51 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida
|
|
- Tabitha Tyler
- 6 years ago
- Views:
Transcription
1 5 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida Lecture : Outline Review: The CDF Tevatron underlying event tunes (Tune A, B, D, AW, DW, D6, DWT, D6T). Predicting the behavior of the underlying event at the LHC. What we expected to see. How well did we do at predicting the behavior of the underlying event at the LHC ( and )? LHC PYTHIA Tunes: PYTHIA 6.4 tunes (AMBT, Z, Z2) and PYTHIA 8 Tune C4. Proton Underlying Event Outgoing Parton Final-State Radiation UE&MB@CMS Outgoing Parton PT(hard) Initial-State Radiation Proton Underlying Event Zakopane, Poland, June -9, 20 CMS ATLAS Rick Field Florida/CDF/CMS Page
2 5 st Cracow School of Theoretical Physics The Soft Side of the LHC Min-Bias and the Underlying Event at the LHC Rick Field University of Florida Lecture 2: Tomorrow How are min-bias collisions related to the underlying event. How well did we do at predicting the behavior of minbias collisions at the LHC ( and )? Baryon and Strange Particle Production at the LHC: Fragmentation tuning. p K + K Λ short u u d u s d s + d s u d s K - u s UE&MB@CMS Ξ d s s Zakopane, Poland, June -9, 20 CMS ATLAS Rick Field Florida/CDF/CMS Page 2
3 Toward an Understanding of Hadron-Hadron Collisions From Feynman-Field to the LHC Rick Field University of Florida Lecture 3: Tuesday Evening Before Feynman-Field Phenomenology: The Berkeley years. Feynman The early days of Feynman-Field Phenomenology. From 7 GeV/c π 0 s to TeV Jets! Field Rick Field Florida/CDF/CMS Page 3
4 QCD Monte-Carlo Models: High Transverse Momentum Jets Hard Scattering Outgoing Parton Initial-State Radiation PT(hard) Hard Scattering Jet Jet Initial-State Radiation Outgoing Parton PT(hard) Hard Scattering Component Proton Underlying Event AntiProton Underlying Event Outgoing Parton Final-State Radiation Outgoing Parton Jet Final-State Radiation 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 finalstate 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). The underlying event is an unavoidable Of course the outgoing colored partons fragment into hadron jet and inevitably underlying event background to most collider observables observables receive contributions from initial and final-state radiation. and having good understand of it leads to more precise collider measurements! Rick Field Florida/CDF/CMS Page 4
5 MPI, Pile-Up, and Overlap MPI: Multiple Parton Interactions Outgoing Parton PT(hard) Initial-State Radiation Proton Proton MPI: Additional 2-to-2 parton-parton scatterings within a single hadron-hadron collision. Underlying Event Underlying Event Outgoing Parton Final-State Radiation Pile-Up Proton Pile-Up Proton Proton Primary Proton Interaction Region z Pile-Up: More than one hadron-hadron collision in the beam crossing. Overlap Overlap: An experimental timing issue where a hadron-hadron collision from the next beam crossing gets included in the hadronhadron collision from the current beam crossing because the next crossing happened before the event could be read out. Rick Field Florida/CDF/CMS Page 5
6 Traditional Approach Transverse region very sensitive to the underlying event! CDF Run Analysis Charged Jet # Direction Toward-Side Jet φ Charged Particle φ Correlations P T > PT min η < η cut Leading Object Direction φ 2π Leading Calorimeter Jet or Leading Charged Particle Jet or Leading Charged Particle or Z-Boson Away Region Transverse Region Toward Toward φ Leading Object Transverse Transverse Transverse Transverse Toward Region Away Away Transverse Region Away-Side Jet Away Region 0 -η cut η +η cut Look at charged particle correlations in the azimuthal angle φ relative to a leading object (i.e. CaloJet#, ChgJet#, PTmax, Z-boson). For CDF PTmin = GeV/c η cut =. Define φ φ < 60 o as Toward, 60 o < φ φ < 20 o as Transverse, and φ φ > 20 o as Away. All three regions have the same area in η-φ space, η φ φ = 2η cut 20 o = 2η cut 2π/3. Construct densities by dividing by the area in η-φ space. Rick Field Florida/CDF/CMS Page 6
7 Charged Jet # Direction Transverse Toward Away φ Transverse Beam-Beam Remnants ISAJET 7.32 (without MPI) Transverse Density ISAJET uses a naïve leading-log parton shower-model which does not agree with the data! "Transverse" Charged Density CDF Run Data data uncorrected theory corrected "Remnants" Isajet February 25, PT(charged jet#) (GeV/c) "Hard".8 TeV η <.0 PT> GeV ISAJET Hard Component Plot shows average transverse charge particle density ( η <, p T > GeV) versus P T (charged jet#) compared to the QCD hard scattering predictions of ISAJET 7.32 (default parameters with P T (hard)>3 GeV/c). The predictions of ISAJET are divided into two categories: charged particles that arise from the break-up of the beam and target (beam-beam remnants); and charged particles that arise from the outgoing jet plus initial and final-state radiation (hard scattering component). Rick Field Florida/CDF/CMS Page 7
8 Charged Jet # Direction Transverse Toward Away Beam-Beam Remnants φ Transverse HERWIG 6.4 (without MPI) Transverse Density "Transverse" Charged Density HERWIG uses a modified leadinglog parton shower-model which does agrees better with the data! CDF Run Data data uncorrected theory corrected Total "Remnants" "Hard" PT(charged jet#) (GeV/c) Herwig 6.4 CTEQ5L PT(hard) > 3 GeV/c.8 TeV η <.0 PT> GeV HERWIG Hard Component Plot shows average transverse charge particle density ( η <, p T > GeV) versus P T (charged jet#) compared to the QCD hard scattering predictions of HERWIG 5.9 (default parameters with P T (hard)>3 GeV/c without MPI). The predictions of HERWIG are divided into two categories: charged particles that arise from the break-up of the beam and target (beam-beam remnants); and charged particles that arise from the outgoing jet plus initial and final-state radiation (hard scattering component). Rick Field Florida/CDF/CMS Page 8
9 Parameter Default Tuning PYTHIA 6.2: Multiple Parton Interaction Parameters Description PARP(83) PARP(84) PARP(85) Double-Gaussian: Fraction of total hadronic matter within PARP(84) Double-Gaussian: Fraction of the overall hadron radius containing the fraction PARP(83) of the total hadronic matter. Probability that the MPI produces two gluons with color connections to the nearest neighbors. Hard Core Color String Multiple Parton Interaction Color String PARP(86) 0.66 Probability that the MPI produces two gluons either as described by PARP(85) or as a closed gluon loop. The remaining fraction consists of quark-antiquark pairs. Multiple Parton Determine Interaction by comparing with 630 GeV data! Color String PARP(89) PARP(82) PARP(90) TeV.9 GeV/c 0.6 Determines the reference energy E 0. The cut-off P T0 that regulates the 2-to-2 scattering divergence /PT 4 /(PT 2 +P T0 2 ) 2 Determines the energy dependence of the cut-off P T0 as follows P T0 (E cm ) = P T0 (E cm /E 0 ) ε with ε = PARP(90) PT0 (GeV/c) PYTHIA Hard-Scattering Cut-Off PT0 Take E 0 =.8 TeV ε = 0.25 (Set A)) PARP(67).0 A scale factor that determines the maximum parton virtuality for space-like showers. The larger the value of PARP(67) the more initialstate radiation. ε = 0.6 (default) 00,000 0,000 00,000 Reference point at.8 TeV CM Energy W (GeV) Rick Field Florida/CDF/CMS Page 9
10 Parameter Default Tuning PYTHIA 6.2: Multiple Parton Interaction Parameters Description PARP(83) PARP(84) PARP(85) Double-Gaussian: Fraction of total hadronic matter within PARP(84) Double-Gaussian: Fraction of the overall hadron radius containing the fraction PARP(83) of the total hadronic matter. Determines the energy Probability that the MPI produces two gluons dependence of the MPI! with color connections to the nearest neighbors. Hard Core Color String Multiple Parton Interaction Color String PARP(86) 0.66 Probability that Affects the MPI the produces amount two of gluons either as described initial-state by PARP(85) radiation! or as a closed gluon loop. The remaining fraction consists of quark-antiquark pairs. Multiple Parton Determine Interaction by comparing with 630 GeV data! Color String PARP(89) PARP(82) PARP(90) TeV.9 GeV/c 0.6 Determines the reference energy E 0. The cut-off P T0 that regulates the 2-to-2 scattering divergence /PT 4 /(PT 2 +P T0 2 ) 2 Determines the energy dependence of the cut-off P T0 as follows P T0 (E cm ) = P T0 (E cm /E 0 ) ε with ε = PARP(90) PT0 (GeV/c) PYTHIA Hard-Scattering Cut-Off PT0 Take E 0 =.8 TeV ε = 0.25 (Set A)) PARP(67).0 A scale factor that determines the maximum parton virtuality for space-like showers. The larger the value of PARP(67) the more initialstate radiation. ε = 0.6 (default) 00,000 0,000 00,000 Reference point at.8 TeV CM Energy W (GeV) Rick Field Florida/CDF/CMS Page 0
