Workshop on Early LHC Physics May 6, 2009 Rick Field – Florida/CDF/CMSPage 1 Workshop on Early...

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Workshop on Early LHC Physics May 6, 200 9 Rick Field – Florida/CDF/CMS Page 1 Workshop on Early Physics Workshop on Early Physics Opportunities at the LHC Opportunities at the LHC Rick Field University of Florida Outline of Talk LBNL May 6, 2009 Proton A ntiProton PT(hard) O utgoing Parton O utgoing Parton U nderlying Event U nderlying Event Initial-State R adiation Final-State Radiation CMS at the LHC CDF Run 2 The Pythia MPI energy scaling parameter PARP(90). “Min-Bias” and the “underlying event” at the LHC. The “underlying event” in Drell-Yan lepton-pair production. n-Bias” and the “Underlying Event” The QCD Monte-Carlo Model tunes. LHC predictions! Summary & Conclusions. Early LHC Thesis Projects.

Transcript of Workshop on Early LHC Physics May 6, 2009 Rick Field – Florida/CDF/CMSPage 1 Workshop on Early...

Page 1: Workshop on Early LHC Physics May 6, 2009 Rick Field – Florida/CDF/CMSPage 1 Workshop on Early Physics Opportunities at the LHC Rick Field University of.

Workshop on Early LHC Physics May 6, 2009

Rick Field – Florida/CDF/CMS Page 1

Workshop on Early Physics Workshop on Early Physics Opportunities at the LHCOpportunities at the LHC

Rick FieldUniversity of Florida

Outline of TalkLBNL May 6, 2009

Proton AntiProton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

CMS at the LHCCDF Run 2

The Pythia MPI energy scaling parameter PARP(90).

“Min-Bias” and the “underlying event” at the LHC.

The “underlying event” in Drell-Yan lepton-pair production.

“Min-Bias” and the “Underlying Event”

The QCD Monte-Carlo Model tunes.

LHC predictions!

Summary & Conclusions.

Early LHC Thesis Projects.

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Rick Field – Florida/CDF/CMS Page 2

QCD Monte-Carlo Models:QCD Monte-Carlo Models:High Transverse Momentum JetsHigh Transverse Momentum Jets

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).

Hard Scattering

PT(hard)

Outgoing Parton

Outgoing Parton

Initial-State Radiation

Final-State Radiation

Hard Scattering

PT(hard)

Outgoing Parton

Outgoing Parton

Initial-State Radiation

Final-State Radiation

Proton AntiProton

Underlying Event Underlying Event

Proton AntiProton

Underlying Event Underlying Event

“Hard Scattering” Component

“Jet”

“Jet”

“Underlying Event”

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.

“Jet”

The “underlying event” is an unavoidable background to most collider observables and having good understand of it leads to

more precise collider measurements!

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QCD Monte-Carlo Models:QCD Monte-Carlo Models:Lepton-Pair ProductionLepton-Pair Production

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).

Proton AntiProton

Underlying Event Underlying Event

Proton AntiProton

Underlying Event Underlying Event

Lepton-Pair Production

Lepton

Anti-Lepton

Initial-State Radiation

Lepton-Pair Production

Lepton

Anti-Lepton

Initial-State Radiation

“Underlying Event”

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-state radiation.

“Jet”

Proton AntiProton

High PT Z-Boson Production

Z-boson

Outgoing Parton

Initial-State Radiation Final-State Radiation

High PT Z-Boson Production

Z-boson

Outgoing Parton

Initial-State Radiation

Final-State Radiation

“Hard Scattering” Component

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Parameter Default

Description

PARP(83) 0.5 Double-Gaussian: Fraction of total hadronic matter within PARP(84)

PARP(84) 0.2 Double-Gaussian: Fraction of the overall hadron radius containing the fraction PARP(83) of the total hadronic matter.

PARP(85) 0.33 Probability that the MPI produces two gluons with color connections to the “nearest neighbors.

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.

PARP(89) 1 TeV Determines the reference energy E0.

PARP(90) 0.16 Determines the energy dependence of the cut-off

PT0 as follows PT0(Ecm) = PT0(Ecm/E0) with = PARP(90)

PARP(67) 1.0 A scale factor that determines the maximum parton virtuality for space-like showers. The larger the value of PARP(67) the more initial-state radiation.

Hard Core

Multiple Parton Interaction

Color String

Color String

Multiple Parton Interaction

Color String

Hard-Scattering Cut-Off PT0

1

2

3

4

5

100 1,000 10,000 100,000

CM Energy W (GeV)P

T0

(G

eV

/c)

PYTHIA 6.206

= 0.16 (default)

= 0.25 (Set A))

Take E0 = 1.8 TeV

Reference pointat 1.8 TeV

Determine by comparingwith 630 GeV data!

Affects the amount ofinitial-state radiation!

Tuning PYTHIA:Tuning PYTHIA:Multiple Parton Interaction ParametersMultiple Parton Interaction Parameters

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““Transverse” ConesTransverse” Conesvs “Transverse” Regionsvs “Transverse” Regions

Sum the PT of charged particles in two cones of radius 0.7 at the same as the leading jet but with || = 90o.

Plot the cone with the maximum and minimum PTsum versus the ET of the leading (calorimeter) jet.

-1 +1

2

0

Leading Jet

Toward Region

Transverse Region

Transverse Region

Away Region

Away Region

-1 +1

2

0

Leading Jet

Cone 1

Cone 2 Transverse Region:

2/3=0.67

Transverse Cone:

(0.7)2=0.49

“Cone Analysis”(Tano, Kovacs, Huston, Bhatti)

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Energy DependenceEnergy Dependenceof the “Underlying Event”of the “Underlying Event”

Sum the PT of charged particles (pT > 0.4 GeV/c) in two cones of radius 0.7 at the same as the leading jet but with || = 90o. Plot the cone with the maximum and minimum PT sum versus the ET of the leading (calorimeter) jet.

