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NexttoLeadingOrder Monte Carlo Simulation
 of Diphoton Production in Hadronic Collisions, arXiv:1106.3939 [hepph
"... ar ..."
Nexttoleadingorder temperature corrections to correlators in QCD
, 1994
"... Corrections of order T 4 to vector and axial current correlators in QCD at a finite temperature T < Tc are obtained using dispersion relations for the amplitudes of deep inelastic scattering on pions. Their relation with the operator product expansion is presented. An interpretation of the result ..."
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of the results in terms of Tdependent meson masses is given: masses of ρ and a1 start to move with temperature in order T 4.
Prospects for Charged Higgs Discovery at Colliders
"... For the preparation of the experimental search for charged Higgs bosons at the LHC detailed studies have been made to determine the expected charged Higgs boson production crosssections and decay branching ratios at s = 14 TeV. In the mass regime below the tquark mass the expected production cros ..."
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crosssections are discussed using PYTHIA and FeynHiggs program packages based on the decay t → H+b. For higher masses NexttoLeadingOrder (NLO) calculations have been used, and particular attention has been given to the intermediatemass region. The decay branching ratios have been studied
Crosssections and branching ratios for charged Higgs
, 907
"... For the preparation of the experimental search for charged Higgs bosons at the LHC detailed studies have been made to determine the expected charged Higgs boson production crosssections and decay branching ratios at √ s = 14 TeV. In the mass regime below the tquark mass the expected production cro ..."
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crosssections are discussed using PYTHIA and FeynHiggs program packages based on the decay t → H + b. For higher masses NexttoLeadingOrder (NLO) calculations have been used, and particular attention has been given to the intermediatemass region. The decay branching ratios have been studied
Germany. GAUGEINDEPENDENT EXTRACTION OF THE NEXTTOLEADINGORDER DEBYE MASS FROM THE GLUON PROPAGATOR
, 1993
"... It is shown that by defining the Debye mass through the relevant pole of the static gluon propagator rather than the zeromomentum limit of the timetime component of the gluon selfenergy, a gaugeindependent result for the nexttoleading order correction can be derived upon resummation of hardth ..."
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It is shown that by defining the Debye mass through the relevant pole of the static gluon propagator rather than the zeromomentum limit of the timetime component of the gluon selfenergy, a gaugeindependent result for the nexttoleading order correction can be derived upon resummation of hard
UW/PT 0414 NexttoLeadingOrder Staggered Chiral Perturbation Theory ∗
, 2004
"... We have extended staggered chiral perturbation theory (SχPT) to O(a 2 p 2), O(a 4), and O(a 2 m), the orders necessary for a full nexttoleading order (NLO) calculation of pseudoGoldstone boson (PGB) masses and decay constants including tastesymmetry violations. We present predictions relating SO ..."
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We have extended staggered chiral perturbation theory (SχPT) to O(a 2 p 2), O(a 4), and O(a 2 m), the orders necessary for a full nexttoleading order (NLO) calculation of pseudoGoldstone boson (PGB) masses and decay constants including tastesymmetry violations. We present predictions relating
Determination of the Strange Quark Content of the Nucleon from a NexttoLeadingOrder QCD Analysis of Neutrino Charm Production
, 1994
"... A 94550. 1 We present the first nexttoleadingorder QCD analysis of neutrino charm production, using a sample of 6090  and induced oppositesign dimuon events observed in the CCFR detector at the Fermilab Tevatron. We find that the nucleon strange quark content is suppressed with respect to ..."
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A 94550. 1 We present the first nexttoleadingorder QCD analysis of neutrino charm production, using a sample of 6090  and induced oppositesign dimuon events observed in the CCFR detector at the Fermilab Tevatron. We find that the nucleon strange quark content is suppressed with respect
NexttoLeadingOrder Corrections to Momentum Correlations in Z 0 → b ¯ b
, 1997
"... We recently completed a calculation of the process e + e − →Q ¯ Q + X, where Q is a heavy quark, at order O(α2 s). As a first application of this calculation we compute the momentum correlations of b¯b pairs at nexttoleadingorder. This quantity is interesting since it may affect the determination ..."
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We recently completed a calculation of the process e + e − →Q ¯ Q + X, where Q is a heavy quark, at order O(α2 s). As a first application of this calculation we compute the momentum correlations of b¯b pairs at nexttoleadingorder. This quantity is interesting since it may affect
LargepT Inclusive π 0 Cross Sections and NexttoLeadingOrder QCD Predictions
, 1999
"... We review the phenomenology of π 0 production at large transverse momentum in protoninduced collisions. Uncertainties in the nexttoleadingorder predictions of Quantum Chromodynamics are discussed. The comparison with data reveals that the disagreement between theory and experiment lies essential ..."
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We review the phenomenology of π 0 production at large transverse momentum in protoninduced collisions. Uncertainties in the nexttoleadingorder predictions of Quantum Chromodynamics are discussed. The comparison with data reveals that the disagreement between theory and experiment lies
Thermalization of an Interacting Quantum Field in the CTP2PI Nexttoleadingorder Large N Scheme
, 2002
"... In this paper we use an O(N)invariant scalar field of unbroken symmetry to investigate whether an interacting quantum field at the nexttoleading order Large N approximation may show signs of thermalization. We develop the closed timepath (CTP) twoparticle irreducible (2PI) effective action in p ..."
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In this paper we use an O(N)invariant scalar field of unbroken symmetry to investigate whether an interacting quantum field at the nexttoleading order Large N approximation may show signs of thermalization. We develop the closed timepath (CTP) twoparticle irreducible (2PI) effective action
Results 1  10
of
995,430