11 PYTHIA default parameters Parameter MSTP(8) MSTP(82) PARP(8) PARP(82) PARP(89) PARP(90) PARP(67) PYTHIA Defaults MPI constant probability , , , "Transverse" Charged Density scattering CDF Data data uncorrected theory corrected Pythia (default) MSTP(82)= PARP(8) =.9 GeV/c PT(charged jet#) (GeV/c).8 TeV η <.0 PT> GeV CTEQ3L CTEQ4L CTEQ5L CDF Min-Bias CDF JET20 Plot shows the Transverse charged particle density versus P T (chgjet#) compared to the QCD hard scattering predictions of PYTHIA (P T (hard) > 0) using the default parameters for multiple parton interactions and CTEQ3L, CTEQ4L, and CTEQ5L. Note Change PARP(67) = 4.0 (< 6.38) PARP(67) =.0 (> 6.38) Default parameters give very poor description of the underlying event! Rick Field Florida/CDF/CMS Page
12 PYTHIA CTEQ5L Parameter MSTP(8) MSTP(82) PARP(82) PARP(83) PARP(84) PARP(85) PARP(86) PARP(89) PARP(90) PARP(67) Tune B.0.8 TeV New PYTHIA default (less initial-state radiation) 4.9 GeV.0 Run PYTHIA Tune A Tune A GeV TeV CDF Default Feburary 25, 2000! "Transverse" Charged Density CDF Preliminary data uncorrected theory corrected CTEQ5L Plot shows the transverse charged particle density versus P T (chgjet#) compared to the QCD hard scattering predictions of two tuned versions of PYTHIA (CTEQ5L, Set B (PARP(67)=) and Set A (PARP(67)=4)). Old PYTHIA default (more initial-state radiation) PYTHIA (Set B) PARP(67)= PYTHIA (Set A) PARP(67)= PT(charged jet#) (GeV/c) Run Analysis.8 TeV η <.0 PT> GeV Rick Field Florida/CDF/CMS Page 2
13 Transverse Cones vs Transverse Regions φ 2π Away Region Transverse Region Leading Jet Toward Region Transverse Region Away Region 0 - η + Transverse Cone: π(0.7) 2 =9π Transverse Region: 2π/3=0.67π φ 2π Cone Leading Jet Cone 2 P T 90 (GeV/c) 0 - η Cone Analysis (Tano, Kovacs, Huston, Bhatti) MAX Data CDF PRELIMINARY MAX Herwig+QFL MAX Pythia6.5+QFL (tuned) MIN Data MIN Herwig+QFL MIN Pythia6.5+QFL (tuned) Sum the P T of charged particles in two cones of radius 0.7 at the same η as the leading jet but with Φ Φ = 90 o. Plot the cone with the maximum and minimum PT sum versus the E T of the leading (calorimeter) jet E T of leading jet (GeV) Rick Field Florida/CDF/CMS Page 3
14 P T 90 (GeV/c) CDF PRELIMINARY MAX Data MAX Herwig+QFL MAX Pythia6.5+QFL (tuned) MIN Data MIN Herwig+QFL MIN Pythia6.5+QFL (tuned) Energy Dependence of the Underlying Event Cone Analysis 6 (Tano, Kovacs, Huston, Bhatti) 630 GeV P T 90 (GeV/c),800 GeV PYTHIA 6.5 P T0 =.4 GeV MAX Data CDF PRELIMINARY MAX Herwig+QFL MAX Pythia6.5+QFL (tuned) MIN Data MIN Herwig+QFL MIN Pythia6.5+QFL (tuned) E T of leading Jet (GeV) PYTHIA 6.5 P T0 = 2.0 GeV Sum the P T of charged particles (p T > GeV/c) in two cones of radius 0.7 at the same η as the leading jet but with Φ Φ = 90 o. Plot the cone with the maximum and minimum PT sum versus the E T of the leading (calorimeter) jet. Note that PYTHIA 6.5 is tuned at 630 GeV with P T0 =.4 GeV and at,800 GeV with P T0 = 2.0 GeV. This implies that ε = PARP(90) should be around 0.30 instead of the 0.6 (default). For the MIN cone 0.25 GeV/c in radius R = 0.7 implies a PT sum density of dpt sum /dηdφ = 0.6 GeV/c and.4 GeV/c in the MAX cone implies dpt sum /dηdφ = 0.9 GeV/c (average PT sum density of 4 GeV/c per unit η-φ) E T of leading jet (GeV) Rick Field Florida/CDF/CMS Page 4
15 Transverse Charged Densities Energy Dependence Charged PTsum Density (GeV) "Transverse" Charged PTsum Density: dptsum/dηdφ 0.60 ε = 0.25 HERWIG ε = ε = 0 CTEQ5L Pythia (Set A) 630 GeV η <.0 PT> GeV PT(charged jet#) (GeV/c) Charged PTsum Density (GeV) "Min Transverse" PTsum Density: dptsum/dηdφ 0.3 Pythia (Set A) HERWIG 6.4 ε = CTEQ5L ε = 0.6 ε = GeV η <.0 PT> GeV PT(charged jet#) (GeV/c) Shows the transverse charged PT sum density ( η <, P T > GeV) versus P T (charged jet#) at 630 GeV predicted by HERWIG 6.4 (P T (hard) > 3 GeV/c, CTEQ5L) and a tuned version of PYTHIA (P T (hard) > 0, CTEQ5L, Set A, ε = 0, ε = 0.6 (default) and ε = 0.25 (preferred)). Also shown are the PT sum densities (0.6 GeV/c and 4 GeV/c) determined from the Tano, Kovacs, Huston, and Bhatti transverse cone analysis at 630 GeV. PT0 (GeV/c) PYTHIA Hard-Scattering Cut-Off PT0 00,000 0,000 00,000 Reference point E 0 =.8 TeV ε = 0.25 (Set A)) ε = 0.6 (default) CM Energy W (GeV) Rick Field Florida/CDF/CMS Page 5
16 Charged PTsum Density (GeV) Transverse Charged Densities "Transverse" Charged PTsum Density: dptsum/dηdφ HERWIG 6.4 ε = 0 Pythia (Set A) ε = PT(charged jet#) (GeV/c) Energy Dependence ε = 0.6 CTEQ5L 630 GeV η <.0 PT> GeV Shows the transverse charged PT sum density ( η <, P T > GeV) versus P T (charged jet#) at 630 GeV predicted by HERWIG 6.4 (P T (hard) > 3 GeV/c, CTEQ5L) and a tuned version of PYTHIA (P T (hard) > 0, CTEQ5L, Set A, ε = 0, ε = 0.6 (default) and ε = 0.25 (preferred)). Also shown are the PT sum densities (0.6 GeV/c and 4 GeV/c) determined from the Tano, Kovacs, Huston, and Bhatti transverse cone analysis at 630 GeV. Charged PTsum Density (GeV) Lowering P T0 at 630 GeV (i.e. increasing ε) increases UE activity resulting in less energy dependence. "Min Transverse" PTsum Density: dptsum/dηdφ Pythia (Set A) ε = 0.25 Increasing ε produces less energy dependence for the ε = 0.6 UE resulting ε = 0 in less UE activity at the LHC! PT0 (GeV/c) PYTHIA PT(charged jet#) (GeV/c) HERWIG 6.4 Hard-Scattering Cut-Off PT0 ε = 0.25 (Set A)) CTEQ5L 630 GeV η <.0 PT> GeV ε = 0.6 (default) CM Energy W (GeV) Rick Field Fermilab MC Workshop Reference point October 4, 2002! E 0 =.8 TeV 00,000 0,000 00,000 Rick Field Florida/CDF/CMS Page 6
17 CDF Run P (Z) T UE Parameters PYTHIA 6.2 CTEQ5L Parameter Tune A Tune A25 MSTP(8) MSTP(82) 4 4 PARP(82) 2.0 GeV 2.0 GeV PARP(83) PARP(84) Tune A GeV PT Distribution /N dn/dpt σ = Z-Boson Transverse Momentum σ = 2.5 CDF Run Data PYTHIA Tune A PYTHIA Tune A25 PYTHIA Tune A50 σ = 5.0 CDF Run published.8 TeV Normalized to PARP(85) PARP(86) Z-Boson PT (GeV/c) ISR Parameter PARP(89) PARP(90) PARP(67) MSTP(9).8 TeV TeV TeV Shows the Run Z-boson p T distribution (<p T (Z)>.5 GeV/c) compared with PYTHIA Tune A (<p T (Z)> = 9.7 GeV/c), Tune A25 (<p T (Z)> = 0. GeV/c), and Tune A50 (<p T (Z)> =.2 GeV/c). PARP(9) PARP(93) Intrensic KT Vary the intrensic KT! Rick Field Florida/CDF/CMS Page 7
18 UE Parameters ISR Parameters Intrensic KT CDF Run P (Z) T PYTHIA 6.2 CTEQ5L Parameter MSTP(8) MSTP(82) PARP(82) PARP(83) PARP(84) PARP(85) PARP(86) PARP(89) PARP(90) PARP(62) PARP(64) PARP(67) MSTP(9) PARP(9) PARP(93) Tune A GeV TeV Tune AW GeV TeV Tune used by the CDF-EWK group! PT Distribution /N dn/dpt Z-Boson Transverse Momentum CDF Run Data PYTHIA Tune A PYTHIA Tune AW Z-Boson PT (GeV/c) CDF Run published.8 TeV Normalized to Shows the Run Z-boson p T distribution (<p T (Z)>.5 GeV/c) compared with PYTHIA Tune A (<p T (Z)> = 9.7 GeV/c), and PYTHIA Tune AW (<p T (Z)> =.7 GeV/c). Effective Q cut-off, below which space-like showers are not evolved. The Q 2 = k T2 in α s for space-like showers is scaled by PARP(64)! Rick Field Florida/CDF/CMS Page 8
19 Jet-Jet Correlations (DØ) Jet#-Jet#2 φ Distribution φ Jet#-Jet#2 MidPoint Cone Algorithm (R = 0.7, f merge = ) L= 50 pb - (Phys. Rev. Lett (2005)) Data/NLO agreement good. Data/HERWIG agreement good. Data/PYTHIA agreement good provided PARP(67) = (i.e. like Tune A, best fit 2.5). Rick Field Florida/CDF/CMS Page 9
20 CDF Run P (Z) T PYTHIA 6.2 CTEQ5L Z-Boson Transverse Momentum UE Parameters Parameter MSTP(8) MSTP(82) PARP(82) PARP(83) PARP(84) PARP(85) Tune DW 4.9 GeV.0 Tune AW GeV 0.9 PT Distribution /N dn/dpt CDF Run Data PYTHIA Tune DW HERWIG CDF Run published.8 TeV Normalized to ISR Parameters PARP(86) PARP(89) PARP(90) PARP(62) PARP(64) PARP(67).0.8 TeV TeV Z-Boson PT (GeV/c) Shows the Run Z-boson p T distribution (<p T (Z)>.5 GeV/c) compared with PYTHIA Tune DW, and HERWIG. MSTP(9) PARP(9) PARP(93) Intrensic KT Tune DW uses D0 s perfered value of PARP(67)! Tune DW has a lower value of PARP(67) and slightly more MPI! Rick Field Florida/CDF/CMS Page 20
21 All use LO α s with Λ = 92 MeV! Parameter Tune AW Tune DW Tune D6 PYTHIA 6.2 Tunes PDF CTEQ5L CTEQ5L CTEQ6L UE Parameters MSTP(8) MSTP(82) PARP(82) GeV 4.9 GeV 4.8 GeV Uses CTEQ6L PARP(83) PARP(84) PARP(85) Tune A energy dependence! ISR Parameter PARP(86) PARP(89) TeV.0.8 TeV.0.8 TeV PARP(90) PARP(62) PARP(64) PARP(67) MSTP(9) PARP(9) PARP(93) Intrinsic KT Rick Field Florida/CDF/CMS Page 2
22 All use LO α s with Λ = 92 MeV! Parameter PYTHIA 6.2 Tunes Tune DWT Tune D6T ATLAS PDF CTEQ5L CTEQ6L CTEQ5L MSTP(8) UE Parameters MSTP(82) PARP(82).9409 GeV.8387 GeV.8 GeV PARP(83) PARP(84) ATLAS energy dependence! PARP(85) ISR Parameter PARP(86) PARP(89).0.96 TeV.0.96 TeV TeV PARP(90) PARP(62) PARP(64) PARP(67) MSTP(9) PARP(9) PARP(93) Intrinsic KT Rick Field Florida/CDF/CMS Page 22
23 PYTHIA 6.2 Tunes All use LO α s with Λ = 92 MeV! Tune A UE Parameters ISR Parameter Tune D Intrinsic KT Parameter Tune DWT Tune D6T ATLAS PDF CTEQ5L CTEQ6L CTEQ5L MSTP(8) MSTP(82) PARP(82).9409 GeV.8387 GeV.8 GeV PARP(83) PARP(84) Tune AW Tune B Tune BW PARP(85) PARP(86).0.0 PARP(89).96 TeV.96 TeV PARP(90) PARP(62) PARP(64) PARP(67) MSTP(9) PARP(9) Tune 2. DW 2. PARP(93) TeV Tune D6 5.0 ATLAS energy dependence! Tune D6T Rick Field Florida/CDF/CMS Page 23