Note that PYTHIA 6.115 is tuned at 630 GeV with PT0 = 1.4 GeV and at 1,800 GeV with PT0 = 2.0 GeV. This implies that = PARP(90) should be around 0.30 instead of the 0.16 (default).

For the MIN cone 0.25 GeV/c in radius R = 0.7 implies a PT sum density of dPTsum/dd = 0.16 GeV/c and 1.4 GeV/c in the MAX cone implies dPTsum/dd = 0.91 GeV/c (average PTsum density of 0.54 GeV/c per unit -).

“Cone Analysis”(Tano, Kovacs, Huston, Bhatti)

630 GeV

PYTHIA 6.115PT0 = 2.0 GeV

1,800 GeV

PYTHIA 6.115PT0 = 1.4 GeV

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““Transverse” Charged DensitiesTransverse” Charged DensitiesEnergy DependenceEnergy Dependence

"Transverse" Charged PTsum Density: dPTsum/dd

0.00

0.20

0.40

0.60

0 5 10 15 20 25 30 35 40 45 50

PT(charged jet#1) (GeV/c)

Ch

arg

ed P

Tsu

m D

ensi

ty (

GeV

)

Pythia 6.206 (Set A) 630 GeV ||<1.0 PT>0.4 GeV

CTEQ5L

HERWIG 6.4 = 0.25

= 0

= 0.16

"Min Transverse" PTsum Density: dPTsum/dd

0.0

0.1

0.2

0.3

0 5 10 15 20 25 30 35 40 45 50

PT(charged jet#1) (GeV/c)

Ch

arg

ed P

Tsu

m D

ensi

ty (

GeV

)

630 GeV ||<1.0 PT>0.4 GeV

= 0.25HERWIG 6.4

= 0.16 = 0

CTEQ5L

Pythia 6.206 (Set A)

Shows the “transverse” charged PTsum density (||<1, PT>0.4 GeV) versus PT(charged jet#1) at 630 GeV predicted by HERWIG 6.4 (PT(hard) > 3 GeV/c, CTEQ5L) and a tuned version of PYTHIA 6.206 (PT(hard) > 0, CTEQ5L, Set A, = 0, = 0.16 (default) and = 0.25 (preferred)).

Also shown are the PTsum densities (0.16 GeV/c and 0.54 GeV/c) determined from the Tano cone analysis at 630 GeV

Hard-Scattering Cut-Off PT0

1

2

3

4

5

100 1,000 10,000 100,000

CM Energy W (GeV)

PT

0

(Ge

V/c

)

PYTHIA 6.206

= 0.16 (default)

= 0.25 (Set A))

Lowering PT0 at 630 GeV (i.e. increasing ) increases UE activity

resulting in less energy dependence.

Increasing produces less energy dependence for the UE resulting in

less UE activity at the LHC!

Reference pointE0 = 1.8 TeV

Rick Field Fermilab MC WorkshopOctober 4, 2002!

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PYTHIA 6.2 TunesPYTHIA 6.2 TunesParameter Tune AW Tune DW Tune D6

PDF CTEQ5L CTEQ5L CTEQ6L

MSTP(81) 1 1 1

MSTP(82) 4 4 4

PARP(82) 2.0 GeV 1.9 GeV 1.8 GeV

PARP(83) 0.5 0.5 0.5

PARP(84) 0.4 0.4 0.4

PARP(85) 0.9 1.0 1.0

PARP(86) 0.95 1.0 1.0

PARP(89) 1.8 TeV 1.8 TeV 1.8 TeV

PARP(90) 0.25 0.25 0.25

PARP(62) 1.25 1.25 1.25

PARP(64) 0.2 0.2 0.2

PARP(67) 4.0 2.5 2.5

MSTP(91) 1 1 1

PARP(91) 2.1 2.1 2.1

PARP(93) 15.0 15.0 15.0

Intrinsic KT

ISR Parameter

UE Parameters

Uses CTEQ6L

All use LO s with = 192 MeV!

Tune A energy dependence!

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PYTHIA 6.2 TunesPYTHIA 6.2 TunesParameter Tune DWT Tune D6T ATLAS

PDF CTEQ5L CTEQ6L CTEQ5L

MSTP(81) 1 1 1

MSTP(82) 4 4 4

PARP(82) 1.9409 GeV 1.8387 GeV 1.8 GeV

PARP(83) 0.5 0.5 0.5

PARP(84) 0.4 0.4 0.5

PARP(85) 1.0 1.0 0.33

PARP(86) 1.0 1.0 0.66

PARP(89) 1.96 TeV 1.96 TeV 1.0 TeV

PARP(90) 0.16 0.16 0.16

PARP(62) 1.25 1.25 1.0

PARP(64) 0.2 0.2 1.0

PARP(67) 2.5 2.5 1.0

MSTP(91) 1 1 1

PARP(91) 2.1 2.1 1.0

PARP(93) 15.0 15.0 5.0

Intrinsic KT

ISR Parameter

UE Parameters

All use LO s with = 192 MeV!

ATLAS energy dependence!

Tune A

Tune AW Tune B Tune BW

Tune D

Tune DWTune D6

Tune D6T

These are “old” PYTHIA 6.2 tunes! There are new 6.420 tunes by

Peter Skands (Tune S320, update of S0)Peter Skands (Tune N324, N0CR)

Hendrik Hoeth (Tune P329, “Professor”)

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Peter’s Pythia Tunes WEBsitePeter’s Pythia Tunes WEBsite

http://home.fnal.gov/~skands/leshouches-plots/

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11stst Workshop on Energy Scaling Workshop on Energy Scalingin Hadron-Hadron Collisionsin Hadron-Hadron Collisions

“On the Boarder” restaurant, Aurora, ILApril 27, 2009

Peter Skands!

Renee Fatemi gave a talk on the “underlying event at ATAR!

