NLO corrections merged with parton showers for Z + 2 jets production using the POWHEG method

[1]  F. Siegert,et al.  W+n-jet predictions at the Large Hadron Collider at next-to-leading order matched with a parton shower. , 2012, Physical review letters.

[2]  Ren-You Zhang,et al.  Next-to-leading order QCD predictions for Z0H0 + jet production at LHC , 2012, Journal of High Energy Physics.

[3]  Pavel Strachota,et al.  Measurement of the production cross section for Z/γ* in association with jets in pp collisions at s√=7 TeV with the ATLAS detector , 2012 .

[4]  Rikkert Frederix,et al.  NLO Higgs boson production plus one and two jets using the POWHEG BOX, MadGraph4 and MCFM , 2012, 1202.5475.

[5]  Frank Siegert,et al.  W+n-Jet Predictions With MC@NLO in Sherpa , 2012 .

[6]  Peter Uwer,et al.  Hadronic top-quark pair-production with one jet and parton showering , 2011, 1110.5251.

[7]  P. Richardson,et al.  Next-to-leading-order Monte Carlo simulation of diphoton production in hadronic collisions , 2011, 1106.3939.

[8]  M. Cacciari,et al.  FastJet user manual , 2011, 1111.6097.

[9]  Frank Siegert,et al.  A critical appraisal of NLO+PS matching methods , 2011, 1111.1220.

[10]  R. Pittau,et al.  aMC@NLO predictions for Wjj production at the Tevatron , 2011, 1110.5502.

[11]  K. Hamilton,et al.  Practical improvements and merging of Powheg simulations for vector boson production , 2011, 1108.0909.

[12]  P. Richardson,et al.  A positive-weight next-to-leading-order Monte Carlo simulation of deep inelastic scattering and Higgs boson production via vector–boson fusion in Herwig++ , 2011, 1106.2983.

[13]  D. Maitre,et al.  Driving Missing Data at Next-to-Leading Order , 2011, 1106.1423.

[14]  F. Taylor,et al.  Measurement of the production cross section for W-bosons in association with jets in pp collisions at √s = 7 TeV with the ATLAS detector , 2011 .

[15]  Z. Trocsanyi,et al.  Top quark pair production in association with a jet at NLO accuracy with parton showering , 2011, 1101.2672.

[16]  Simone Alioli,et al.  Jet pair production in POWHEG , 2010, 1012.3380.

[17]  E. Re,et al.  Vector boson plus one jet production in POWHEG , 2010, 1009.5594.

[18]  E. Re,et al.  A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX , 2010, 1002.2581.

[19]  M. Huber,et al.  A proposal for a standard interface between Monte Carlo tools and one-loop programs , 2010, Comput. Phys. Commun..

[20]  P. Nason,et al.  NLO Higgs boson production via vector-boson fusion matched with shower in POWHEG , 2009, 0911.5299.

[21]  J. Winter,et al.  Event generation with , 2009 .

[22]  F. Siegert,et al.  Event generation with SHERPA 1.1 , 2008, 0811.4622.

[23]  D. Maitre,et al.  An Automated Implementation of On-shell Methods for One-Loop Amplitudes , 2008, 0803.4180.

[24]  M. Cacciari,et al.  The anti-$k_t$ jet clustering algorithm , 2008, 0802.1189.

[25]  P. Nason,et al.  Matching NLO QCD computations with Parton Shower simulations: the POWHEG method , 2007, 0709.2092.

[26]  G. Ridolfi,et al.  A Positive-weight next-to-leading-order Monte Carlo for heavy flavour hadroproduction , 2007, 0707.3088.

[27]  Tim Stelzer,et al.  MadGraph/MadEvent v4: The New Web Generation , 2007, 0706.2334.

[28]  M. Cacciari,et al.  Dispelling the N3 myth for the kt jet-finder , 2005, hep-ph/0512210.

[29]  P. Nason.  A new method for combining NLO QCD with shower Monte Carlo algorithms , 2004, hep-ph/0409146.

[30]  C. Oleari,et al.  QCD corrections to electroweak nu(l) j j and l+ l- j j production , 2003, hep-ph/0310156.

[31]  J. Campbell,et al.  Next-to-leading order QCD predictions for $W$ + 2 jet and $Z$ + 2 jet production at the CERN LHC , 2003, hep-ph/0308195.

[32]  P. Nason,et al.  Matching NLO QCD and parton showers in heavy flavour production , 2003, hep-ph/0305252.

[33]  S. Frixione,et al.  Matching NLO QCD computations and parton shower simulations , 2002, hep-ph/0204244.

[34]  J. Campbell,et al.  Next-to-leading order corrections to $W^+$ 2 jet and $Z^+$ 2 jet production at hadron colliders , 2002, hep-ph/0202176.

[35]  J. Huston,et al.  New generation of parton distributions with uncertainties from global QCD analysis , 2002, hep-ph/0201195.

[36]  G. Soff,et al.  AMEGIC++ 1.0: A Matrix element generator in C++ , 2001, hep-ph/0109036.

[37]  T. Plehn,et al.  Determining the structure of Higgs couplings at the CERN LargeHadron Collider. , 2001, Physical review letters.

[38]  T. Plehn,et al.  A Method for identifying $H\to\tau^+\tau^-\to e^\pm \mu^\mp p_T$ at the CERN LHC , 1999, hep-ph/9911385.

[39]  K. Hagiwara,et al.  Searching for $H\to\tau^+\tau^-$ in weak boson fusion at the CERN LHC , 1998, hep-ph/9808468.

[40]  L. Dixon,et al.  ONE-LOOP AMPLITUDES FOR E+E- TO FOUR PARTONS , 1997, hep-ph/9708239.

[41]  D. Rainwater,et al.  Probing color-singlet exchange in Z+2-jet events at the CERN LHC. , 1996, Physical review. D, Particles and fields.

[42]  K. Hagiwara,et al.  Amplitudes for multi-parton processes involving a current at e+e−, e±p, and hadron colliders , 1989 .

[43]  K. Hagiwara,et al.  Helicity amplitudes for heavy lepton production in e+e− annihilation☆ , 1986 .