24 "Transverse" Charged Density Min-Bias Associated Charged Particle Density 35% more at RHIC means 26% less at the LHC! RDF Preliminary generator level Min-Bias 0.2 TeV ~.35 PY Tune DW PY Tune DWT Charged Particles ( η <.0, PT> GeV/c) PTmax (GeV/c) "Transverse" Charged Density.6.2 RDF Preliminary generator level Min-Bias 4 TeV PY Tune DWT ~.35 Charged Particles ( η <.0, PT> GeV/c) PTmax (GeV/c) PY Tune DW RHIC PTmax Direction φ Toward Transverse Transverse 0.2 TeV 4 TeV (~factor of 70 increase) LHC PTmax Direction φ Toward Transverse Transverse Away Away Shows the associated charged particle density in the transverse regions as a function of PTmax for charged particles (p T > GeV/c, η <, not including PTmax) for min-bias events at 0.2 TeV and 4 TeV from PYTHIA Tune DW and Tune DWT at the particle level (i.e. generator level). The STAR data from RHIC favors Tune DW! Rick Field Florida/CDF/CMS Page 24
25 Min-Bias Associated Charged Particle Density "Transverse" Charged Density.2 RDF Preliminary py Tune DW generator level ~.9 ~2.7 Min-Bias Charged Particles ( η <.0, PT> GeV/c) PTmax (GeV/c) 0.2 TeV 4 TeV.96 TeV RHIC PTmax Direction φ Toward Transverse Transverse 0.2 TeV.96 TeV (UE increase ~2.7 times) Tevatron PTmax Direction φ Toward Transverse Transverse.96 TeV 4 TeV (UE increase ~.9 times) LHC PTmax Direction φ Toward Transverse Transverse Away Away Away Shows the associated charged particle density in the transverse region as a function of PTmax for charged particles (p T > GeV/c, η <, not including PTmax) for min-bias events at 0.2 TeV,.96 TeV and 4 TeV predicted by PYTHIA Tune DW at the particle level (i.e. generator level). Rick Field Florida/CDF/CMS Page 25
26 The Underlying Event at STAR At STAR they have measured the underlying event at W = 200 GeV ( η <, p T > 0.2 GeV) and compared their uncorrected data with PYTHIA Tune A + STAR-SIM. Rick Field Florida/CDF/CMS Page 26
27 The Underlying Event at STAR At STAR they have measured the underlying event at W = 200 GeV ( η <, p T > 0.2 GeV) and compared their uncorrected data with PYTHIA Tune A + STAR-SIM. Rick Field Florida/CDF/CMS Page 27
28 Transverse Charged Particle Density "Transverse" Charged Density RDF LHC Prediction! RDF Preliminary generator level Min-Bias.96 TeV PY64 Tune S320 PY64 Tune P329 PY64 Tune N PTmax (GeV/c) PY Tune A Charged Particles ( η <.0, PT> GeV/c) "Transverse" Charged Density.6.2 RDF Preliminary generator level PY ATLAS PY Tune A PY64 Tune S320 PY Tune DW Min-Bias 4 TeV Charged Particles ( η <.0, PT> GeV/c) PTmax (GeV/c) PY64 Tune P329 PY Tune DWT PTmax Direction PTmax Direction φ φ Toward Toward Transverse Transverse Tevatron LHC Transverse Transverse Away Away Shows the associated charged particle density in the transverse region as a function of PTmax for charged particles (p T > GeV/c, η <, not including PTmax) for min-bias events at.96 TeV from PYTHIA Tune A, Tune S320, Tune N324, and Tune P329 at the particle level (i.e. generator level). Extrapolations of PYTHIA Tune A, Tune DW, Tune DWT, Tune S320, Tune P329, and pyatlas to the LHC. Rick Field Florida/CDF/CMS Page 28
29 Transverse Charged Particle Density "Transverse" Charged Density RDF LHC Prediction! RDF Preliminary generator level "Transverse" Charged Density PY Tune A PY64 Tune P329 PY64 Tune N324 PY Tune A PY64 Tune S320 PY64 Tune S320 PY Tune DW Min-Bias Min-Bias Charged Particles If the ( η <.0, LHC PT> GeV/c) data are 4 not TeV in.96 TeV Charged Particles ( η <.0, PT> GeV/c) the 4range 6 8 shown 20 0here then PTmax (GeV/c) PTmax (GeV/c) PTmax Direction Transverse Toward Away PY64 Tune P329 φ Transverse Tevatron.6.2 RDF Preliminary generator level we learn new (QCD) physics! Rick Field October 3, 2009 LHC PTmax Direction Transverse Toward Away PY ATLAS φ Transverse PY Tune DWT Shows the associated charged particle density in the transverse region as a function of PTmax for charged particles (p T > GeV/c, η <, not including PTmax) for min-bias events at.96 TeV from PYTHIA Tune A, Tune S320, Tune N324, and Tune P329 at the particle level (i.e. generator level). Extrapolations of PYTHIA Tune A, Tune DW, Tune DWT, Tune S320, Tune P329, and pyatlas to the LHC. Rick Field Florida/CDF/CMS Page 29
30 Transverse Charged Density PTmax Direction φ Toward Transverse Transverse Away ChgJet# Direction φ Toward Transverse Transverse Away Muon-Pair Direction φ Toward "Transverse" Charged Density.6.2 RDF Preliminary py Tune DW generator level PTmax DY(muon-pair) 70 < M(pair) < 0 GeV ChgJet# PT(chgjet#) or PTmax or PT(pair) (GeV/c) Charged Particles ( η <.0, PT> GeV/c) Transverse Transverse Away Shows the charged particle density in the transverse region for charged particles (p T > GeV/c, η < ) at as defined by PTmax, PT(chgjet#), and PT(muon-pair) from PYTHIA Tune DW at the particle level (i.e. generator level). Charged particle jets are constructed using the Anti-KT algorithm with d =. Rick Field Florida/CDF/CMS Page 30
31 Min-Bias Associated Charged Particle Density "Transverse" Charged Density.2 RDF Preliminary py Tune DW generator level Min-Bias PTmax (GeV/c) 4 TeV.96 TeV 0.9 TeV 0.2 TeV 0 TeV Charged Particles ( η <.0, PT> GeV/c) "Transverse" Charged Density.2 RDF Preliminary py Tune DW generator level Tevatron RHIC LHC Center-of-Mass Energy (TeV) LHC0 PTmax = 5.25 GeV/c LHC4 Charged Particles ( η <.0, PT> GeV/c) RHIC PTmax Direction φ Toward Transverse Transverse 0.2 TeV.96 TeV (UE increase ~2.7 times) Tevatron PTmax Direction φ Toward Transverse Transverse.96 TeV 4 TeV (UE increase ~.9 times) LHC PTmax Direction φ Toward Transverse Transverse Away Away Away Shows the associated charged particle density in the transverse region as a function of PTmax for charged particles (p T > GeV/c, η <, not including PTmax) for min-bias events at 0.2 TeV, 0.9 TeV,.96 TeV,, 0 TeV, 4 TeV predicted by PYTHIA Tune DW at the particle Linear scale! level (i.e. generator level). Rick Field Florida/CDF/CMS Page 3
32 Min-Bias Associated Charged Particle Density "Transverse" Charged Density.2 RDF Preliminary py Tune DW generator level Min-Bias Charged Particles ( η <.0, PT> GeV/c) PTmax (GeV/c) 4 TeV.96 TeV 0.9 TeV 0.2 TeV 0 TeV "Transverse" Charged Density.2 RDF Preliminary py Tune DW generator level RHIC Tevatron Charged Particles ( η <.0, PT> GeV/c) Center-of-Mass Energy (TeV) LHC4 LHC0 LHC7 PTmax = 5.25 GeV/c LHC7 PTmax Direction φ Toward Transverse Transverse Away 4 TeV (UE increase ~20%) Linear on a log plot! LHC4 PTmax Direction φ Toward Transverse Transverse Away Shows the associated charged particle density in the transverse region as a function of PTmax for charged particles (p T > GeV/c, η <, not including PTmax) for min-bias events at 0.2 TeV, 0.9 TeV,.96 TeV,, 0 TeV, 4 TeV predicted by PYTHIA Tune DW at the particle Log scale! level (i.e. generator level). Rick Field Florida/CDF/CMS Page 32
33 Conclusions November 2009 We are making good progress in understanding and modeling the underlying event. RHIC data at 200 GeV are very important! The new Pythia p T ordered tunes (py64 S320 and py64 P329) are very similar to Tune A, Tune AW, and Tune DW. At present the new tunes do not fit the data better than Tune AW and Tune DW. However, the new tune are theoretically preferred! It is clear now that the default value PARP(90) = 0.6 is not correct and the value should be closer to the Tune A value of The new and old PYTHIA tunes are beginning to converge and I believe we are finally in a position to make some legitimate predictions at the LHC! All tunes with the default value PARP(90) = 0.6 are wrong and are overestimating the activity of min-bias and the underlying event at the LHC! This includes all my T tunes and the (old) ATLAS tunes! Need to measure Min-Bias and the underlying event at the LHC as soon as possible to see if there is new QCD physics to be learned! PT0 (GeV/c) Proton Underlying Event Outgoing Parton PYTHIA Final-State Radiation UE&MB@CMS Outgoing Parton PT(hard) Hard-Scattering Cut-Off PT0 ε = 0.25 (Set A)) ε = 0.6 (default) Initial-State Radiation AntiProton Underlying Event 00,000 0,000 00,000 CM Energy W (GeV) Rick Field Florida/CDF/CMS Page 33
34 Transverse Charged Particle Density "Transverse" Charged Density RDF Preliminary Fake Data pydw generator level PTmax Prediction! ChgJet# PTmax or PT(chgjet#) (GeV/c) Charged Particles ( η <2.0, PT> GeV/c) Fake data (from MC) at on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) and the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2. The fake data (from PYTHIA Tune DW) are generated at the particle level (i.e. generator level) assuming M min-bias events at (36,595 events in the plot). PT(chgjet#) Direction Transverse Toward Away φ Transverse PTmax Direction Transverse Toward Away φ Transverse Rick Field MB&UE@CMS Workshop CERN, November 6, 2009 Leading Charged Particle Jet, chgjet#. Leading Charged Particle, PTmax. Rick Field Florida/CDF/CMS Page 34