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The “Underlying Event” at STARThe “Underlying Event” at STAR

At STAR they have measured the “underlying event at W = 200 GeV (|| < 1, pT > 0.2 GeV) and compared with Pythia Tune A.

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Proton-AntiProton CollisionsProton-AntiProton Collisionsat the Tevatronat the Tevatron

Elastic Scattering Single Diffraction

M

tot = ELSD DD HC

Double Diffraction

M1 M2

Proton AntiProton

“Soft” Hard Core (no hard scattering)

Proton AntiProton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

“Hard” Hard Core (hard scattering)

Hard Core

1.8 TeV: 78mb = 18mb + 9mb + (4-7)mb + (47-44)mb

The CDF “Min-Bias” trigger picks up most of the “hard

core” cross-section plus a small amount of single & double

diffraction.

The “hard core” component contains both “hard” and

“soft” collisions.

Beam-Beam Counters

3.2 < || < 5.9

CDF “Min-Bias” trigger1 charged particle in forward BBC

AND1 charged particle in backward BBC

tot = ELIN

“Inelastic Non-Diffractive Component”

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Charged Particle Density: dN/dCharged Particle Density: dN/dCharged Particle Density: dN/d

0.0

1.0

2.0

3.0

4.0

5.0

-8 -6 -4 -2 0 2 4 6 8

PseudoRapidity

Ch

arg

ed

Par

ticl

e D

en

sit

y

Min-Bias1.96 TeV

PY Tune A

PY64 Tune P329

RDF Preliminarygenerator level

PY64 Tune S320

Charged Particles (all PT)

Charged Particle Density: dN/d

0.0

0.5

1.0

1.5

2.0

-8 -6 -4 -2 0 2 4 6 8

PseudoRapidity

Ch

arg

ed

Par

ticl

e D

en

sit

y

RDF Preliminarygenerator level

Charged Particles (PT>0.5 GeV/c)

Min-Bias1.96 TeV

PY64 Tune P329

PY Tune A

PY64 Tune S320

Charged particle (all pT) pseudo-rapidity distribution, dNchg/dd, at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324.

Charged particle (pT>0.5 GeV/c) pseudo-rapidity distribution, dNchg/dd, at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324.

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Charged Particle Density: dN/dCharged Particle Density: dN/d

Proton AntiProton

“Minumum Bias” Collisions

Tevatron LHC

Extrapolations of PYTHIA Tune A, Tune S320, and Tune P329 to the LHC.

Charged Particle Density: dN/d

0.0

1.0

2.0

3.0

4.0

5.0

-8 -6 -4 -2 0 2 4 6 8

PseudoRapidity

Ch

arg

ed

Part

icle

De

ns

ity

Min-Bias1.96 TeV

PY Tune A

PY64 Tune P329

RDF Preliminarygenerator level

PY64 Tune S320

Charged Particles (all PT)

Charged Particle Density: dN/d

0.0

2.0

4.0

6.0

8.0

-8 -6 -4 -2 0 2 4 6 8

PseudoRapidity

Ch

arg

ed

Pa

rtic

le D

en

sit

y

RDF Preliminarygenerator level

Charged Particles (all PT) Min-Bias14 TeV

PY Tune A

PY64 Tune P329

PY64 Tune S320

Charged particle (all pT) pseudo-rapidity distribution, dNchg/dd, at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324.

Proton Proton

“Minumum Bias” Collisions

RDF LHC Prediction!

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Charged Particle Density: dN/dCharged Particle Density: dN/d

Proton AntiProton

“Minumum Bias” Collisions

Tevatron LHC

Extrapolations of PYTHIA Tune A, Tune S320, and Tune P329 to the LHC.

Charged particle (pT > 0.5 GeV/c) pseudo-rapidity distribution, dNchg/dd, at 1.96 TeV for inelastic non-diffractive collisions from PYTHIA Tune A, Tune S320, and Tune P324.

Proton Proton

“Minumum Bias” Collisions

Charged Particle Density: dN/d

0.0

0.5

1.0

1.5

2.0

-8 -6 -4 -2 0 2 4 6 8

PseudoRapidity

Ch

arg

ed

Part

icle

De

ns

ity

RDF Preliminarygenerator level

Charged Particles (PT>0.5 GeV/c)

Min-Bias1.96 TeV

PY64 Tune P329

PY Tune A

PY64 Tune S320

Charged Particle Density: dN/d

0.0

1.0

2.0

3.0

4.0

-8 -6 -4 -2 0 2 4 6 8

PseudoRapidity

Ch

arg

ed

Pa

rtic

le D

en

sit

y

RDF Preliminarygenerator level

Charged Particles (PT>0.5 GeV/c) Min-Bias14 TeV

PY64 Tune P329

PY Tune A

PY64 Tune S320

RDF LHC Prediction!

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Min-Bias CorrelationsMin-Bias Correlations

Data at 1.96 TeV on the average pT of charged particles versus the number of charged particles (pT > 0.4 GeV/c, || < 1) for “min-bias” collisions at CDF Run 2. The data are corrected to the particle level and are compared with PYTHIA Tune A at the particle level (i.e. generator level).

Proton AntiProton

“Minumum Bias” Collisions

Average PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 10 20 30 40 50

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarydata corrected

generator level theory

Charged Particles (||<1.0, PT>0.4 GeV/c)

Min-Bias1.96 TeV

ATLAS

pyA

pyDW

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Min-Bias: Average PT versus NchgMin-Bias: Average PT versus Nchg

Proton AntiProton

“Soft” Hard Core (no hard scattering)

Proton AntiProton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

“Hard” Hard Core (hard scattering)

CDF “Min-Bias”

= +

Average PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 5 10 15 20 25 30 35 40

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarydata corrected

generator level theory

Charged Particles (||<1.0, PT>0.4 GeV/c)

Min-Bias1.96 TeV

pyAnoMPI

ATLAS

pyA

Proton AntiProton

Multiple-Parton Interactions

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Final-State Radiation

Initial-State Radiation

+

Beam-beam remnants (i.e. soft hard core) produces low multiplicity and small <pT> with <pT> independent of the multiplicity.

