider resonant production of sneutrino and slepton at hadronic colliders such as the Tevatron and the LHC within the context of a R-parity violating supersymmetric model. We present next to leading order QCD corrections to total cross sections which originate from both quark- as well as gluon-initiated processes. For couplings involving only the first generation quarks, the K factor at the Tevatron can be as large as 1.5 for a 100 GeV sfermion and falls to nearly 1.1 as the sfermion mass reaches 1 TeV. At the LHC, the variation is between 1.2 and 1.45 for masses less than 2 TeV. While the dependence on the parton density parametrization is found to be mild, this ceases to be true if the strange quark plays a dominant role in the production process. We also study the renormalization and factorization-scale dependence and find it to be less pronounced for the NLO cros sections as compared to the LO. The results obtained in this article are also applicable to resonant production of any color-neutral scalar
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