35 Transverse Charge Density "Transverse" Charged Density.2 RDF Preliminary py Tune DW generator level Prediction! factor of 2! PTmax (GeV/c) Charged Particles ( η <2.0, PT> GeV/c) Rick Field MB&UE@CMS Workshop CERN, November 6, 2009 LHC PTmax Direction φ Toward Transverse Transverse Away (UE increase ~ factor of 2) ~ ~ LHC PTmax Direction φ Toward Transverse Transverse Away Shows the charged particle density in the transverse region for charged particles (p T > GeV/c, η < 2) at and as defined by PTmax from PYTHIA Tune DW and at the particle level (i.e. generator level). Rick Field Florida/CDF/CMS Page 35
36 Transverse Charged Particle Density "Transverse" Charged Density RDF Preliminary Fake Data pydw generator level PTmax Monte-Carlo! ChgJet# Charged Particles ( η <2.0, PT> GeV/c) "Transverse" Charged Density CMS Preliminary data uncorrected pydw + SIM PTmax Real Data! ChgJet# Charged Particles ( η <2.0, PT> GeV/c) PTmax or PT(chgjet#) (GeV/c) PTmax or PT(chgjet#) (GeV/c) Fake data (from MC) at on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) and the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2. The fake data (from PYTHIA Tune DW) are generated at the particle level (i.e. generator level) assuming M min-bias events at (36,595 events in the plot). CMS preliminary data at on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) and the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2. The data are uncorrected and compared with PYTHIA Tune DW after detector simulation (26,25 events in the plot). Rick Field Florida/CDF/CMS Page 36
37 Transverse Charged PTsum Density PTsum Density (GeV/c) "Transverse" Charged PTsum Density: dpt/dηdφ RDF Preliminary Fake Data pydw generator level PTmax Monte-Carlo! ChgJet# PTmax or PT(chgjet#) (GeV/c) Charged Particles ( η <2.0, PT> GeV/c) PTsum Density (GeV/c) "Transverse" Charged PTsum Density: dpt/dηdφ CMS Preliminary data uncorrected pydw + SIM PTmax Real Data! ChgJet# PTmax or PT(chgjet#) (GeV/c) Charged Particles ( η <2.0, PT> GeV/c) Fake data (from MC) at on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle (PTmax) and the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2. The fake data (from PYTHIA Tune DW) are generated at the particle level (i.e. generator level) assuming M min-bias events at (36,595 events in the plot). CMS preliminary data at on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle (PTmax) and the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2. The data are uncorrected and compared with PYTHIA Tune DW after detector simulation (26,25 events in the plot). Rick Field Florida/CDF/CMS Page 37
38 PYTHIA Tune DW Charged Particle Density.2 CMS Preliminary data uncorrected pydw + SIM PT(chgjet#) GeV/c CMS preliminary data at and on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2. The data are uncorrected and compared with PYTHIA Tune DW after detector simulation. PT(chgjet#) Direction Charged Particles ( η <2.0, PT> GeV/c) φ CMS "Transverse" Charged Density.2 RDF Preliminary ATLAS corrected data Tune DW generator level PTmax (GeV/c) PTmax Direction φ ATLAS Charged Particles ( η <2.5, PT> GeV/c) ATLAS preliminary data at and on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η < 2.5. The data are corrected and compared with PYTHIA Tune DW at the generator level. Toward Toward Transverse Transverse Transverse Transverse Away Away Rick Field Florida/CDF/CMS Page 38
39 PYTHIA Tune DW Charged Particle Density.2 CMS Preliminary data uncorrected pydw + SIM Ratio PT(chgjet#) GeV/c Ratio: / CMS Preliminary data uncorrected pydw + SIM simulation. / Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) (GeV/c) PT(chgjet#) Direction φ CMS CMS preliminary data at and Ratio of CMS preliminary data at on the transverse charged particle density, and on the transverse charged dn/dηdφ, as defined by the leading charged particle density, dn/dηdφ, as defined by the particle jet (chgjet#) for charged particles with leading charged particle jet (chgjet#) for p T > GeV/c and η < 2. The data are charged particles with p T > GeV/c and η uncorrected and compared with PYTHIA Tune < 2. The data are uncorrected and compared DW after detector simulation. with PYTHIA Tune DW after detector PT(chgjet#) Direction Charged Particles ( η <2.0, PT> GeV/c) φ CMS Toward Toward Transverse Transverse Transverse Transverse Away Away Rick Field Florida/CDF/CMS Page 39
40 PYTHIA Tune DW Ratio: / CMS Preliminary data uncorrected pydw + SIM / Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) (GeV/c) CMS Ratio: / RDF Preliminary ATLAS corrected data pydw generator level / Charged Particles ( η <2.5, PT> GeV/c) PTmax (GeV/c) ATLAS Ratio of CMS preliminary data at and on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2. The data are uncorrected and compared with PYTHIA Tune DW after detector PT(chgjet#) Direction simulation. Toward φ Ratio of the ATLAS preliminary data at and on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η < 2.5. The data are corrected and compared with PYTHIA Tune DW at PTmax Direction the generator level. Toward φ Transverse Transverse Transverse Transverse Away Away Rick Field Florida/CDF/CMS Page 40
41 PYTHIA Tune DW How well did we do at predicting the underlying event at and? "Transverse" Charged Density CMS Preliminary data uncorrected pydw + SIM PTmax Tune DW ChgJet# Charged Particles ( η <2.0, PT> GeV/c) PTmax or PT(chgjet#) (GeV/c) Charged Particle Density.2 CMS Preliminary data uncorrected pydw + SIM Tune DW Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c I am surprised that the Tunes did not do a better job of predicting the behavior of the underlying event at and! Ratio: / CMS Preliminary data uncorrected pydw + SIM / Tune DW Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) (GeV/c) Rick Field Florida/CDF/CMS Page 4
42 PYTHIA Tune DW How well did we do at predicting the underlying event at and? "Transverse" Charged Density CMS Preliminary data uncorrected pydw + SIM PTmax Tune DW ChgJet# Charged Particles ( η <2.0, PT> GeV/c) PTmax or PT(chgjet#) (GeV/c) Charged Particle Density.2 CMS Preliminary data uncorrected pydw + SIM Tune DW Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c I am surprised that the Tunes did as well as they did at predicting the behavior of the underlying event at and! Ratio: / CMS Preliminary data uncorrected pydw + SIM / Tune DW Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) (GeV/c) Rick Field Florida/CDF/CMS Page 42
43 PYTHIA Tune DW How well did we do at predicting the underlying event at and? "Transverse" Charged Density 0.6 CMS Preliminary data uncorrected pydw + SIM PTmax ChgJet# 0.2 Tune DW at charged particles with p Charged Particles ( η <2.0, PT> GeV/c) T > GeV/c. Tune DW Charged Particles ( η <2.0, PT> GeV/c) We do not know if the models correctly PTmax or PT(chgjet#) (GeV/c) describe the UE at lower p T values! PT(chgjet#) GeV/c Charged Particle Density.2 CMS Preliminary data uncorrected pydw + SIM Warning! All the UE studies look I am surprised that the Tunes did as well as they did at predicting the behavior of the underlying event at and! Ratio: / CMS Preliminary data uncorrected pydw + SIM / Tune DW Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) (GeV/c) Rick Field Florida/CDF/CMS Page 43
44 ATLAS Tune AMBT Judith Katzy LPCC MB&UE working group meeting, May 3, 200. Emily Nurse ICHEP, July 24, 200. ATLAS-CONF Rick Field Florida/CDF/CMS Page 44
45 ATLAS Tune AMBT Subset of the min-bias data! Attempt to fit a subset of the min-bias data (Nchg 6) where the contamination due to diffraction is expected to be small! Rick Field Florida/CDF/CMS Page 45
46 PYTHIA Tune Z All my previous tunes (A, DW, DWT, D6, D6T, CW, X, and X2) were PYTHIA 6.4 tunes using the old Q 2 -ordered parton showers and the old MPI model (really 6.2 tunes)! I believe that it is time to move to PYTHIA 6.4 (p T -ordered parton showers and new MPI model)! Tune Z: I started with the parameters of ATLAS Tune AMBT, but I changed LO* to CTEQ5L and I varied PARP(82) and PARP(90) to get a very good fit of the CMS UE data at 900 GeV and. The ATLAS Tune AMBT was designed to fit the inelastic data for Nchg 6 and to fit the PTmax UE data with PTmax > 0 GeV/c. Tune AMBT is primarily a min-bias tune, while Tune Z is a UE tune! Proton PARP(90) Color Connections Underlying Event Outgoing Parton Final-State Radiation PARP(82) Diffraction Outgoing Parton PT(hard) UE&MB@CMS Initial-State Radiation Proton Underlying Event Rick Field Florida/CDF/CMS Page 46
47 PYTHIA Tune Z Parameter Tune Z (R. Field CMS) Tune AMBT (ATLAS) Parton Distribution Function CTEQ5L LO* Parameters not shown are the PYTHIA 6.4 defaults! PARP(82) MPI Cut-off PARP(89) Reference energy, E PARP(90) MPI Energy Extrapolation PARP(77) CR Suppression PARP(78) CR Strength PARP(80) Probability colored parton from BBR PARP(83) Matter fraction in core PARP(84) Core of matter overlap PARP(62) ISR Cut-off PARP(93) primordial kt-max MSTP(8) MPI, ISR, FSR, BBR model 2 2 MSTP(82) Double gaussion matter distribution 4 4 MSTP(9) Gaussian primordial kt MSTP(95) strategy for color reconnection 6 6 Rick Field Florida/CDF/CMS Page 47