Hard scattering (with no MPI) produces large multiplicity and large <pT>.

Hard scattering (with MPI) produces large multiplicity and medium <pT>.

The CDF “min-bias” trigger picks up most of the “hard

core” component!

This observable is sensitive to the MPI tuning!

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Average PT versus NchgAverage PT versus Nchg

Proton AntiProton

“Minumum Bias” Collisions

Proton AntiProton

Drell-Yan Production

Anti-Lepton

Lepton

Underlying Event Underlying Event

Data at 1.96 TeV on the average pT of charged particles versus the number of charged particles (pT > 0.4 GeV/c, || < 1) for “min-bias” collisions at CDF Run 2. The data are corrected to the particle leveland are compared with PYTHIA Tune A, Tune DW, and the ATLAS tune at the particle level (i.e. generator level).

Particle level predictions for the average pT of charged particles versus the number of charged particles (pT > 0.5 GeV/c, || < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV) at CDF Run 2.

Average PT versus Nchg

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25 30 35

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarygenerator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

HW

JIM

pyAW

ATLAS

Average PT versus Nchg

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25 30 35

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarydata corrected

generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

HW

JIM

pyAW

ATLAS

Average PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 5 10 15 20 25 30 35 40

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarydata corrected

generator level theory

Charged Particles (||<1.0, PT>0.4 GeV/c)

Min-Bias1.96 TeV

pyAnoMPI

ATLAS

pyA

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Rick Field – Florida/CDF/CMS Page 20

Average PT versus NchgAverage PT versus Nchg

Proton AntiProton

Drell-Yan Production (no MPI)

Anti-Lepton

Lepton

Underlying Event Underlying Event

Average PT versus Nchg

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25 30 35

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarydata corrected

generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

HW

JIM

pyAW

ATLAS

Proton AntiProton

Drell-Yan Production (with MPI)

Anti-Lepton

Lepton

Underlying Event Underlying Event

Drell-Yan

Proton AntiProton

High PT Z-Boson Production

Z-boson

Outgoing Parton

Initial-State Radiation Final-State Radiation

= +

Z-boson production (with low pT(Z) and no MPI) produces low multiplicity and small <pT>.

+

High pT Z-boson production produces large multiplicity and high <pT>.

Z-boson production (with MPI) produces large multiplicity and medium <pT>.

No MPI!

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Rick Field – Florida/CDF/CMS Page 21

Average PT(Z) versus NchgAverage PT(Z) versus Nchg

Proton AntiProton

Drell-Yan Production

Anti-Lepton

Lepton

Underlying Event Underlying Event

Data on the average pT of charged particles versus the number of charged particles (pT > 0.5 GeV/c, || < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV) at CDF Run 2. The data are corrected to the particle level and are compared with various Monte-Carlo tunes at the particle level ( i.e. generator level).

Average PT versus Nchg

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25 30 35

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarydata corrected

generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

HW

JIM

pyAW

ATLAS

PT(Z-Boson) versus Nchg

0

20

40

60

80

0 5 10 15 20 25 30 35 40

Number of Charged Particles

Ave

rag

e P

T(Z

) (G

eV

/c)

CDF Run 2 Preliminarygenerator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

pyAW

HW

JIM

ATLAS

No MPI!

Predictions for the average PT(Z-Boson) versus the number of charged particles (pT > 0.5 GeV/c, || < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV) at CDF Run 2.

PT(Z-Boson) versus Nchg

0

20

40

60

80

0 5 10 15 20 25 30 35 40

Number of Charged Particles

Ave

rag

e P

T(Z

) (G

eV/c

)

CDF Run 2 Preliminarydata corrected

generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

pyAW

HW

JIM

ATLAS

Proton AntiProton

High PT Z-Boson Production

Z-boson

Outgoing Parton

Initial-State Radiation

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Rick Field – Florida/CDF/CMS Page 22

Average PT versus NchgAverage PT versus Nchg

Proton AntiProton

Drell-Yan Production

Anti-Lepton

Lepton

Underlying Event Underlying Event

Predictions for the average pT of charged particles versus the number of charged particles (pT > 0.5 GeV/c, || < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV, PT(pair) < 10 GeV/c) at CDF Run 2.

Average Charged PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 5 10 15 20 25 30 35

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarygenerator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

PT(Z) < 10 GeV/c

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

HW

pyAW

Average Charged PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 5 10 15 20 25 30 35

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarygenerator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

PT(Z) < 10 GeV/c

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

HW

JIM

ATLAS

pyAW

Average Charged PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 5 10 15 20 25 30 35

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

CDF Run 2 Preliminarydata corrected

generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

PT(Z) < 10 GeV/c

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

HW

JIM

ATLAS

pyAW

Data the average pT of charged particles versus the number of charged particles (pT > 0.5 GeV/c, || < 1, excluding the lepton-pair) for for Drell-Yan production (70 < M(pair) < 110 GeV, PT(pair) < 10 GeV/c) at CDF Run 2. The data are corrected to the particle level and are compared with various Monte-Carlo tunes at the particle level (i.e. generator level).

PT(Z) < 10 GeV/c

No MPI!

Average PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 10 20 30 40

Number of Charged Particles

Ave

rag

e P

T (

Ge

V/c

)

CDF Run 2 Preliminarydata corrected

generator level theory

Charged Particles (||<1.0)pyA

Min-Bias PT > 0.4 GeV/c

Drell-Yan PT > 0.5 GeV PT(Z) < 10 GeV/c

pyAW

Proton AntiProton

“Minumum Bias” Collisions Remarkably similar behavior! Perhaps indicating that MPI playing an important role in

both processes.

