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Studying the “Underlying Event” at CDF
“Leading Jet” vs Z-Boson
Rick Field University of Florida
Outline of Talk CDF Run 2
◻The “Towards”, “Away”, and “Transverse” regions of η-φ space.
◻Four Jet Topologies.
◻The “transMAX” and “transMIN” regions.
◻The “underlying event” in Drell-Yan production.
“Leading Jet”
Proton
Underlying Event
Outgoing Parton
Final-State Radiation
Outgoing Parton
PT(hard)
Initial-State Radiation AntiProton
Underlying Event
◻The observables: First look at average quantities. Then do Drell-Yan Production Lepton distributions.
◻Look at
versus Nchg in “min-bias” and Drell-Yan.
Proton
Underlying Event
AntiProton
Underlying Event
◻Show some extrapolations of Drell-Yan to the LHC.
Anti-Lepton
Fourth HERA-LHC Workshop Rick Field – Florida/CDF/CMS Page 1 May 26-30, 2008
Studying the “Underlying Event” at CDF
“Leading Jet” vs Z-Boson
Rick Field University of Florida
Outline of Talk CDF Run 2
The goal is to produce data (corrected to the
particle level) that can be used by the theorists to tune and improve the QCD Monte-Carlo models that are used to simulate hadron-hadront
◻The “transMAX” and “transMIN” regions.
Outgoing Parton
PT(hard)
Initial-State Radiation AntiProton
Underlying Event
◻The “underlying event” in Drell-Yan production. ield Outgoing Parton
Final-State Radiation
◻The observables: First look at average quantities. Then do Drell-Yan Production distributions. Deepak Kar
◻Look-at versus Nchg in “min-bias” and Underlying Event
Lepton
AntiProton
Underlying Event
◻Show some extrapolations of Drell-Yan to the LHC.
Anti-Lepton
Fourth HERA-LHC Workshop Rick Field – Florida/CDF/CMS Page 2 May 26-30, 2008
QCD Monte-Carlo Models: High Transverse Momentum Jets
Hard Scattering
Initial-State Radiation
Outgoing Parton
PT(hard)
Hard Scattering
Initial-State Radiation
Outgoing Parton
PT(hard) “Hard Scattering” Component
Proton
Underlying Event
AntiProton
Underlying Event
Final-State Radiation
Outgoing Parton
Final-State Radiation
Outgoing Parton
Proton
Underlying Event
AntiProton
Underlying Event
“Underlying Event”
◻Start with the perturbative 2-to-2 (or sometimes 2-to-3) parton-parton scattering and add initial and final-state gluon radiation (in the leading log approximation or modified leading log approximation).
◻The “underlying event” consists of the “beam-beam remnants” and from particles arising from soft or semi-soft multiple parton interactions (MPI).
◻Of course the outgoing colored partons fragment into hadron “jet” and inevitably “underlying event” observables receive contributions from initial and final-state radiation.
Fourth HERA-LHC Workshop Rick Field – Florida/CDF/CMS Page 3 May 26-30, 2008
QCD Monte-Carlo Models: High Transverse Momentum Jets
Hard Scattering
Initial-State Radiation
Outgoing Parton
PT(hard)
Hard Scattering “Jet” Outgoing Parton
Initial-State Radiation PT(hard) “Hard Scattering” Component
Proton
Underlying Event
AntiProton
Underlying Event
Final-State Radiation
Outgoing Parton
“Final-State Radiation
Outgoing Parton
Proton
Underlying Event
AntiProton
Underlying Event
“Underlying Event”
◻Start with the perturbative 2-to-2 (or sometimes 2-to-3) parton-parton scattering and add initial and final-state gluon radiation (in the leading log approximation or modified leading log approximation).
◻The “underlying event” consists of the “beam-beam remnants” and from particles arising from soft or semi-soft multiple parton interactions (MPI).
◻Of course the outgoing colored partons fragment into hadron i“jet” andi inevitably “underlying event” observables receive contributions from initial and final-state radiation.ads to
more precise collider measurements!
Fourth HERA-LHC Workshop Rick Field – Florida/CDF/CMS Page 4 May 26-30, 2008
QCD Monte-Carlo Models: Lepton-Pair Production
Lepton-Pair Production Anti-Lepton
Initial-State Radiation
Lepton-Pair Production Anti-Lepton
Initial-State Radiation
“Hard Scattering” Component
Proton
Underlying Event
AntiProton
Lepton
Underlying Event
Proton
Lepton Underlying Event
AntiProton
Underlying Event
“Underlying Event”
◻Start with the perturbative Drell-Yan muon pair production and add initial-state gluon radiation (in the leading log approximation or modified leading log approximation).
◻The “underlying event” consists of the “beam-beam remnants” and from particles arising from soft or semi-soft multiple parton interactions (MPI).
◻Of course the outgoing colored partons fragment into hadron “jet” and inevitably “underlying event” observables receive contributions from initial and final-state radiation.
Fourth HERA-LHC Workshop Rick Field – Florida/CDF/CMS Page 5 May 26-30, 2008
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