48 CMS UE Data Charged Particle Density.2 CMS Preliminary data uncorrected Theory + SIM D6T PT(chgjet#) GeV/c CMS preliminary data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are uncorrected and compared with PYTHIA Tune DW and D6T after detector simulation (SIM). Color reconnection suppression. Color reconnection strength. DW CMS Tune Z (CTEQ5L) PARP(82) =.932 PARP(90) = PARP(77) =.06 PARP(78) = 38 Charged Particle Density.2 CMS Preliminary data uncorrected pyz + SIM Tune Z Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c CMS CMS preliminary data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are uncorrected and compared with PYTHIA Tune Z after detector simulation (SIM). Tune Z is a PYTHIA 6.4 using p T -ordered parton showers and the new MPI model! Rick Field Florida/CDF/CMS Page 48
49 PYTHIA 6.2 Tunes Parameter Tune AW Tune DW Tune D6 PDF CTEQ5L CTEQ5L CTEQ6L UE Parameters MSTP(8) MSTP(82) PARP(82) GeV 4.9 GeV 4.8 GeV Uses CTEQ6L PARP(83) PARP(84) PARP(85) ISR Parameter PARP(86) PARP(89) PARP(90) PARP(62) TeV TeV TeV Reduce PARP(82) by factor of.8/.9 = 0.95 Everything else the same! PARP(64) PARP(67) MSTP(9) PARP(9) Tune A energy dependence! (not the default) PARP(93) Intrinsic KT CMS: We wanted a CTEQ6L version of Tune Z in a hurry! Rick Field Florida/CDF/CMS Page 49
50 PYTHIA Tune Z2 My guess! Parameter Tune Z (R. Field CMS) Tune Z2 (R. Field CMS) Parton Distribution Function CTEQ5L CTEQ6L PARP(82) MPI Cut-off PARP(89) Reference energy, E PARP(90) MPI Energy Extrapolation PARP(77) CR Suppression PARP(78) CR Strength PARP(80) Probability colored parton from BBR Reduce PARP(82) by factor of.83/.93 = 0.95 Everything else the same! PARP(83) Matter fraction in core PARP(84) Core of matter overlap PARP(62) ISR Cut-off PARP(93) primordial kt-max MSTP(8) MPI, ISR, FSR, BBR model 2 2 MSTP(82) Double gaussion matter distribution 4 4 MSTP(9) Gaussian primordial kt MSTP(95) strategy for color reconnection 6 6 Rick Field Florida/CDF/CMS Page 50
51 PYTHIA Tune Z2 My guess! Parameter Tune Z (R. Field CMS) Tune Z2 (R. Field CMS) Parton Distribution Function CTEQ5L CTEQ6L PARP(82) MPI Cut-off PARP(89) Reference energy, E PARP(90) MPI Energy Extrapolation PARP(77) CR Suppression PARP(78) CR Strength PARP(80) Probability colored parton from BBR Reduce PARP(82) by factor of.83/.93 = 0.95 Everything else the same! PARP(83) Matter fraction in core PARP(84) Core of matter overlap PARP(62) ISR Cut-off PARP(93) primordial kt-max PARP(90) same For Z and Z2! MSTP(8) MPI, ISR, FSR, BBR model 2 2 MSTP(82) Double gaussion matter distribution 4 4 MSTP(9) Gaussian primordial kt MSTP(95) strategy for color reconnection 6 6 Rick Field Florida/CDF/CMS Page 5
52 PYTHIA 8 Tunes R. Corke and T. Sjöstrand CTEQ6L MRST LO** CTEQ6L PT0 = PARP(82) ε = PARP(90) Tevatron LHC p T0 (W)=p T0 (W/W 0 ) ε ε = PARP(90) p T0 = PARP(82) W = E cm Rick Field Florida/CDF/CMS Page 52
53 PYTHIA Tune Z2 Parameter Parton Distribution Function PARP(82) MPI Cut-off PARP(89) Reference energy, E0 PARP(90) MPI Energy Extrapolation PARP(77) CR Suppression PARP(78) CR Strength PARP(80) Probability colored parton from BBR PARP(83) Matter fraction in core PARP(84) Core of matter overlap PARP(62) ISR Cut-off PARP(93) primordial kt-max MSTP(8) MPI, ISR, FSR, BBR model MSTP(82) Double gaussion matter distribution MSTP(9) Gaussian primordial kt MSTP(95) strategy for color reconnection Tune Z2 (R. Field CMS) CTEQ6L PY8 Tune C4 (Corke-Sjöstrand) CTEQ6L PARP(90) much different! Rick Field Florida/CDF/CMS Page 53
54 CMS UE Data Charged Particle Density.6.2 CMS Preliminary data corrected Tune Z generator level PT(chgjet#) GeV/c CMS Tune Z Charged Particles ( η <2.0, PT> GeV/c) CMS preliminary data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are corrected and compared with PYTHIA Tune Z at the generator level. PTsum Density (GeV/c) "Transverse" Charged PTsum Density: dpt/dηdφ CMS Preliminary data corrected Tune Z generator level CMS Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c Tune Z CMS preliminary data at and 7 TeV on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are corrected and compared with PYTHIA Tune Z at the generator level. CMS corrected data! Very nice agreement! CMS corrected data! Rick Field Florida/CDF/CMS Page 54
55 PYTHIA 6.4 Tune Z2 Charged Particle Density.6.2 CMS Preliminary data corrected Tune Z2 generator level Tune Z2 Charged Particles ( η <2.0, PT> GeV/c) PTsum Density (GeV/c) "Transverse" Charged PTsum Density: dpt/dηdφ CMS Preliminary data corrected Tune Z2 generator level Tune Z2 Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c PT(chgjet#) GeV/c CMS preliminary data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are corrected and compared with PYTHIA Tune Z2 at the generator level. CMS preliminary data at and 7 TeV on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are corrected and compared with PYTHIA Tune Z2 at the generator level. CMS corrected data! Not good! Bad energy dependence! CMS corrected data! Rick Field Florida/CDF/CMS Page 55
56 PYTHIA 8 Tune C4 Charged Particle Density.6.2 CMS Preliminary data corrected PY8 Tune C4 generator level PY8 Tune C4 Charged Particles ( η <2.0, PT> GeV/c) PTsum Density (GeV/c) "Transverse" Charged PTsum Density: dpt/dηdφ CMS Preliminary data corrected PY8 Tune C4 generator level PY8 Tune C4 Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c PT(chgjet#) GeV/c CMS preliminary data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are corrected and compared with PYTHIA 8 Tune C4 at the generator level. CMS preliminary data at and 7 TeV on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0. The data are corrected and compared with PYTHIA 8 Tune C4 at the generator level. CMS corrected data! Not good! PTsum too small! CMS corrected data! Rick Field Florida/CDF/CMS Page 56
57 Transverse Ratio: PTsum/Nchg PTsum/Nchg (GeV/c) "Transverse" Charged Particle Ratio: PTsum/Nchg CMS Preliminary data corrected Tune Z generator level Tune Z PTsum/Nchg (GeV/c) "Transverse" Charged Particle Ratio: PTsum/Nchg CMS Preliminary data corrected Tune Z2 generator level Tune Z2 Charged Particles ( η <2.0, PT> GeV/c) Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c PT(chgjet#) GeV/c CMS preliminary data at and 7 TeV on the transverse ratio PTsum/Nchg as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0 compared with PYTHIA Tune Z, Z2, and PY8C4 at the generator level. Z good! PY8C4 and Z2 Bad! PTsum/Nchg (GeV/c) "Transverse" Charged Particle Ratio: PTsum/Nchg CMS Preliminary data corrected PY8 Tune C4 generator level PY8 Tune C4 Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c Rick Field Florida/CDF/CMS Page 57
58 Energy Dependence Charged Density Ratio "Transverse" Charged Particle Density: Ratio CMS Preliminary data corrected generator level theory Z2 Z PY8C4 Charged Density Ratio "Transverse" Charged PTsum Density: Ratio CMS Preliminary data corrected generator level theory Z2 Z PY8C4 divided by Charged Particles ( η <2.0, PT> GeV/c) divided by Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c PT(chgjet#) GeV/c CMS data on the energy dependence ( divided by ) of the transverse charged particle density as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0 compared with PYTHIA Tune Z, Z2, and PY8C4 at the generator level. CMS data on the energy dependence ( divided by ) of the transverse charged PTsum density as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0 compared with PYTHIA Tune Z, Z2, and PY8C4 at the generator level. CMS corrected data! Z and PY8C4 good! Z2 Bad! CMS corrected data! Rick Field Florida/CDF/CMS Page 58
59 Charged Density Ratio Energy Dependence "Transverse" Charged Particle Density: Ratio CMS Preliminary data corrected generator level theory Z2 divided by CTEQ6L: PARP(90) =0.275 Charged Particles ( η <2.0, PT> GeV/c) PT(chgjet#) GeV/c CMS data on the energy dependence ( divided by ) of the transverse charged particle density as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0 compared with PYTHIA Tune Z, Z2, and PY8C4 at the generator level. Z PY8C4 CTEQ6L: PARP(90) = 0.9 "Transverse" Charged PTsum Density: Ratio Charged Density Ratio CMS Preliminary data corrected generator level theory divided by Charged Particles ( η <2.0, PT> GeV/c) CTEQ5L: PARP(90) =0.275 Z2 PT(chgjet#) GeV/c CMS data on the energy dependence ( divided by ) of the transverse charged PTsum density as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0 compared with PYTHIA Tune Z, Z2, and PY8C4 at the generator level. Z PY8C4 CMS corrected data! Duh! The energy dependence depends on Z and PY8C4 good! Z2 Bad! both PARP(90) and the structure function! CMS corrected data! Rick Field Florida/CDF/CMS Page 59
60 ATLAS UE Data "Transverse" Charged Density.2 RDF Preliminary ATLAS corrected data Tune Z generator level ATLAS Tune Z Charged Particles ( η <2.5, PT> GeV/c) PTsum Density (GeV/c).5.0 "Transverse" Charged PTsum Density: dpt/dηdφ RDF Preliminary ATLAS corrected data Tune Z generator level ATLAS Tune Z Charged Particles ( η <2.5, PT> GeV/c) PTmax (GeV/c) PTmax (GeV/c) ATLAS published data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η < 2.5. The data are corrected and compared with PYTHIA Tune Z at the generator level. ATLAS published data at and 7 TeV on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η < 2.5. The data are corrected and compared with PYTHIA Tune Z at the generrator level. ATLAS publication arxiv: December 3, 200 Rick Field Florida/CDF/CMS Page 60