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Rick Field – Florida/CDF/CMS Page 23

Min-Bias: Average PT versus NchgMin-Bias: Average PT versus Nchg

Proton AntiProton

“Minumum Bias” Collisions

Tevatron LHC

Extrapolations of PYTHIA Tune A, Tune DW, Tune S320, and Tune P324 to the LHC.

The average pT of charged particles versus the number of charged particles (pT > 0.5 GeV/c, || < 1) for “min-bias” collisions at 1.96 TeV from PYTHIA Tune A, Tune DW, Tune S320, Tune N324, and Tune P324.

Proton Proton

“Minumum Bias” Collisions

Average PT versus Nchg

0.6

0.8

1.0

1.2

1.4

0 5 10 15 20 25 30 35

Number of Charged Particles

Av

era

ge

PT

(G

eV

/c)

Min-Bias1.96 TeV

RDF Preliminarygenerator level

PY64 Tune N324

Charged Particles (||<1.0, PT>0.5 GeV/c)

PY64 Tune P329

PY Tune A

PY64 Tune S320

PY Tune DW

Average PT versus Nchg

0.6

0.8

1.0

1.2

1.4

1.6

0 5 10 15 20 25 30 35 40

Number of Charged Particles

Ave

rag

e P

T (

GeV

/c)

Min-Bias14 TeV

RDF Preliminarygenerator level

Charged Particles (||<1.0, PT>0.5 GeV/c)

PY Tune DWPY Tune A

PY64 Tune P329

PY64 Tune S320

RDF LHC Prediction!

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Rick Field – Florida/CDF/CMS Page 24

Use the maximum pT charged particle in the event, PTmax, to define a direction and look at the the “associated” density, dNchg/dd, in “min-bias” collisions (pT > 0.5 GeV/c, || < 1).

PTmax Direction

Correlations in

Charged Particle Density: dN/dd

0.0

0.1

0.2

0.3

0.4

0.5

0 30 60 90 120 150 180 210 240 270 300 330 360

(degrees)

Ch

arg

ed

Pa

rtic

le D

en

sit

y

PTmax

Associated DensityPTmax not included

CDF Preliminarydata uncorrected

Charged Particles (||<1.0, PT>0.5 GeV/c)

Charge Density

Min-Bias

“Associated” densities do not include PTmax!

Highest pT charged particle!

PTmax Direction

Correlations in

Shows the data on the dependence of the “associated” charged particle density, dNchg/dd, for charged particles (pT > 0.5 GeV/c, || < 1, not including PTmax) relative to PTmax (rotated to 180o) for “min-bias” events. Also shown is the average charged particle density, dNchg/dd, for “min-bias” events.

It is more probable to find a particle accompanying PTmax than it is to

find a particle in the central region!

CDF Run 2 Min-Bias “Associated”CDF Run 2 Min-Bias “Associated”Charged Particle DensityCharged Particle Density

Page 25: Workshop on Early LHC Physics May 6, 2009 Rick Field – Florida/CDF/CMSPage 1 Workshop on Early Physics Opportunities at the LHC Rick Field University of.

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Associated Particle Density: dN/dd

0.0

0.2

0.4

0.6

0.8

1.0

0 30 60 90 120 150 180 210 240 270 300 330 360

(degrees)

As

so

cia

ted

Pa

rtic

le D

en

sit

y

PTmax > 2.0 GeV/c

PTmax > 1.0 GeV/c

PTmax > 0.5 GeV/c

CDF Preliminarydata uncorrected

PTmaxPTmax not included

Charged Particles (||<1.0, PT>0.5 GeV/c)

Min-Bias

PTmax Direction

Correlations in

Shows the data on the dependence of the “associated” charged particle density, dNchg/dd, for charged particles (pT > 0.5 GeV/c, || < 1, not including PTmax) relative to PTmax (rotated to 180o) for “min-bias” events with PTmax > 0.5, 1.0, and 2.0 GeV/c.

Transverse Region

Transverse Region

Jet #1

Shows “jet structure” in “min-bias” collisions (i.e. the “birth” of the leading two jets!).

Jet #2

Ave Min-Bias0.25 per unit -

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

PTmax > 0.5 GeV/c

PTmax > 2.0 GeV/c

CDF Run 2 Min-Bias “Associated”CDF Run 2 Min-Bias “Associated”Charged Particle DensityCharged Particle Density Rapid rise in the particle

density in the “transverse” region as PTmax increases!

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Rick Field – Florida/CDF/CMS Page 26

Shows the data on the dependence of the “associated” charged particle density, dNchg/dd, for charged particles (pT > 0.5 GeV/c, || < 1, not including PTmax) relative to PTmax (rotated to 180o) for “min-bias” events with PTmax > 0.5 GeV/c and PTmax > 2.0 GeV/c compared with PYTHIA Tune A (after CDFSIM).

PTmax Direction

Correlations in

Associated Particle Density: dN/dd

0.0

0.2

0.4

0.6

0.8

1.0

0 30 60 90 120 150 180 210 240 270 300 330 360

(degrees)

As

so

cia

ted

Pa

rtic

le D

en

sit

y

PTmax > 2.0 GeV/c

PY Tune A

PTmax > 0.5 GeV/c

PY Tune A

CDF Preliminarydata uncorrectedtheory + CDFSIM

PTmaxPTmax not included (||<1.0, PT>0.5 GeV/c)

PY Tune A 1.96 TeV

PYTHIA Tune A predicts a larger correlation than is seen in the “min-bias” data (i.e. Tune A “min-bias” is a bit too “jetty”).

PTmax > 2.0 GeV/c

PTmax > 0.5 GeV/c

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

Transverse Region Transverse

Region

PY Tune A

CDF Run 2 Min-Bias “Associated”CDF Run 2 Min-Bias “Associated”Charged Particle DensityCharged Particle Density

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Rick Field – Florida/CDF/CMS Page 27

Min-Bias “Associated”Min-Bias “Associated”Charged Particle DensityCharged Particle Density

Shows the “associated” charged particle density in the “toward”, “away” and “transverse” regions as a function of PTmax for charged particles (pT > 0.5 GeV/c, || < 1, not including PTmax) for “min-bias” events at 1.96 TeV from PYTHIA Tune A (generator level).