61 CMS-ATLAS UE Data Charged Particle Density.6.2 RDF Preliminary data corrected Tune Z generator level ATLAS: PTmax CMS: Chgjet# Charged Particles (PT > GeV/c) PTmax or PT(chgjet#) (GeV/c) CMS (red) ATLAS (blue) Tune Z CMS preliminary data at on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle jet (chgjet#) for charged particles with p T > GeV/c and η < 2.0 together with the ATLAS published data at on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η < 2.5 The data are corrected and compared with PYTHIA Tune Z at the generator level. Charged Particle Density.6.2 RDF Preliminary data corrected Tune Z generator level Charged Particles (PT > GeV/c) PTmax or PT(chgjet#) (GeV/c) CMS (red) ATLAS (blue) Tune Z Amazing agreement! Rick Field Florida/CDF/CMS Page 6
62 ATLAS UE Data "Transverse" Charged Density RDF Preliminary ATLAS corrected data Tune Z generator level Tune Z PT > GeV/c PTmax (GeV/c) PT > 0. GeV/c ATLAS Charged Particles ( η <2.5) PTsum Density (GeV/c) "Transverse" Charged PTsum Density: dpt/dηdφ RDF Preliminary ATLAS corrected data Tune Z generator level Tune Z PT > GeV/c PTmax (GeV/c) PT > 0. GeV/c ATLAS Charged Particles ( η <2.5) ATLAS published data at on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and p T > 0. GeV/c ( η < 2.5). The data are corrected and compared with PYTHIA Tune Z at the generator level. ATLAS published data at on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and p T > 0. GeV/c ( η < 2.5). The data are corrected and compared with PYTHIA Tune Z at the generator level. ATLAS publication arxiv: December 3, 200 Rick Field Florida/CDF/CMS Page 62
63 ATLAS UE Data "Transverse" Charged Density RDF Preliminary ATLAS corrected data Tune Z generator level Tune Z "Transverse" Ratio 0./ PT > GeV/c.0 PT > 0. GeV/c Charged Particles ( η <2.5) Charge PTsum Density PTmax (GeV/c) ATLAS published data at on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and p T > 0. GeV/c ( η < 2.5). The data are corrected and compared with PYTHIA Tune Z at the generator level. "Transverse" Ratio: PT > 0. and > GeV/c ATLAS PTsum Density (GeV/c).0 "Transverse" Charged PTsum Density: dpt/dηdφ 2.5 RDF Preliminary ATLAS corrected data 2.0 Tune Z generator level RDF Preliminary ATLAS corrected data Charge Particle Density Tune Z.5 Tune Z generator level PT > GeV/c PTmax (GeV/c) Charged Particles ( η <2.5) PT > 0. GeV/c Charged Particles ( η <2.5) ATLAS published data at on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and p T > 0. GeV/c ( η < 2.5). The data are corrected and compared with PYTHIA Tune Z at the generator level PTmax (GeV/c) ATLAS publication arxiv: December 3, 200 ATLAS Rick Field Florida/CDF/CMS Page 63
64 ATLAS UE Data "Transverse" Charged Density.2 RDF Preliminary ATLAS corrected data Tune Z generator level Tune Z PTmax (GeV/c) ATLAS Charged Particles ( η <, PT> GeV/c) ATLAS preliminary data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η <. The data are corrected and compared with PYTHIA Tune Z at the generator level. PTsum Density (GeV/c).5.0 "Transverse" Charged PTsum Density: dpt/dηdφ RDF Preliminary ATLAS corrected data Tune Z generator level Tune Z Charged Particles ( η <, PT > GeV/c) PTmax (GeV/c) ATLAS ATLAS preliminary data at and 7 TeV on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η <. The data are corrected and compared with PYTHIA Tune Z at the generrator level. ATLAS-CONF February 2, 20 Rick Field Florida/CDF/CMS Page 64
65 ATLAS UE Data "Transverse" Charged Density.2 RDF Preliminary ATLAS corrected data Tune Z generator level Tune Z PTmax (GeV/c) ATLAS Charged Particles ( η <, PT> GeV/c) ATLAS preliminary data at and 7 TeV on the transverse charged particle density, dn/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η <. The data are corrected and compared with PYTHIA Tune Z at the generator level. PTsum Density (GeV/c).5.0 "Transverse" Charged PTsum Density: dpt/dηdφ RDF Preliminary ATLAS corrected data Tune Z generator level Tune Z Charged Particles ( η <, PT > GeV/c) PTmax (GeV/c) ATLAS ATLAS preliminary data at and 7 TeV on the transverse charged PTsum density, dpt/dηdφ, as defined by the leading charged particle (PTmax) for charged particles with p T > GeV/c and η <. The data are corrected and compared with PYTHIA Tune Z at the generrator level. ATLAS-CONF February 2, 20 Rick Field Florida/CDF/CMS Page 65
Tevatron Energy Scan. Energy Dependence of the Underlying Event. Rick Field Craig Group & David Wilson University of Florida
Rick Field Craig Group & David Wilson University of Florida Tevatron Energy Scan Energy Dependence of the Underlying Event Outline of Talk Wine & Cheese talk, October 4, 2002. Studying the underlying event
More informationHEP Seminar. Studying the Energy Dependence of the Underlying Event at the Tevatron and the LHC Rick Field University of Florida.
Studying the Energy Dependence of the Underlying Event at the Tevatron and the LHC Rick Field University of Florida HEP Seminar Outline Early studies the underlying event (UE) at CDF and PYTHIA Tune A.
More informationToward an Understanding of Hadron-Hadron. Collisions From Feynman-Field to the LHC
Toward an Understanding of Hadron-Hadron Collisions From Feynman-Field to the LHC Rick Field University of Florida Outline of Talk The old days of Feynman-Field Phenomenology. XXIèmes Rencontres de Blois
More informationThe LHC Physics Environment
The LHC Physics Environment Talk : What We Have Learned at the Tevatron Rick Field University of Florida Outline of Talk The old days of Feynman-Field Phenomenology. Review what we learned about minbias,
More informationMinimum Bias at CDF and CMS
Minimum Bias at CDF and CMS Minumum Bias Collisions Proton AntiProton CDF Run 2 CMS Outline of Talk Review the CDF Run 2 minimum bias tune (i.e. PYTHIA Tune A). UE&MB@CMS Show the minimum bias predictions
More informationUniversity of Glasgow Tevatron Energy Scan: Findings & Surprises
Outline of Talk University of Glasgow Tevatron Energy Scan: Findings & Surprises Rick Field University of Florida Simulating hadron-hadron collisions: The early days of Feynman-Field Phenomenology. The
More informationCollisions Rick s View of Hadron Collisions
st Workshop on Energy Scaling in Hadron-Hadron Collisions Rick s View of Hadron Collisions Rick Field University of Florida Fermilab 2009 Outline of Talk The early days of Feynman-Field Phenomenology.
More informationPYTHIA 6.2 Tunes for Run II
PYTHIA 6.2 Tunes for Run II Outline of Talk Min-Bias Collisions! Min-Bias Generators Hadron Hadron! The in Hard Scattering Processes Proton Outgoing Parton PT(hard) Initial-State Radiation AntiProton Outgoing
More informationUsing Drell-Yan to Probe the
Using Drell-Yan to Probe the Underlying Event in Run 2 at CDF Deepak Kar University of Florida (On behalf of the CDF Collaboration) Experimental Particle Physics Seminar 30 th October 2008 Prologue: We
More informationToward an Understanding of Hadron-Hadron. Collisions From Feynman-Field to the LHC
Rick Field University of Florida Outline of Talk Ricky & Sally. Toward an Understanding of Hadron-Hadron Collisions From Feynman-Field to the LHC The Berkeley Years Rick & Jimmie. The early days of Feynman-Field
More informationLHCP QCD at the Tevatron. Rick Field University of Florida (for the CDF & D0 Collaborations) Outline of Talk. with help from Christina Mesropian
with help from Christina Mesropian QCD at the Tevatron Rick Field University of Florida (for the CDF & D0 Collaborations) Outline of Talk D0 Photon + Jet Measurements. CDF W/Z + Upsilon Search. CDF Measurements
More informationMin-Bias Data: Jet Evolution and Event Shapes
Min-Bias Data: Jet Evolution and Event Shapes Rick Field and David Stuart July 1, 1999 Abstract The Min-Bias data are used to study the transition between soft and hard collisions. We study this transition
More informationThe Underlying Event in Run II ChgJets versus JetClu Jets
The Underlying Event in Run II ChgJets versus JetClu Jets Outline of Talk! The evolution of charged particle jets and the underlying event. Study the event topology relative to the leading chgjet and compare
More informationMini-Bias and Underlying Event Studies at CMS
Yuan Chao Department of Physics National Taiwan University 1617 Taipei, TAIWAN 1 Introduction The Tevatron experiments provide us very good information for the quantum chromodynamics (QCD) modelings of
More informationQCD and jets physics at the LHC with CMS during the first year of data taking. Pavel Demin UCL/FYNU Louvain-la-Neuve
QCD and jets physics at the LHC with CMS during the first year of data taking Pavel Demin UCL/FYNU Louvain-la-Neuve February 8, 2006 Bon appétit! February 8, 2006 Pavel Demin UCL/FYNU 1 Why this seminar?
More informationMinimum-Bias and Underlying-Event Physics
2008 CTEQ MCnet Summer School on QCD Phenomenology and Monte Carlo Event Generators 8 16 August 2008 Debrecen, Hungary Minimum-Bias and Underlying-Event Physics Torbjörn Sjöstrand Department of Theoretical
More informationQCD at CDF. Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration
QCD at CDF Régis Lefèvre IFAE Barcelona On behalf of the CDF Collaboration Jet Inclusive Cross-Section Underlying event studies Jet Shapes Specific processes _ W+Jets, γ + γ, γ + b/c, b-jet / bb jet Diffraction
More informationCharged particle multiplicity in proton-proton collisions with ALICE
Charged particle multiplicity in proton-proton collisions with ALICE Introduction on the motivations for a pp physics programme with ALICE A short review on the detectors used to reconstruct charged particle
More informationMinimum Bias and Underlying Event Studies at CDF
FERMILAB-CONF--531-E Minimum Bias and Underlying Event Studies at CDF INFN, Bologna E-mail: moggi@bo.infn.it Soft, non-perturbative, interactions are poorly understood from the theoretical point of view
More informationPhysics at Hadron Colliders Part II
Physics at Hadron Colliders Part II Marina Cobal Università di Udine 1 The structure of an event One incoming parton from each of the protons enters the hard process, where then a number of outgoing particles
More informationQCD Studies at LHC with the Atlas detector
QCD Studies at LHC with the Atlas detector Introduction Sebastian Eckweiler - University of Mainz (on behalf of the ATLAS Collaboration) Examples of QCD studies Minimum bias & underlying event Jet-physics
More informationUnderlying Event Measurements at the LHC
14th EDS Blois Workshop Underlying Event Measurements at the LHC Michael Heinrich for the ATLAS and CMS collaborations INSTITUTE OF EXPERIMENTAL PARTICLE PHYSICS (EKP) PHYSICS FACULTY KIT University of
More informationLHC MPI and underlying event results
LHC MPI and underlying event results Marianna Testa (ATLAS) for the ALICE, ATLAS, CMS & LHCb collaborations SM@LHC 2012, Copenhagen, 10-13 April 2012 The Underlying Event Everything in hadron collisions
More informationTesting QCD at the LHC and the Implications of HERA DIS 2004
Testing QCD at the LHC and the Implications of HERA DIS 2004 Jon Butterworth Impact of the LHC on QCD Impact of QCD (and HERA data) at the LHC Impact of the LHC on QCD The LHC will have something to say
More informationDouble Parton Scattering in CMS. Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x th June 2017 Bari, Italy
Double Parton Scattering in CMS Deniz SUNAR CERCI Adiyaman University On behalf of the CMS Collaboration Low-x 2017 17th June 2017 Bari, Italy Outline Introduction to DPS DPS measurements with CMS 2b +
More informationRecent QCD results from ATLAS
Recent QCD results from ATLAS PASCOS 2013 Vojtech Pleskot Charles University in Prague 21.11.2013 Introduction / Outline Soft QCD: Underlying event in jet events @7TeV (2010 data) Hard double parton interactions
More informationAtlas results on diffraction
Atlas results on diffraction Alessia Bruni INFN Bologna, Italy for the ATLAS collaboration Rencontres du Viet Nam 14th Workshop on Elastic and Diffractive Scattering Qui Nhon, 16/12/2011 EDS 2011 Alessia
More informationQCD at hadron colliders
QCD at hadron colliders Soushi Tsuno Okayama University Outline Introduction: Focus on current (Tevatron) and future (LHC) hadron colliders High pt pqcd phenomena & issues: PDF measurement Jet Physics
More informationJet Energy Calibration. Beate Heinemann University of Liverpool
Jet Energy Calibration Beate Heinemann University of Liverpool Fermilab, August 14th 2006 1 Outline Introduction CDF and D0 calorimeters Response corrections Multiple interactions η-dependent corrections
More informationCharged Particle Multiplicity in pp Collisions at s = 13 TeV
Charged Particle Multiplicity in pp Collisions at s = 13 TeV Khadeejah ALGhadeer PhD in Engineering, Physics The Workshop of the APS Topical Group on Hadronic Physics Charged Particle Multiplicity IN PP
More informationMPI in PYTHIA. 1. Brief overview 2. Color reconnection and the top mass
MPI in PYTHIA 1. Brief overview 2. Color reconnection and the top mass Torbjörn Sjöstrand Department of Astronomy and Theoretical Physics Lund University Sölvegatan 14A, SE-223 62 Lund, Sweden MPI@LHC
More informationPDFs for Event Generators: Why? Stephen Mrenna CD/CMS Fermilab
PDFs for Event Generators: Why? Stephen Mrenna CD/CMS Fermilab 1 Understanding Cross Sections @ LHC: many pieces to the puzzle LO, NLO and NNLO calculations K-factors Benchmark cross sections and pdf correlations
More informationPrecision QCD at the Tevatron. Markus Wobisch, Fermilab for the CDF and DØ Collaborations
Precision QCD at the Tevatron Markus Wobisch, Fermilab for the CDF and DØ Collaborations Fermilab Tevatron - Run II Chicago Ecm: 1.8 1.96 TeV more Bunches 6 36 Bunch Crossing 3500 396ns CDF Booster Tevatron
More informationParticle spectra in Minimum Bias events at 13TeV
Particle spectra in Minimum Bias events at TeV Juan Manuel Grados Luyando on behalf of the CMS collaboration Deutsches Elektronen-Synchrotron, Hamburg MPI@LHC 05 Trieste, Italy Motivation Probe the different
More informationQCD dijet analyses at DØ
QCD dijet analyses at DØ Pavel Demine for the DØ collaboration DAPNIA-SPP, CEA Saclay, France Contents: DØ detector Jet reconstruction at DØ Dijet mass spectrum Dijet azimuthal angle decorrelation XII
More informationRecent results on soft QCD topics from ATLAS
Recent results on soft QCD topics from ATLAS Roman Lysák Institute of Physics, Prague on behalf of the ATLAS collaboration Bormio 2016 Overview Understanding of soft-qcd interactions has direct impact
More informationMPI in PYTHIA 8. Richard Corke. Department of Astronomy and Theoretical Physics Lund University. September 2010
MPI in PYTHIA 8 Richard Corke Department of Astronomy and Theoretical Physics Lund University September Richard Corke (Lund University) MPI@DESY September / 5 Overview MPI in PYTHIA 8 Enhanced screening
More informationHadron Collider Physics, HCP2004, June 14-18
) " % "" ' & % % " ) " % '% &* ' ) * ' + " ' ) ( $#! ' "") ( * " ) +% % )( (. ' + -, '+ % &* ' ) ( 021 % # / ( * *' 5 4* 3 %( '' ' " + +% Hadron Collider Physics, HCP2004, June 14-18 The Run II DØ Detector
More informationNikos Varelas. University of Illinois at Chicago. CTEQ Collaboration Meeting Northwestern November 20, Nikos Varelas. CTEQ Meeting Nov 20, 2009
QCD Physics at CMS University of Illinois at Chicago CTEQ Collaboration Meeting Northwestern November 0, 009 1 QCD Physics at CMS University of Illinois at Chicago CTEQ Collaboration Meeting Northwestern
More informationLessons from the early LHC data for MC tuning
Lessons from the early LHC data for MC tuning P. S k a n d s ( C E R N ) Multiple Partonic Interactions at LHC, November 211, Hamburg A Factorized View 1. Where is the energy going? Note: only linearized
More informationReview of LHCb results on MPI, soft QCD and diffraction
Review of LHCb results on MPI, soft QCD and diffraction Marcin Kucharczyk on behalf of LHCb collaboration HNI Krakow EDS Blois 2015, Borgo (Corse), 30.06.2015 Outline LHCb - general purpose forward experiment
More informationResponse to the Referee for Physical Review DG8044
Response to the Referee for Physical Review We would like to thank the referee for the effort he has put into his report. We agree with many of the referee s comments and we now realize that there are
More informationQCD Jets at the LHC. Leonard Apanasevich University of Illinois at Chicago. on behalf of the ATLAS and CMS collaborations
QCD Jets at the LHC Leonard Apanasevich University of Illinois at Chicago on behalf of the ATLAS and CMS collaborations Outline Physics at the LHC Jet Reconstruction and Performance Clustering Algorithms
More informationJets (and photons) at the LHC. J. Huston LPC March 10, 2010
Jets (and photons) at the LHC J. Huston LPC March 10, 2010 More references Understanding cross sections at the LHC we have to understand QCD (at the LHC) PDF s, PDF luminosities and PDF uncertainties LO,
More informationJet reconstruction in W + jets events at the LHC
Jet reconstruction in W + jets events at the LHC Ulrike Schnoor Michigan State University High Energy Physics Institutsseminar IKTP TU Dresden, Nov 4, 010 Jet reconstruction in W + jets events at the LHC
More informationQCD at LHC in pp. Department of Theoretical Physics, Lund University
3rd Nordic LHC and Beyond Workshop 2-3 February 2009 Lund, Sweden QCD at LHC in pp Torbjörn Sjöstrand Department of Theoretical Physics, Lund University Introduction: the structure of an event Multiple
More informationThe inclusive jet cross section, jet algorithms, underlying event and fragmentation corrections. J. Huston Michigan State University
The inclusive jet cross section, jet algorithms, underlying event and fragmentation corrections J. Huston Michigan State University Tevatron in Run II 36 bunches (396 ns crossing time) 2 CDF in Run II
More informationWhat to do with Multijet Events?
DØ note 4465 2004-06-03 What to do with Multijet Events? T. Hebbeker RWTH Aachen ABSTRACT Multijet events are frequently produced in p p collisions. Events with several jets might indicate physics beyond
More informationTests of Pythia8 Rescattering Model
Tests of Pythia8 Rescattering Model arxiv:5.325v [hep-ph] Nov 25 Tasnuva Chowdhury Shahjalal University of Science and Technology Sylhet, Bangladesh. Deepak Kar University of Witwatersrand Johannesburg,
More informationQCD Jet Physics with CMS LHC
QCD Jet Physics with CMS Detector @ LHC Y.Chao for the CMS Collaboration (National Taiwan University, Taipei, Taiwan) QCD10 (25th annivervary) 2010/06/28-07/03 The Large Hadron Collider Four major experiments
More informationRecent forward physics and diffraction results from CMS
Recent forward physics and diffraction results from CMS Gabor Veres (CERN) on behalf of the CMS Collaboration ISMD 2015 Conference, Wildbad Kreuth, Germany October 5th, 2015 Outline CMS: forward instrumentation
More informationProton anti proton collisions at 1.96 TeV currently highest centre of mass energy
Tevatron & Experiments 2 Proton anti proton collisions at 1.96 TeV currently highest centre of mass energy Tevatron performing very well 6.5 fb 1 delivered (per experiment) 2 fb 1 recorded in 2008 alone
More informationResults from D0: dijet angular distributions, dijet mass cross section and dijet azimuthal decorrelations
Results from D: dijet angular distributions, dijet mass cross section and dijet azimuthal decorrelations Zdenek Hubacek Czech Technical University in Prague E-mail: zdenek.hubacek@cern.ch on behalf of
More informationSOFT QCD AT ATLAS AND CMS
SAHAL YACOOB UNIVERSITY OF CAPE TOWN ON BEHALF OF THE ATLAS AND CMS COLLABORATIONS SOFT QCD AT ATLAS AND CMS 28th Rencontres de Blois INTRODUCTION IN 15 MINUTES 2 Inelastic cross section ATLAS and CMS
More informationHow to Measure Top Quark Mass with CMS Detector??? Ijaz Ahmed Comsats Institute of Information Technology, Islamabad
How to Measure Top Quark Mass with CMS Detector??? Ijaz Ahmed Comsats Institute of Information Technology, Islamabad Outlines o o o o o o o High Pt top basic idea Methods for jets selection Top quark mass
More informationUnderlying Event measurements with first LHC data
Underlying Event measurements with first LHC data Holger Schulz Graduiertenkolleg Masse, Spektrum, Symmetrie Berlin, Septemer 29, 2009 Holger Schulz Underlying Event measurements with first LHC data 1
More informationCharmonium production versus multiplicity in PYTHIA8
Hard-Soft correlations in hadronic collisions Steffen Weber Charmonium production versus multiplicity in PYTHIA8 Hard-Soft correlations in hadronic collisions Clermont-Ferrand July 23, 2018 Steffen Weber