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

Associated Charged Particle Density: dN/dd

0.0

0.1

1.0

10.0

0 30 60 90 120 150 180 210 240 270 300 330 360

(degrees)

Ch

arg

ed

Par

ticl

e D

en

sit

y

RDF Preliminarypy Tune A generator level

Charged Particles (||<1.0, PT>0.5 GeV/c)

Min-Bias1.96 TeV

PTmax > 0.5 GeV/cPTmax > 1.0 GeV/c

PTmax > 2.0 GeV/cPTmax > 5.0 GeV/c

PTmax > 10.0 GeV/c

Associated Charged Particle Density: dN/dd

0.0

0.4

0.8

1.2

1.6

0 2 4 6 8 10 12 14 16 18 20

PTmax (GeV/c)

Ch

arg

ed P

arti

cle

Den

sity

RDF Preliminarypy Tune A generator level

Min-Bias1.96 TeV

Charged Particles (||<1.0, PT>0.5 GeV/c)

"Toward"

"Transverse"

"Away"

Shows the dependence of the “associated” charged particle density, dNchg/dd, for charged particles (pT > 0.5 GeV/c, || < 1, not including PTmax) relative to PTmax (rotated to 180o) for “min-bias” events at 1.96 TeV with PTmax > 0.5, 1.0, 2.0, 5.0, and 10.0 GeV/c from PYTHIA Tune A (generator level).

Associated Charged Particle Density: dN/dd

0.0

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25

PTmax (GeV/c)

Ch

arg

ed

Par

ticl

e D

en

sit

y

Charged Particles (||<1.0, PT>0.5 GeV/c)

Min-Bias14 TeV

"Toward"

"Transverse"

"Away"

RDF Preliminarypy Tune A generator level

"Transverse" Charged Particle Density: dN/dd

0.0

0.2

0.4

0.6

0.8

1.0

1.2

0 5 10 15 20 25

PTmax (GeV/c)

"Tra

ns

vers

e"

Ch

arg

ed D

ensi

ty

RDF Preliminarypy Tune A generator level

Min-Bias

Charged Particles (||<1.0, PT>0.5 GeV/c)

14 TeV

1.96 TeV

“Toward” Region

“Transverse” “Transverse”

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

~ factor of 2!

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Rick Field – Florida/CDF/CMS Page 30

Min-Bias “Associated”Min-Bias “Associated”Charged Particle DensityCharged Particle Density

Shows the “associated” charged particle density in the “transverse” region as a function of PTmax for charged particles (pT > 0.5 GeV/c, || < 1, not including PTmax) for “min-bias” events at 1.96 TeV from PYTHIA Tune A, Tune S320, Tune N324, and Tune P329 at the particle level (i.e. generator level).

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

"Transverse" Charged Particle Density: dN/dd

0.0

0.2

0.4

0.6

0.8

0 2 4 6 8 10 12 14 16 18 20

PTmax (GeV/c)

"Tra

ns

ve

rse

" C

harg

ed

Den

sit

y RDF Preliminarygenerator level

PY Tune A

PY64 Tune P329

PY64 Tune S320

Charged Particles (||<1.0, PT>0.5 GeV/c)

PY64 Tune N324

Min-Bias1.96 TeV

"Transverse" Charged Particle Density: dN/dd

0.0

0.4

0.8

1.2

1.6

0 5 10 15 20 25

PTmax (GeV/c)

"Tra

nsv

ers

e" C

har

ged

Den

sit

y

PY Tune A

Min-Bias14 TeV Charged Particles (||<1.0, PT>0.5 GeV/c)

RDF Preliminarygenerator level

PY64 Tune P329

PY64 Tune S320 PY Tune DW

PY Tune DWT

Tevatron LHC

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

Extrapolations of PYTHIA Tune A, Tune DW, Tune DWT, Tune S320, and Tune P329 to the LHC.

RDF LHC Prediction!

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Rick Field – Florida/CDF/CMS Page 31

Z-Boson Direction

“Toward”

“Transverse” “Transverse”

“Away”

Charged Particle DensityCharged Particle Density

Data at 1.96 TeV on the density of charged particles, dN/dd, with pT > 0.5 GeV/c and || < 1 for “Z-Boson” and “Leading Jet” events as a function of the leading jet pT or PT(Z) for the “toward”, “away”, and “transverse” regions. The data are corrected to the particle level (with errors that include both the statistical error and the systematic uncertainty) and are compared with PYTHIA Tune AW and Tune A, respectively, at the particle level (i.e. generator level).

Jet #1 Direction

“Toward”

“Transverse” “Transverse”

“Away”

Charged Particle Density: dN/dd

0

1

2

3

4

0 20 40 60 80 100 120 140 160 180 200

PT(jet#1) (GeV/c)

Ave

rag

e C

har

ge

d D

en

sity

CDF Run 2 Preliminarydata corrected

pyA generator level

"Leading Jet"MidPoint R=0.7 |(jet#1)|<2

Charged Particles (||<1.0, PT>0.5 GeV/c)

"Away"

"Toward"

"Transverse"

Charged Particle Density: dN/dd

0

1

2

3

0 20 40 60 80 100

PT(Z-Boson) (GeV/c)

Ave

rag

e C

har

ge

d D

ensi

ty

CDF Run 2 Preliminarydata corrected

pyAW generator level"Away"

"Transverse"

"Toward"

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

Proton AntiProton

High PT Z-Boson Production

Z-boson

Outgoing Parton

Initial-State Radiation

Proton AntiProton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

"Transverse" Charged Particle Density: dN/dd

0.0

0.3

0.6

0.9

1.2

0 20 40 60 80 100 120 140 160 180 200

PT(jet#1) or PT(Z-Boson) (GeV/c)