More informationSome studies for ALICE
Some studies for ALICE Motivations for a p-p programme in ALICE Special features of the ALICE detector Preliminary studies of Physics Performances of ALICE for the measurement of some global properties
More informationStudy of observables for measurement of MPI using Z+jets process
Study of observables for measurement of MPI using Z+jets process PANJAB University, IN Email: ramandeep.kumar@cern.ch AKAL University, IN 7th International Workshop on Multiple Parton Interactions at the
More informationTransverse Energy-Energy Correlation on Hadron Collider. Deutsches Elektronen-Synchrotron
Transverse Energy-Energy Correlation on Hadron Collider Wei Wang ( 王伟 ) Deutsches Elektronen-Synchrotron Work with Ahmed Ali, Fernando Barreiro, Javier Llorente arxiv: 1205.1689, Phys.Rev. D86, 114017(2012)
More informationParticle Physics. Lecture 11: Mesons and Baryons
Particle Physics Lecture 11: Mesons and Baryons Measuring Jets Fragmentation Mesons and Baryons Isospin and hypercharge SU(3) flavour symmetry Heavy Quark states 1 From Tuesday: Summary In QCD, the coupling
More informationMC ATLAS Stephen Jiggins on behalf of the ATLAS Collaboration University College London (UCL)
MC Tuning @ ATLAS Stephen Jiggins on behalf of the ATLAS Collaboration University College London (UCL) Contents Contents: 1) Monte Carlo models/event generation 2) Basic Tuning Methodology 3) A2 tune series
More informationSummary of Working Group C: Hadronic Final States DIS03, St.Petersburg
Summary of Working Group C: Hadronic Final States DIS03, St.Petersburg Conveners: Jon Butterworth, Yuri Dokshitzer Event shapes & energy flows: DIS final states vs e + e -. Jets and energy flows: proton-antiproton
More informationMBR Monte Carlo Simulation in PYTHIA8
The Rockefeller University, 10 York Avenue, New York, NY 06, USA E-mail: robert.ciesielski@rockefeller.edu Konstantin Goulianos The Rockefeller University, 10 York Avenue, New York, NY 06, USA E-mail:
More informationJet Physics with ALICE
Jet Physics with ALICE Oliver Busch for the ALICE collaboration Oliver Busch Tsukuba 2014 /03/13 1 Outline introduction results from pp jets in heavy-ion collisions results from Pb-Pb collisions jets in
More informationQCD Studies at the Tevatron
QCD Studies at the Tevatron Results from the CDF and DØ Collaborations Markus Wobisch, Louisiana Tech University DESY Seminar, June 24, 2008 Fermilab Tevatron - Run II CDF Chicago pp at 1.96 TeV DØ 36x36
More informationMeasurement of the associated production of direct photons and jets with the Atlas experiment at LHC. Michele Cascella
Measurement of the associated production of direct photons and jets with the Atlas experiment at LHC Michele Cascella Graduate Course in Physics University of Pisa The School of Graduate Studies in Basic
More informationRecent Results on Jet Physics and α s
Recent Results on Jet Physics and α s XXI Physics in Collision Conference Seoul, Korea June 8, Presented by Michael Strauss The University of Oklahoma Outline Introduction and Experimental Considerations
More informationMeasurement of multi-jet cross sections in proton proton collisions at a 7 TeV center-of-mass energy
Eur. Phys. J. C (2011) 71:1763 DOI 10.1140/epjc/s10052-011-1763-6 Regular Article - Experimental Physics Measurement of multi-jet cross sections in proton proton collisions at a 7 TeV center-of-mass energy
More informationPoS(IHEP-LHC-2011)008
in pp collisions at the LHC Sergei Lobanov Joint Institute for Nuclear Research, Dubna, Russian Federation E-mail: Sergey.Lobanov@cern.ch Artem Maevskiy M.V. Lomonosov Moscow State University, Russian
More informationLecture 5. QCD at the LHC Joey Huston Michigan State University
Lecture 5 QCD at the LHC Joey Huston Michigan State University Tevatron data Wealth of data from the Tevatron, both Run 1 and Run 2, that allows us to test/add to our pqcd formalism with analysis procedures/
More informationThe ATLAS Detector at the LHC
The ATLAS Detector at the LHC Results from the New Energy Frontier Cristina Oropeza Barrera Experimental Particle Physics University of Glasgow Somewhere near the Swiss Alps... A Toroidal LHC ApparatuS
More informationMulti-jet production and jet correlations at CMS
Multi-jet production and jet correlations at Gábor I. Veres on behalf of the Collaboration CERN E-mail: gabor.veres@cern.ch Hadronic jet production at the LHC is an excellent testing ground for QCD. Essential
More informationProperties of Proton-proton Collision and. Comparing Event Generators by Multi-jet Events
Properties of Proton-proton Collision and Comparing Event Generators by Multi-jet Events Author: W. H. TANG 1 (Department of Physics, The Chinese University of Hong Kong) Supervisors: Z. L. MARSHALL 2,
More informationIntroduction to Monte Carlo generators - II
Introduction to Monte Carlo generators - II (Fully exclusive modeling of high-energy collisions) Andrzej Siódmok CTEQ School - University of Pittsburgh, USA 18-28 July 2017 Thanks to: S. Gieseke, S.Höche,
More informationTop Quark Mass Reconstruction from High Pt Jets at LHC
Top Quark Mass Reconstruction from High Pt Jets at LHC IJAZ AHMED National Centre for Physics Islamabad, Pakistan Signaling the Arrival of the LHC Era, ICTP, Italy Outlines o o o o o o o o o o Motivations
More informationDouble & multi parton scatterings in p-a collisions at the LHC
Double & multi parton scatterings in p-a collisions at the LHC Workshop on MPI at the LHC Tel Aviv University, 17th Oct. 2012 David d'enterria CERN (*) Part of the results based on: Dd'E & A. Snigirev
More informationJET FRAGMENTATION DENNIS WEISER
JET FRAGMENTATION DENNIS WEISER OUTLINE Physics introduction Introduction to jet physics Jets in heavy-ion-collisions Jet reconstruction Paper discussion The CMS experiment Data selection and track/jet
More informationRecent progress from Les Houches WG. Photon isolation and fragmentation contribution
Recent progress from Les Houches WG Photon isolation and fragmentation contribution Workshop PPSHC - 30/03/2012 Nicolas Chanon - ETH Zürich In behalf of the Photon Les Houches WG N. Chanon, S. Gascon-Shotkin,
More informationRecent DØ results in Diffractive and Jet Physics
Recent DØ results in Diffractive and Jet Physics * Fermi National Accelerator Laboratory, P.O. Box 500, Batavia, IL 60510 E-mail: odell@fnal.gov DØ measurements of the inclusive jet cross section and the
More informationFYST17 Lecture 6 LHC Physics II
FYST17 Lecture 6 LHC Physics II 1 Today & Monday The LHC accelerator Challenges The experiments (mainly CMS and ATLAS) Important variables Preparations Soft physics EWK physics Some recent results Focus
More informationAzimuthal decorrelations between jets in QCD
Azimuthal decorrelations between jets in QCD Andrea Banfi ETH Zurich q q p 1 p 1 Outline Azimuthal decorrelations in QCD hard processes Dijets in the back-to-back region Phenomenology of azimuthal decorrelations
More informationHigh Pt Top Quark Mass Reconstruction in CMS
High Pt Top Quark Mass Reconstruction in CMS IJAZ AHMED National Centre for Physics (NCP), Islamabad First IPM meeting on LHC Physics, April 20-24 24 2009 Isfahan,, Iran Outlines o o o o o o o o o o Introduction
More informationDouble- & multi-parton scatterings in p-a collisions at the LHC
Double- & multi-parton scatterings in p-a collisions at the LHC Workshop on p-a collisions at the LHC ECT* Trento, 10th May 2013 David d'enterria CERN (*) Part of the results based on: Dd'E & A. Snigirev,
More informationMeasurement of jet production in association with a Z boson at the LHC & Jet energy correction & calibration at HLT in CMS
Measurement of jet production in association with a Z boson at the LHC & Jet energy correction & calibration at HLT in CMS Fengwangdong Zhang Peking University (PKU) & Université Libre de Bruxelles (ULB)
More informationMultiple Parton-Parton Interactions: from pp to A-A
Multiple Parton-Parton Interactions: from pp to A-A Andreas Morsch CERN QCD Challenges at LHC Taxco, Mexico, Jan 18-22 (2016) Multiple Parton-Parton Interactions Phys. Lett. B 167 (1986) 476 Q i 2 Λ QCD
More informationThe Heavy Quark Search at the LHC
The Heavy Quark Search at the LHC The Heavy Quark Search at the LHC Backgrounds: estimating and suppressing tt, multijets,... jet mass technique NLO effects matrix elements for extra jets initial state
More informationPhysics at Hadron Colliders
Physics at Hadron Colliders Part 2 Standard Model Physics Test of Quantum Chromodynamics - Jet production - W/Z production - Production of Top quarks Precision measurements -W mass - Top-quark mass QCD
More informationFYST17 Lecture 6 LHC Physics II
FYST17 Lecture 6 LHC Physics II 1 Today, (tomorrow) & Next week The LHC accelerator Challenges The experiments (mainly CMS and ATLAS) Important variables Preparations Soft physics minímum bias, underlying
More informationResults on QCD and Heavy Flavors Production at the Tevatron
Results on QCD and Heavy Flavors Production at the Tevatron Donatella Lucchesi INFN and University of Padova October 21 Padova Outline: Machine and detector description Latest results on QCD Heavy Flavor:
More informationarxiv: v1 [nucl-th] 23 Jan 2019
arxiv:1901.08157v1 [nucl-th] 23 Jan 2019 Cyclotron Institute and Department of Physics and Astronomy, Texas A&M University, College Station TX 77843, USA E-mail: rjfries@comp.tamu.edu Michael Kordell Cyclotron
More informationColin Jessop. University of Notre Dame
Colin Jessop University of Notre Dame Test the evolution of QCD to higher energies ( and lower x) Search for new particles with Quarks, gluons and photons in Final state Jet production is dominant process
More informationRidge correlation structure in high multiplicity pp collisions with CMS
Ridge correlation structure in high multiplicity pp collisions with CMS Dragos Velicanu for the CMS Collaboration MBUEWG CERN, Geneva, June 17 2011 Results from High Multiplicity pp Dragos Velicanu (MIT)
More informationarxiv: v1 [hep-ex] 15 Jan 2019
CMS-CR-8/37 January 7, 9 Top Quark Modelling and Tuning at CMS arxiv:9.559v [hep-ex] 5 Jan 9 Emyr Clement on behalf of the CMS Collaboration University of Bristol Recent measurements dedicated to improving
More informationTwo Early Exotic searches with dijet events at ATLAS
ATL-PHYS-PROC-2011-022 01/06/2011 Two Early Exotic searches with dijet events at ATLAS University of Toronto, Department of Physics E-mail: rrezvani@physics.utoronto.ca This document summarises two exotic
More informationQCD at the Tevatron: The Production of Jets & Photons plus Jets
QCD at the Tevatron: The Production of Jets & Photons plus Jets Mike Strauss The University of Oklahoma The Oklahoma Center for High Energy Physics for the CDF and DØD Collaborations APS 2009 Denver, Colorado
More informationEarly physics with Atlas at LHC
Early physics with Atlas at LHC Bellisario Esposito (INFN-Frascati) On behalf of the Atlas Collaboration Outline Atlas Experiment Physics goals Next LHC run conditions Physics processes observable with
More informationCMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on CMS information server CMS NOTE 1999/065 The Compact Muon Solenoid Experiment CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland 25 November 1999 Top mass determination in
More informationPoS(Confinement X)171
in pp collisions at LHC energies Institute for Particle and Nuclear Physics, Wigner RCP, HAS 2 Budapest, XII. Konkoly Thege Miklos ut 29-33 E-mail: sona.pochybova@cern.ch With increasing luminosities at
More informationNon-perturbative effects in transverse momentum distribution of electroweak bosons
Non-perturbative effects in transverse momentum distribution of electroweak bosons Andrzej Siódmok a,e in collaboration with M. H. Seymour b,c & S. Gieseke b,d a Jagiellonian University, b CERN, c University
More information