"Tra

nsv

erse

" C

ha

rged

Den

sit

y

CDF Run 2 Preliminarydata corrected

generator level theory

Charged Particles (||<1.0, PT>0.5 GeV/c)

"Leading Jet"

"Z-Boson"

"Away" Charged Particle Density: dN/dd

0

1

2

3

4

0 20 40 60 80 100 120 140 160 180 200

PT(jet#1) or PT(Z-Boson) (GeV/c)

"Aw

ay"

Ch

arg

ed D

ensi

ty

CDF Run 2 Preliminarydata corrected

generator level theory

Charged Particles (||<1.0, PT>0.5 GeV/c)

"Leading Jet"

"Z-Boson"

"Away" Charged Particle Density: dN/dd

0

1

2

3

0 20 40 60 80 100

PT(Z-Boson) (GeV/c)

"Aw

ay"

Ch

arg

ed D

en

sity

CDF Run 2 Preliminarydata corrected

generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

JIM

HW

pyAW

HERWIG + JIMMYTune (PTJIM = 3.6)

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Z-Boson: “Towards”, Transverse”, Z-Boson: “Towards”, Transverse”, & “TransMIN” Charge Density& “TransMIN” Charge Density

Data at 1.96 TeV on the density of charged particles, dN/dd, with pT > 0.5 GeV/c and || < 1 for “Z-Boson” events as a function of PT(Z) for the “toward” and “transverse” regions. The data are corrected to the particle level (with errors that include both the statistical error and the systematic uncertainty) and are compared with PYTHIA Tune AW and HERWIG (without MPI) at the particle level (i.e. generator level).

Z-BosonDirection

“Toward”

“Transverse” “Transverse”

“Away”

Charged Particle Density: dN/dd

0.0

0.3

0.6

0.9

0 20 40 60 80 100

PT(Z-Boson) (GeV/c)

Ch

arg

ed

De

ns

ity

CDF Run 2 Preliminarydata corrected

pyAW generator level"Transverse

"Toward"

"Drell-Yan Production"70 < M(pair) < 110 GeV Charged Particles (||<1.0, PT>0.5 GeV/c)

excluding the lepton-pair

Proton AntiProton

High PT Z-Boson Production

Z-boson

Outgoing Parton

Initial-State Radiation

Proton AntiProton

High PT Z-Boson Production

Z-boson

Outgoing Parton

Initial-State Radiation

Charged Particle Density: dN/dd

0.0

0.3

0.6

0.9

0 20 40 60 80 100

PT(Z-Boson) (GeV/c)

Ch

arg

ed

De

ns

ity

CDF Run 2 Preliminarydata corrected

pyAW generator level

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

"Toward"

"transMIN"

Z-Boson Direction

“Toward”

“TransMAX” “TransMIN”

“Away”

"Toward" Charged Particle Density: dN/dd

0.0

0.3

0.6

0.9

0 20 40 60 80 100

PT(Z-Boson) (GeV/c)

"To

war

d"

Ch

arg

ed D

ensi

ty

CDF Run 2 Preliminarydata corrected

generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV Charged Particles (||<1.0, PT>0.5 GeV/c)

excluding the lepton-pair

HW

JIM

pyAW

ATLASpyDW

"TransMIN" Charged Particle Density: dN/dd

0.0

0.2

0.4

0.6

0 20 40 60 80 100

PT(Z-Boson) (GeV/c)

"Tra

ns

MIN

" C

har

ged

De

ns

ity CDF Run 2 Preliminary

data corrected generator level theory

"Drell-Yan Production"70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)excluding the lepton-pair

ATLAS

HWpyAW

JIM

pyDW

"TransMIN" Charged Particle Density: dN/dd

0.0

0.2

0.4

0.6

0.8

0 20 40 60 80 100 120 140 160 180 200

PT(jet#1) or PT(Z-Boson) (GeV/c)

"Tra

nsM

IN"

Ch

arg

ed D

en

sit

y CDF Run 2 Preliminarydata corrected

generator level theory

Charged Particles (||<1.0, PT>0.5 GeV/c)

"Leading Jet"

"Z-Boson"

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"Toward" Charged Particle Density: dN/dd

0.0

0.4

0.8

1.2

1.6

0 25 50 75 100 125 150

Lepton-Pair PT (GeV/c)

"To

war

d"

Ch

arg

ed D

ensi

ty

Drell-Yan14 TeV

70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)

RDF Preliminarygenerator level

PY Tune DWT PY Tune DW

PY64 Tune P329 PY64 Tune S320

Z-Boson: “Towards” RegionZ-Boson: “Towards” Region

Data at 1.96 TeV on the density of charged particles, dN/dd, with pT > 0.5 GeV/c and || < 1 for “Z-Boson” events as a function of PT(Z) for the “toward” region from PYTHIA Tune AW, Tune DW, Tune S320, and Tune P329 at the particle level (i.e. generator level).

Z-BosonDirection

“Toward”

“Transverse” “Transverse”

“Away”

Z-BosonDirection

“Toward”

“Transverse” “Transverse”

“Away”

"Toward" Charged Particle Density: dN/dd

0.0

0.2

0.4

0.6

0.8

0 25 50 75 100 125 150

Lepton-Pair PT (GeV/c)

"To

war

d"

Ch

arg

ed D

ensi

ty

RDF Preliminarygenerator level

70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)

Drell-Yan1.96 TeVPY Tune DW PY Tune AW

PY64 Tune S320PY64 Tune P329

Tevatron LHC

Extrapolations of PYTHIA Tune AW, Tune DW, Tune DWT, Tune S320, and Tune P329 to the LHC.

RDF LHC Prediction!

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Workshop on Early LHC Physics May 6, 2009

Rick Field – Florida/CDF/CMS Page 35

Z-Boson: “Towards” RegionZ-Boson: “Towards” Region

Data at 1.96 TeV on the charged PTsum density, dPT/dd, with pT > 0.5 GeV/c and || < 1 for “Z-Boson” events as a function of PT(Z) for the “toward” region from PYTHIA Tune AW, Tune DW, Tune S320, and Tune P329 at the particle level (i.e. generator level).

Z-BosonDirection

“Toward”

“Transverse” “Transverse”

“Away”

Z-BosonDirection

“Toward”

“Transverse” “Transverse”

“Away”

Tevatron LHC

Extrapolations of PYTHIA Tune AW, Tune DW, Tune DWT, Tune S320, and Tune P329 to the LHC.

"Toward" Charged PTsum Density: dN/dd

0.0

0.2

0.4

0.6

0.8

1.0

0 25 50 75 100 125 150

Lepton-Pair PT (GeV/c)

"To

war

d"

PT

sum

Den

sity

RDF Preliminarygenerator level

Drell-Yan1.96 TeV

70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)

PY Tune DW

PY Tune AW

PY64 Tune S320

PY64 Tune P329

"Toward" Charged PTsum Density: dN/dd

0.0

0.4

0.8

1.2

1.6

2.0

0 25 50 75 100 125 150

Lepton-Pair PT (GeV/c)

"To

war

d"

PT

sum

Den

sity

RDF Preliminarygenerator level

Drell-Yan14 TeV

70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)

PY Tune DWT

PY Tune DW

PY64 Tune P329

PY64 Tune S320

RDF LHC Prediction!

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Workshop on Early LHC Physics May 6, 2009

Rick Field – Florida/CDF/CMS Page 36

LHC PredictionsLHC Predictions

Proton AntiProton

“Minumum Bias” Collisions

Proton AntiProton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

Proton AntiProton

Drell-Yan Production

Anti-Lepton

Lepton

Underlying Event Underlying Event

Charged Particle Density: dN/d

0.0

1.0

2.0

3.0

4.0

-8 -6 -4 -2 0 2 4 6 8

PseudoRapidity

Ch

arg

ed P

arti

cle

Den

sity

RDF Preliminarygenerator level

Charged Particles (PT>0.5 GeV/c) Min-Bias14 TeV

PY64 Tune P329

PY Tune A

PY64 Tune S320

"Transverse" Charged Particle Density: dN/dd

0.0

0.4

0.8

1.2

1.6

0 5 10 15 20 25

PTmax (GeV/c)

"Tra

ns

ve

rse

" C

ha

rge

d D

en

sit

y

PY Tune A

Min-Bias14 TeV Charged Particles (||<1.0, PT>0.5 GeV/c)

RDF Preliminarygenerator level

PY64 Tune P329

PY64 Tune S320 PY Tune DW

PY Tune DWT

"Toward" Charged Particle Density: dN/dd

0.0

0.4

0.8

1.2

1.6

0 25 50 75 100 125 150

Lepton-Pair PT (GeV/c)

"To

war

d"

Ch

arg

ed D

ensi

tyDrell-Yan

14 TeV

70 < M(pair) < 110 GeV

Charged Particles (||<1.0, PT>0.5 GeV/c)

RDF Preliminarygenerator level

PY Tune DWT PY Tune DW

PY64 Tune P329 PY64 Tune S320

The amount of activity in “min-bias” collisions.

I believe we are now in a position to make some predictions at the LHC!

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

Z-BosonDirection

“Toward”

“Transverse” “Transverse”

“Away”

The amount of activity in the “underlying event” in hard scattering events.

The amount of activity in the “underlying event” in Drell-Yan events.

If the LHC data are not in the range shown here then

we learn new physics!

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Workshop on Early LHC Physics May 6, 2009

Rick Field – Florida/CDF/CMS Page 37

Summary & ConclusionsSummary & Conclusions We are making good progress in understanding and modeling the

“underlying event”.

It is clear now that the default value PARP(90) = 0.16 is not correct and the value should be closer to the Tune A value of 0.25.

The new Pythia pT 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!

Proton AntiProton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

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!

All tunes with the default value PARP(90) = 0.16 are wrong and are overestimating the activity of min-bias and the underlying event at the LHC! This includes all the ATLAS tunes and all my “T” tunes!

UE&MB@CMSUE&MB@CMS

Hard-Scattering Cut-Off PT0

1

2

3

4

5

100 1,000 10,000 100,000

CM Energy W (GeV)

PT

0

(Ge

V/c

)

PYTHIA 6.206

= 0.16 (default)

= 0.25 (Set A))

However, I believe that the better fits to the LEP

fragmentation data at high z will lead to small improvements

of Tune A at the Tevatron!

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Workshop on Early LHC Physics May 6, 2009

Rick Field – Florida/CDF/CMS Page 38

Early LHC Thesis ProjectsEarly LHC Thesis Projects

Proton Proton

“Minumum Bias” Collisions

PTmax Direction

“Toward”

“Transverse” “Transverse”

“Away”

ChgJet#1 Direction

“Toward”

“Transverse” “Transverse”

“Away”

Thesis 1: Measure dNchg/d and <PT> versus Nchg in “min-bias” collisions.

Thesis 2: Measure the “toward”, “away”, and “transverse” region as a function of PTmax in “min-bias” collisions.

Thesis 3: Measure the “toward”, “away”, and “transverse” region as a function of PT(chgjet#1).

Thesis 4: Measure the “toward”, “away”, and “transverse” region as a function of PT(Z) for Z-boson production.

Thesis 5: Measure PT(Z) and <pT> versus Nchg for Z-boson production (all PT(Z), PT(Z) < 10 GeV/c).

Proton Proton

Drell-Yan Production

Anti-Lepton

Lepton

Underlying Event Underlying Event

Z-Boson Direction

“Toward”

“Transverse” “Transverse”

“Away”

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation