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Cracow School of Physics Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page 1 51 51 st st Cracow School of Theoretical Physics Cracow School of Theoretical Physics The Soft Side of the LHC The Soft Side of the LHC Rick Field University of Florida UE&MB@CMS UE&MB@CMS Lecture 2: Outline CMS ATLAS Zakopane, Poland, June 11-19, 2011 Min-Bias and the Underlying Event at the LHC How are “min-bias” collisions related to the “underlying event”. How well did we do at predicting the behavior of “min- bias” collisions at the LHC (900 GeV and 7 TeV)? Baryon and Strange Particle Production at the LHC: Fragmentation tuning. K + u s K - u s K short d s s d + p u u d Λ Λ Λ ud s Ξ Ξ Ξ - - - d s s

51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

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Page 1: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 1

5151stst Cracow School of Theoretical PhysicsCracow School of Theoretical PhysicsThe Soft Side of the LHCThe Soft Side of the LHC

Rick FieldUniversity of Florida

UE&MB@CMSUE&MB@CMS

Lecture 2: Outline

CMS

ATLAS

Zakopane, Poland, June 11-19, 2011

Min-Bias and the Underlying Event at the LHC

� How are “min-bias” collisions related to the “underlying event”.

� How well did we do at predicting the behavior of “min-bias” collisions at the LHC (900 GeV and 7 TeV)?

� Baryon and Strange Particle Production at the LHC:Fragmentation tuning.

K+

u s K -

u s

K short

d s s d +

p

u u d

ΛΛΛΛ

u d s

ΞΞΞΞ−−−−

d s s

Page 2: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 2

Toward an Understanding ofToward an Understanding ofHadronHadron--HadronHadron CollisionsCollisions

Rick FieldUniversity of Florida

From Feynman-Field to the LHC

Lecture 3: Tomorrow Evening

�The early days of Feynman-Field Phenomenology.

�Before Feynman-Field Phenomenology: The Berkeley years.

�From 7 GeV/cππππ0’s to 1 TeV Jets!

Feynman

Field

Page 3: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 3

ProtonProton--Proton CollisionsProton Collisions Elastic Scattering Single Diffraction

M

σσσσtot = σσσσEL + + + + σσσσSD++++σσσσDD++++σσσσHC

Double Diffraction

M 1 M 2

Proton Proton

“Soft” Hard Core (no hard scattering)

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event Initial-State Radiation

Final-State Radiation

“Hard” Hard Core (hard scattering)

Hard Core The “hard core” component

contains both “hard” and “soft” collisions.

“Inelastic Non-Diffractive Component”

ND

Page 4: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 4

The Inelastic NonThe Inelastic Non--Diffractive Diffractive CrossCross--SectionSection

Proton Proton

Proton Proton +

Proton Proton

Proton Proton

+

Proton Proton +

+ …

“Semi-hard” parton-parton collision(pT < ≈2 GeV/c)

Occasionally one of the parton-partoncollisions is hard(pT > ≈2 GeV/c)

Majority of “min-bias” events!

Multiple-partoninteractions (MPI)!

Page 5: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 5

The The ““ Underlying EventUnderlying Event””

Proton Proton

Select inelastic non-diffractive events that contain a hard scattering

Proton Proton

Proton Proton +

Proton Proton

+ + …

“Semi-hard” parton-parton collision(pT < ≈2 GeV/c)

Hard parton-partoncollisions is hard(pT > ≈2 GeV/c) The “underlying-event” (UE)!

Multiple-partoninteractions (MPI)!

Given that you have one hard scattering it is more probable to have MPI! Hence, the UE has more activity than “min-bias”.

1/(pT)4→ 1/(pT2+pT0

2)2

Page 6: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 6

Model of Model of σσσσσσσσNDND

Proton Proton

Proton Proton +

Proton Proton

Proton Proton

+

Proton Proton +

+ …

“Semi-hard” parton-parton collision(pT < ≈2 GeV/c)

Allow leading hard scattering to go to zero pT with same cut-off as the MPI!

Model of the inelastic non-diffractive cross section!

Multiple-partoninteractions (MPI)!

Proton Proton

1/(pT)4→ 1/(pT2+pT0

2)2

Page 7: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 7

UE TunesUE Tunes

Proton Proton

Proton Proton +

Proton Proton

Proton Proton

+

Proton Proton +

+ …

“Underlying Event”

“Min-Bias” (ND)

Fit the “underlying event” in a hard

scattering process.

Predict MB (ND)!

1/(pT)4→ 1/(pT2+pT0

2)2

Allow primary hard-scattering to go to pT = 0 with same cut-off!

Single Diffraction

M

Double Diffraction

M 1 M 2

“Min-Bias” (add single & double diffraction)

Predict MB (IN)!

Page 8: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 8

UE TunesUE Tunes

Proton Proton

Proton Proton +

Proton Proton

Proton Proton

+

Proton Proton +

+ …

“Underlying Event”

“Min-Bias” (ND)

Fit the “underlying event” in a hard

scattering process.

Predict MB (ND)!

1/(pT)4→ 1/(pT2+pT0

2)2

Allow primary hard-scattering to go to pT = 0 with same cut-off!

Single Diffraction

M

Double Diffraction

M 1 M 2

“Min-Bias” (add single & double diffraction)

Predict MB (IN)!

All of Rick’s tunes (except X2):A, AW, AWT,DW, DWT,

D6, D6T, CW, X1, and Tune Z1,are UE tunes!

Page 9: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 9

Charged Particle MultiplicityCharged Particle Multiplicity

� Data at 1.96 TeV on the charged particle multiplicity (pT > 0.4 GeV/c, |ηηηη| < 1) for “min-bias”collisions at CDF Run 2 (non-diffractive cross-section).

Charged Multiplicity Distribution

1.0E-08

1.0E-07

1.0E-06

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

0 5 10 15 20 25 30 35 40 45 50 55

Number of Charged Particles

Pro

bab

ility

CDF Run 2 <Nchg>=4.5

Normalized to 1

CDF Run 2 Preliminary

Min-Bias 1.96

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

i

Proton AntiProton

“Minimum Bias” Collisions

� The data are compared with PYTHIA Tune A and Tune A without multiple partoninteractions (pyAnoMPI ).

Charged Multiplicity Distribution

1.0E-08

1.0E-07

1.0E-06

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

0 5 10 15 20 25 30 35 40 45 50 55

Number of Charged Particles

Pro

bab

ility

CDF Run 2 <Nchg>=4.5

py Tune A <Nchg> = 4.3

pyAnoMPI <Nchg> = 2.6

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

CDF Run 2 Preliminary

Min-Bias 1.96 Normalized to 1

No MPI! Tune A!

Page 10: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 10

PYTHIA Tune A MinPYTHIA Tune A Min --BiasBias““ SoftSoft”” + + ”” HardHard ””

�Comparison of PYTHIA Tune A with the pT distribution of charged particles for “min-bias”collisions at CDF Run 1 (non-diffractive cross-section).

Charged Particle Density

1.0E-06

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

0 2 4 6 8 10 12 14

PT(charged) (GeV/c)

Ch

arg

ed D

ensi

ty d

N/d

ηη ηηdφφ φφd

PT

(1/

GeV

/c)

Pythia 6.206 Set A

CDF Min-Bias Data

CDF Preliminary

1.8 TeV |ηηηη|<1

PT(hard) > 0 GeV/c12% of “Min-Bias” events have PT(hard) > 5 GeV/c!

1% of “Min-Bias” events have PT(hard) > 10 GeV/c!

�PYTHIA Tune A predicts that 12% of all “Min-Bias” ev ents are a result of a hard 2-to-2 parton-parton scattering with PT(hard) > 5 GeV/c (1% with PT(hard) > 10 GeV/c)!

Lots of “hard” scattering in “Min-Bias” at the Tevatron!

Ten decades!

pT = 50 GeV/c!

Page 11: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 11

MB TunesMB Tunes

Proton Proton +

Proton Proton

Proton Proton

+

Proton Proton +

+ …

“Underlying Event”

“Min-Bias” (ND)

Predict the “underlying event” in a hard

scattering process!

Fit MB (ND).

Proton Proton

Page 12: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 12

MB TunesMB Tunes

Proton Proton +

Proton Proton

Proton Proton

+

Proton Proton +

+ …

“Underlying Event”

“Min-Bias” (ND)

Predict the “underlying event” in a hard

scattering process!

Fit MB (ND).

Proton Proton

Most of Peter Skand’s tunes:S320 Perugia 0, S325 Perugia X,

S326 Perugia 6are MB tunes!

Page 13: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 13

MB+UE TunesMB+UE Tunes

Proton Proton

Proton Proton +

Proton Proton

Proton Proton

+

Proton Proton +

+ …

“Underlying Event”

“Min-Bias” (ND)

Fit the “underlying event” in a hard

scattering process!

Fit MB (ND).

Most of Hendrik’s “Professor”tunes: ProQ20, P329

are MB+UE!

The ATLAS AMBT1 Tune is an MB+UE tune, butbecause they include in the fit the ATLAS UE data

with PTmax > 10 GeV/c (big errors) the LHC UE datadoes not have much pull (hence mostly an MB tune!).

Simultaneous fit to both MB & UE

Page 14: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 14

LHC MB Predictions: 900 LHC MB Predictions: 900 GeVGeV

Proton Proton

“Minimum Bias” Collisions

�Compares the 900 GeV ALICE data with PYTHIA Tune DW and Tune S320 Perugia 0. Tune DW uses the old Q2-ordered parton shower and the old MPI model. Tune S320 uses the new pT-ordered parton shower and the new MPI model. The numbers in parentheses are the average value of dN/dηηηη for the region |ηηηη| < 0.6.

Proton Proton

“Minimum Bias” Collisions

Charged Particle Density: dN/dηηηη

0

1

2

3

4

5

-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

ALICE INEL

UA5 INEL

pyDW INEL (2.67)

pyS320 INEL (2.70)

RDF Preliminary

INEL = HC+DD+SD 900 GeV

Charged Particles (all pT)

Charged Particle Density: dN/dηηηη

0

1

2

3

4

5

-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

UA5

ALICE

pyDW_10mm (3.04)

pyS320_10mm (3.09)

NSD = HC+DD 900 GeV

RDF Preliminary

Page 15: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 15

LHC MB Predictions: 900 LHC MB Predictions: 900 GeVGeV

Proton Proton

“Minimum Bias” Collisions

�Compares the 900 GeV ALICE data with PYTHIA Tune DW and Tune S320 Perugia 0. Tune DW uses the old Q2-ordered parton shower and the old MPI model. Tune S320 uses the new pT-ordered parton shower and the new MPI model. The numbers in parentheses are the average value of dN/dηηηη for the region |ηηηη| < 0.6.

Proton Proton

“Minimum Bias” Collisions

Charged Particle Density: dN/dηηηη

0

1

2

3

4

5

-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

ALICE INEL

UA5 INEL

pyDW INEL (2.67)

pyS320 INEL (2.70)

RDF Preliminary

INEL = HC+DD+SD 900 GeV

Charged Particles (all pT)

Charged Particle Density: dN/dηηηη

0

1

2

3

4

5

-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

UA5

ALICE

pyDW_10mm (3.04)

pyS320_10mm (3.09)

NSD = HC+DD 900 GeV

RDF Preliminary

Charged Particle Density: dN/dηηηη

0

1

2

3

4

5

-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

ALICE INELUA5 INELpyDW times 1.11 (2.97)pyS320 times 1.11 (3.00)

RDF Preliminary

INEL = HC+DD+SD 900 GeV

times 1.11

Charged Particles (all pT)

Off by 11%!

Page 16: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 16

ATLAS INEL ATLAS INEL dNdN/d/dηηηηηηηη

Soft particles!

� None of the tunes fit the ATLAS INEL dN/d ηηηηdata with PT > 100 MeV! They all predict too few particles.

� The ATLAS Tune AMBT1 was designed to fit the inelastic data for Nchg≥ 6 with pT > 0.5 GeV/c!

Off by 20-50%!

Page 17: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 17

Charged Particle Density: dN/dηηηη

0

2

4

6

8

-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

7 TeV

RDF PreliminaryCMS NSD data

pyDW generator level

dashed = ND solid = NSD

CMS CMS dNdN/d/dηηηηηηηη

�Generator level dN/dηηηη (all pT). Shows the NSD = HC + DD and the HC = ND contributions for Tune DW. Also shows the CMS NSD data.

CMS

Tune DW

All p T

Soft particles!

Proton Proton

“Minimum Bias” Collisions

Off by 50%!

Page 18: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 18

PYTHIA Tune DWPYTHIA Tune DWCharged Particle Density: dN/dηηηη

0

1

2

3

4

5

-2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

900 GeVpT > 0.15 GeV/c

RDF PreliminaryALICE INEL data

pyDW generator level

pT > 0.5 GeV/c

pT > 1.0 GeV/c

At Least 1 Charged Particle |ηηηη| < 0.8

� ALICE inelastic data at 900 GeV on the dN/dηηηη distribution for charged particles (pT > PTmin) for events with at least one charged particle with pT > PTmin and |ηηηη| < 0.8 for PTmin = 0.15 GeV/c, 0.5 GeV/c, and 1.0 GeV/c compared with PYTHIA Tune DW at the generator level.

If one increases the pTthe agreement

improves!

Tune DW

Proton Proton

“Minimum Bias” Collisions

Page 19: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 19

PYTHIA Tune DWPYTHIA Tune DW

� ALICE inelastic data at 900 GeV on the dN/dηηηη distribution for charged particles (pT > PTmin) for events with at least one charged particle with pT > PTmin and |ηηηη| < 0.8 for PTmin = 0.15 GeV/c, 0.5 GeV/c, and 1.0 GeV/c compared with PYTHIA Tune Z1 at the generator level (dashed = ND, solid = INEL).

Charged Particle Density: dN/dηηηη

0

1

2

3

4

5

-2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

900 GeVpT > 0.15 GeV/c

RDF PreliminaryALICE INEL data

pyDW generator level

pT > 0.5 GeV/c

pT > 1.0 GeV/c

dashed = ND solid = INEL

At Least 1 Charged Particle |ηηηη| < 0.8

Diffraction contributes less at

harder scales!

Tune DW

Proton Proton

“Minimum Bias” Collisions

Cannot trust PYTHIA 6.2 modeling of diffraction!

Page 20: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 20

MinMin --Bias CollisionsBias Collisions

� CMS NSD dataon the charged particle rapidity distribution at 7 TeV compared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit ηηηη, (1/NNSD) dN/dηηηη.

CMS

Proton Proton

“Minimum Bias” Collisions

Okay not perfect, but remember we know that SD and DD are not modeled well!

Charged Particle Density: dN/dηηηη

0

2

4

6

8

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

pyZ1 ND = dashedpyZ1 NSD = solid

CMS DataPYTHIA Tune Z1

NSD (all pT) 7 TeV

� ALICE NSD data on the charged particle rapidity distribution at 900 GeV compared with PYTHIA Tune Z1 . The plot shows the average number of particles per INEL collision per unit ηηηη, (1/NINEL ) dN/dηηηη.

Tune Z1

Charged Particle Density: dN/dηηηη

0

2

4

6

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

pyZ1 NSD = dashedpyZ1 INEL = solid

ALICE DataPYTHIA Tune Z1

INEL (all pT) 900 GeV

Tune Z1

ALICE

NSD = ND + DD

INEL = NSD + SD

Page 21: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 21

PYTHIA Tune Z1PYTHIA Tune Z1

� ALICE inelastic data at 900 GeV on the dN/dηηηη distribution for charged particles (pT > PTmin) for events with at least one charged particle with pT > PTmin and |ηηηη| < 0.8 for PTmin = 0.15 GeV/c, 0.5 GeV/c, and 1.0 GeV/c compared with PYTHIA Tune Z1 at the generator level.

Charged Particle Density: dN/dηηηη

0

1

2

3

4

5

-2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0

PseudoRapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

900 GeVpT > 0.15 GeV/c

RDF PreliminaryALICE INEL data

pyZ1 generator level

pT > 0.5 GeV/c

pT > 1.0 GeV/c

At Least 1 Charged Particle |ηηηη| < 0.8

Proton Proton

“Minumum Bias” Collisions

Okay not perfect, but remember we do not know if the SD & DD are correct!

Page 22: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 22

NSD Multiplicity DistributionNSD Multiplicity Distribution

�Generator level charged multiplicity distribution (all pT, |ηηηη| < 2) at 900 GeV and 7 TeV. Shows the NSD = HC + DD prediction for Tune Z1. Also shows the CMS NSD data.

Charged Multiplicity Distribution

1.0E-04

1.0E-03

1.0E-02

1.0E-01

0 20 40 60 80 100

Number of Charged Particles

Pro

bab

ility

Charged Particles (all PT, |ηηηη|<2.0)

RDF Preliminarydata CMS NSD

pyZ1 generator level

7 TeV

900 GeV

CMS

Tune Z1

Difficult to produce enough events with large multiplicity!

Proton Proton

“Minumum Bias” Collisions

Okay not perfect!But not that bad!

Page 23: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 23

MB versus UEMB versus UE

� CMS NSD dataon the charged particle rapidity distribution at 7 TeV compared with PYTHIA Tune Z1 . The plot shows the average number of charged particles per NSD collision per unit ηηηη, (1/NNSD) dN/dηηηη.

CMS

Proton Proton

“Minimum Bias” Collisions

Charged Particle Density: dN/dηηηη

0

2

4

6

8

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

pyZ1 ND = dashedpyZ1 NSD = solid

CMS DataPYTHIA Tune Z1

NSD (all pT) 7 TeV

Tune Z1

NSD = ND + DD

� CMS NSD dataon the charged particle rapidity distribution at 7 TeV compared with PYTHIA Tune Z1. The plot shows the average number of charged particles per NSD collision per unit ηηηη−−−−φφφφ, (1/NNSD) dN/dηηηηdφφφφ.

Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

pyZ1 ND = dashed

pyZ1 NSD = solid

CMS DataPYTHIA Tune Z1

NSD (all pT) 7 TeV

Divide be 2ππππ

Page 24: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 24

MB versus UEMB versus UE

Proton Proton

“Minimum Bias” Collisions

CMSTune Z1 NSD = ND + DD

� CMS NSD dataon the charged particle rapidity distribution at 7 TeV compared with PYTHIA Tune Z1. The plot shows the average number of charged particles per NSD collision per unit ηηηη−−−−φφφφ, (1/NNSD) dN/dηηηηdφφφφ.

Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

pyZ1 ND = dashed

pyZ1 NSD = solid

CMS DataPYTHIA Tune Z1

NSD (all pT) 7 TeV

Transverse Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25

PT max (GeV/c)

Ch

arg

ed P

arti

cle

Den

sity

7 TeV ND

Charged Particles (|ηηηη| < 2, all pT)

RDF PreliminaryPYTHIA Tune Z1

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� Shows the density of charged particles in the “transverse” region as a function of PTmax for charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Tune Z1

Factor of 2!

Page 25: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 25

MB versus UEMB versus UE

Proton Proton

“Minimum Bias” Collisions

CMSTune Z1 NSD = ND + DD

� CMS NSD dataon the charged particle rapidity distribution at 7 TeV compared with PYTHIA Tune Z1. The plot shows the average number of charged particles per NSD collision per unit ηηηη−−−−φφφφ, (1/NNSD) dN/dηηηηdφφφφ.

Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

pyZ1 ND = dashed

pyZ1 NSD = solid

CMS DataPYTHIA Tune Z1

NSD (all pT) 7 TeV

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� ATLAS data on the density of charged particles in the “transverse” region as a function of PTmax for charged particles (pT> 0.1 GeV/c, |ηηηη| < 2.5) at 7 TeV compared with PYTHIA Tune Z1.

Factor of 2!

"Transverse" Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

0 2 4 6 8 10 12 14 16 18 20

PTmax (GeV/c)

"Tra

nsv

erse

" C

har

ged

Den

sity

RDF PreliminaryATLAS corrected data

Tune Z1 generator level

7 TeV Charged Particles (pT > 0.1 GeV/c, |ηηηη|<2.5)

ATLAS

Page 26: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 26

Baryon & Strange Particle Baryon & Strange Particle Production at the LHCProduction at the LHC

� Strange Particle Production in Proton-Proton Collisions at 900 GeV with ALICE at the LHC, arXiv:1012.3257 [hep-ex] December 18, 2010.

� Production of Pions, Kaons and Protons in pp Collisions at 900 GeV with ALICE at the LHC, arXiv:1101.4110 [hep-ex] January 25, 2011.

� Strange Particle Production in pp Collisions at 900 GeV and 7 TeV, CMS Paper: arXiv:1102.4282 [hep-ex] Feb 21, 2011, submitted to JHEP.

Step 1:Look at the overall particle yields (all pT). K+

u s

K -

u s

K short

d s s d +

p

u u d

ΛΛΛΛ

u d s

ΞΞΞΞ−−−−

d s s

Step 2:Look at the ratios of the overall particle yields (all pT). (K++ K -)

(ππππ++ ππππ-) =

Strange Meson

Non-strange Meson

K short

(ππππ++ ππππ-) =

Strange Meson

Non-strange Meson (p + p)

(ππππ++ ππππ-) =

Non-strange Baryon

Non-strange Meson

(ΛΛΛΛ + ΛΛΛΛ)

2Kshort = Single-strange Baryon

Strange Meson

(ΞΞΞΞ + ΞΞΞΞ)

2Kshort = Double-strange Baryon

Strange Meson

Step 3:Look at the pT dependence of the particle yields and ratios.

I know there are more nice results

from the LHC, but this is all I can show

today. Sorry!

INEL

INEL

NSD

Page 27: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 27

KaonKaon ProductionProduction

� CMS NSD dataon the Kshort rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of Kshort per NSD collision per unit Y, (1/NNSD) dN/dY.

Kshort Rapidity Distribution: dN/dY

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT) Tune Z1

CMS

Kshort Rapidity Distribution: dN/dY

0.0

0.1

0.2

0.3

0.4

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY 900 GeV

CMS & ALICE DataPYTHIA Tune Z1

CMS NSD

ALICE INEL pyZ1 NSD = solid

pyZ1 INEL = dashed

� CMS NSD data on the Kshort rapidity distribution at 900 GeV and the ALICE point at Y = 0 (INEL) compared with PYTHIA Tune Z1. The ALICE point is the average number of Kshort per INEL collision per unit Y at Y = 0, (1/NINEL ) dN/dY.

Tune Z1

INEL = NSD + SD

Proton Proton

“Minimum Bias” Collisions

No overall shortage of Kaons in PYTHIA Tune Z1!

Page 28: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 28

KaonKaon ProductionProduction

� ALICE INEL data on the charged kaonrapidity distribution at 900 GeV compared with PYTHIA Tune Z1 . The plot shows the average number of charged kaons per INEL collision per unit Y at Y = 0, (1/NINEL ) dN/dY.

Proton Proton

“Minimum Bias” Collisions

Charged Kaons Rapidity: dN/dY

0.0

0.2

0.4

0.6

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

ALICE DataPYTHIA Tune Z1

INEL (all pT) 900 GeVpyZ1 NSD = dashedpyZ1 INEL = solid

(K++K-)

Rapidity Distribution Ratio: Kaons/Pions

0.0

0.1

0.2

0.3

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

ALICE DataPYTHIA Tune Z1

INEL (all pT) 900 GeV

(K++K-)/(ππππ++ππππ-)

� ALICE INEL data on the charged kaon to charged pion rapidity ratio at 900 GeVcompared with PYTHIA Tune Z1 .

ALICE ALICE

Tune Z1 Tune Z1

No overall shortage of Kaons in PYTHIA Tune Z1!

(K++ K-)

(ππππ++ ππππ-) =

Strange Meson

Non-strange Meson

Page 29: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 29

KaonKaon ProductionProduction

� ALICE INEL data on the charged kaonrapidity distribution at 900 GeV compared with PYTHIA Tune Z1 . The plot shows the average number of charged kaons per INEL collision per unit Y at Y = 0, (1/NINEL ) dN/dY.

Proton Proton

“Minimum Bias” Collisions

Charged Kaons Rapidity: dN/dY

0.0

0.2

0.4

0.6

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

ALICE DataPYTHIA Tune Z1

INEL (all pT) 900 GeVpyZ1 NSD = dashedpyZ1 INEL = solid

(K++K-)

Rapidity Distribution Ratio: Kaons/Pions

0.0

0.1

0.2

0.3

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

ALICE DataPYTHIA Tune Z1

INEL (all pT) 900 GeV

(K++K-)/(ππππ++ππππ-)

� ALICE INEL data on the charged kaon to charged pion rapidity ratio at 900 GeVcompared with PYTHIA Tune Z1 .

ALICE ALICE

Tune Z1 Tune Z1

Rapidity Distribution Ratio: Kshort/Kaons

0.0

0.2

0.4

0.6

0.8

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

ALICE DataPYTHIA Tune Z1

INEL (all pT) 900 GeV

Kshort/(K++K-)

No overall shortage of Kaons in PYTHIA Tune Z1!

(K++ K-)

(ππππ++ ππππ-) =

Strange Meson

Non-strange Meson

Page 30: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 30

KaonKaon ProductionProduction

� Rick’s plot of the CMS NSD dataon the K short rapidity distribution at 7 TeV and 900 GeV. The plot shows the average number of K short per NSD collision per unit Y, (1/NNSD) dN/dY, versus Y from -2 → 2.

CMS measures (1/NNSD) dN/dY

� Real CMS NSD dataon the Kshort rapidity distribution at 7 TeV and 900 GeV. The plot shows the average number of Kshort per NSD collision per unit Y, (1/NNSD) dN/dY, versus |Y| from 0 → 2.

Kshort Rapidity Distribution: dN/dY

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

versus |Y| from 0 → 2

I am old and I like to see both sides so I assumed symmetry about Y = 0 and plotted the same data on both sides (Y → -Y). The way CMS does it is the correct way!But my way helps me see better what is going on. Please refer to the CMS publication for the official plots!

Warning: I am not plotting what CMS actually measures!

This is the correct way!

I have plotted the same data twice!

Page 31: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 31

Lambda ProductionLambda Production

� CMS NSD dataon the Lambda+AntiLambdarapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

Proton Proton

“Minimum Bias” Collisions

(Lam+LamBar) Rapidity Distribution: dN/dY

0.00

0.05

0.10

0.15

0.20

0.25

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

(ΛΛΛΛ+ΛΛΛΛ)_

Rapidity Distribution Ratio: (Lam+LamBar)/(2Kshort)

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

CMS DataPYTHIA Tune Z1

7 TeV

NSD (all pT)

(ΛΛΛΛ+ΛΛΛΛ)/(2Kshort)_

CMS Tune Z1

� CMS NSD dataon the Lambda+AntiLambda to 2Kshort rapidity ratio at 7 TeV compared with PYTHIA Tune Z1 .

CMS

Tune Z1

Factor of 1.5!

Oops! Not enough Lambda’s in PYTHIA Tune Z1!

(ΛΛΛΛ + ΛΛΛΛ)

2Kshort = Single-strange Baryon

Strange Meson

Page 32: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 32

Cascade ProductionCascade Production

� CMS NSD dataon the Cascade-+AntiCascade-

rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

Proton Proton

“Minimum Bias” Collisions

(Cas+CasBar) Rapidity Distribution: dN/dY

0.00

0.01

0.02

0.03

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

Rapidity Distribution Ratio: (Cas+CasBar)/(2Kshort)

0.00

0.01

0.02

0.03

0.04

0.05

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

CMS DataPYTHIA Tune Z1

7 TeV

NSD (all pT)

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)/(2Kshort)_

CMS

Tune Z1

� CMS data on the Cascade-+AntiCascade- to 2Kshort rapidity ratio at 7 TeV compared with PYTHIA Tune Z1 .

CMS

Tune Z1

Factor of 2!

Yikes! Way too few Cascade’s in PYTHIA Tune Z1!

(ΞΞΞΞ + ΞΞΞΞ)

2Kshort = Double-strange Baryon

Strange Meson

Page 33: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 33

PYTHIA Fragmentation PYTHIA Fragmentation ParametersParameters

� PARJ(1) : (D = 0.10) is P(qq)/P(q), the suppression of diquark-antidiquark pair production in the colour field, compared with quark–antiquark production. Notation: PARJ(1) = qq/q

� PARJ(2) : (D = 0.30) is P(s)/P(u), the suppression of s quark pair production in the field compared with u or d pair production. Notation: PARJ(2) = s/u.

� PARJ(3) : (D = 0.4) is (P(us)/P(ud))/(P(s)/P(u)), the extra suppression of strange diquarkproduction compared with the normal suppression of strange quarks. Notation: PARJ(3) = us/u.

Can we increase the overall rate of strange baryons by varying a few fragmentation parameters?

This work is very preliminary!

Page 34: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 34

PYTHIA Fragmentation PYTHIA Fragmentation ParametersParameters

� PARJ(1) : (D = 0.10) is P(qq)/P(q), the suppression of diquark-antidiquark pair production in the colour field, compared with quark–antiquark production. Notation: PARJ(1) = qq/q

� PARJ(2) : (D = 0.30) is P(s)/P(u), the suppression of s quark pair production in the field compared with u or d pair production. Notation: PARJ(2) = s/u.

� PARJ(3) : (D = 0.4) is (P(us)/P(ud))/(P(s)/P(u)), the extra suppression of strange diquarkproduction compared with the normal suppression of strange quarks. Notation: PARJ(3) = us/u.

Can we increase the overall rate of strange baryons by varying a few fragmentation parameters?

This work is very preliminary!

Warning! This may cause problemsfitting the LEP data. If sowe must understand why!

We do not want one tune for e+e- and another one for

hadron-hadron collisions!

Page 35: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 35

PYTHIA Fragmentation PYTHIA Fragmentation ParametersParameters

� PYTHIA Tune Z1C : Same as Tune Z1 except qq/q is increased 0.1 → 0.12and us/s is increased from 0.4 → 0.8.

Rapidity Distribution Ratio: (Lam+LamBar)/(2Kshort)

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

CMS DataPYTHIA Tune Z1

7 TeVNSD (all pT) s/u: 0.3 -> 0.5

us/s: 0.4 -> 1.0

qq/q: 0.1 -> 0.2

Z1 default

(ΛΛΛΛ+ΛΛΛΛ)/(2Kshort)_

Rapidity Distribution Ratio: (Cas+CasBar)/(2Kshort)

0.00

0.01

0.02

0.03

0.04

0.05

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

CMS DataPYTHIA Tune Z1

7 TeVNSD (all pT)

s/u: 0.3 -> 0.5

us/s: 0.4 -> 1.0qq/q: 0.1 -> 0.2

Z1 default

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)/(2Kshort)_

Rapidity Distribution Ratio: Kaons/Pions

0.0

0.1

0.2

0.3

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

ALICE DataPYTHIA Tune Z1

INEL (all pT) 900 GeV

(K++K-)/(ππππ++ππππ-)s/u: 0.3 -> 0.5

us/s: 0.4 -> 1.0

qq/q: 0.1 -> 0.2Z1 default

Page 36: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 36

KaonKaon ProductionProduction

� CMS NSD dataon the Kshort rapidity distribution at 7 TeV and 900 GeV compared with PYTHIA Tune Z1 . The plot shows the average number of Kshort per NSD collision per unit Y, (1/NNSD) dN/dY.

Kshort Rapidity Distribution: dN/dY

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT) Tune Z1CMS

Kshort Rapidity Distribution: dN/dY

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

Ch

arg

ed P

arti

cle

Rat

io

CMS DataPYTHIA Tune Z1C

900 GeV

7 TeV

NSD (all pT)

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

� CMS dNSD ataon the Kshort rapidity distribution at 7 TeV and 900 GeV compared with PYTHIA Tune Z1C . The plot shows the average number of Kshort per NSD collision per unit Y, (1/NNSD) dN/dY.

Tune Z1CCMS

Proton Proton

“Minimum Bias” Collisions

For Kaon production Tune Z1 and Z1C are almost identical!

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Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 37

KaonKaon ProductionProduction

� CMS NSD dataon the Kshort rapidity distribution at 7 TeV and 900 GeV compared with PYTHIA Tune Z1 . The plot shows the average number of Kshort per NSD collision per unit Y, (1/NNSD) dN/dY.

Kshort Rapidity Distribution: dN/dY

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT) Tune Z1CMS

Kshort Rapidity Distribution: dN/dY

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

Ch

arg

ed P

arti

cle

Rat

io

CMS DataPYTHIA Tune Z1C

900 GeV

7 TeV

NSD (all pT)

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

� CMS dNSD ataon the Kshort rapidity distribution at 7 TeV and 900 GeV compared with PYTHIA Tune Z1C . The plot shows the average number of Kshort per NSD collision per unit Y, (1/NNSD) dN/dY.

Tune Z1CCMS

Rapidity Distribution Ratio: Kaons/Pions

0.0

0.1

0.2

0.3

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

ALICE DataPYTHIA Tune Z1 & Z1C

INEL (all pT) 900 GeV

(K++K-)/(ππππ++ππππ-)

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

Proton Proton

“Minimum Bias” Collisions

For Kaon production Tune Z1 and Z1C are almost identical!

Page 38: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 38

Lambda ProductionLambda Production

� CMS NSD dataon the Lambda+AntiLambdarapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

(Lam+LamBar) Rapidity Distribution: dN/dY

0.00

0.05

0.10

0.15

0.20

0.25

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

(ΛΛΛΛ+ΛΛΛΛ)_

(Lam+LamBar) Rapidity Distribution: dN/dY

0.00

0.05

0.10

0.15

0.20

0.25

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

Ch

arg

ed P

arti

cle

Rat

io

CMS DataPYTHIA Tune Z1C

900 GeV

7 TeV

NSD (all pT)

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΛΛΛΛ+ΛΛΛΛ)_

� CMS NSD dataon the Lambda+AntiLambdarapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

CMS Tune Z1

CMS

Tune Z1C

Proton Proton

“Minimum Bias” Collisions

Not bad! Many more Lambda’s in PYTHIA Tune Z1C!

Page 39: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 39

Lambda ProductionLambda Production

� CMS NSD dataon the Lambda+AntiLambdarapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

(Lam+LamBar) Rapidity Distribution: dN/dY

0.00

0.05

0.10

0.15

0.20

0.25

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

(ΛΛΛΛ+ΛΛΛΛ)_

(Lam+LamBar) Rapidity Distribution: dN/dY

0.00

0.05

0.10

0.15

0.20

0.25

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

Ch

arg

ed P

arti

cle

Rat

io

CMS DataPYTHIA Tune Z1C

900 GeV

7 TeV

NSD (all pT)

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΛΛΛΛ+ΛΛΛΛ)_

� CMS NSD dataon the Lambda+AntiLambdarapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

CMS Tune Z1

CMS

Tune Z1C

Rapidity Distribution Ratio: (Lam+LamBar)/(2Kshort)

0.0

0.1

0.2

0.3

0.4

0.5

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

CMS DataPYTHIA Tune Z1 & Z1C

7 TeV

NSD (all pT)

(ΛΛΛΛ+ΛΛΛΛ)/(2Kshort)_

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

Proton Proton

“Minimum Bias” Collisions

Not bad! Many more Lambda’s in PYTHIA Tune Z1C!

Page 40: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 40

Cascade ProductionCascade Production

� CMS NSD dataon the Cascade-+AntiCascade-rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

(Cas+CasBar) Rapidity Distribution: dN/dY

0.00

0.01

0.02

0.03

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

(Cas+CasBar) Rapidity Distribution: dN/dY

0.00

0.01

0.02

0.03

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

Ch

arg

ed P

arti

cle

Rat

io

CMS DataPYTHIA Tune Z1C

900 GeV

7 TeV

NSD (all pT)

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

CMS

Tune Z1

CMS

Tune Z1C

� CMS NSD dataon the Cascade-+AntiCascade-rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

Proton Proton

“Minimum Bias” Collisions

Wow! PYTHIA Tune Z1C looks very nice here!

Page 41: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 41

Cascade ProductionCascade Production

� CMS NSD dataon the Cascade-+AntiCascade-rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

(Cas+CasBar) Rapidity Distribution: dN/dY

0.00

0.01

0.02

0.03

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

(Cas+CasBar) Rapidity Distribution: dN/dY

0.00

0.01

0.02

0.03

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

Ch

arg

ed P

arti

cle

Rat

io

CMS DataPYTHIA Tune Z1C

900 GeV

7 TeV

NSD (all pT)

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

CMS

Tune Z1

CMS

Tune Z1C

Rapidity Distribution Ratio: (Cas+CasBar)/(2Kshort)

0.00

0.01

0.02

0.03

0.04

0.05

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

7 TeV

NSD (all pT)

CMS DataPYTHIA Tune Z1 & Z1C

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)/(2Kshort)_

� CMS NSD dataon the Cascade-+AntiCascade-rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

Proton Proton

“Minimum Bias” Collisions

Wow! PYTHIA Tune Z1C looks very nice here!

Page 42: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 42

Cascade ProductionCascade Production

� CMS NSD dataon the Cascade-+AntiCascade-rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

(Cas+CasBar) Rapidity Distribution: dN/dY

0.00

0.01

0.02

0.03

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

CMS DataPYTHIA Tune Z1

900 GeV

7 TeV

NSD (all pT)

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

(Cas+CasBar) Rapidity Distribution: dN/dY

0.00

0.01

0.02

0.03

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

Ch

arg

ed P

arti

cle

Rat

io

CMS DataPYTHIA Tune Z1C

900 GeV

7 TeV

NSD (all pT)

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

CMS

Tune Z1

CMS

Tune Z1C

Rapidity Distribution Ratio: (Cas+CasBar)/(2Kshort)

0.00

0.01

0.02

0.03

0.04

0.05

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

7 TeV

NSD (all pT)

CMS DataPYTHIA Tune Z1 & Z1C

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)/(2Kshort)_

� CMS NSD dataon the Cascade-+AntiCascade-rapidity distribution at 7 TeV and 900 GeVcompared with PYTHIA Tune Z1 . The plot shows the average number of particles per NSD collision per unit Y, (1/NNSD) dN/dY.

Rapidity Ratio: (Cas+CasBar)/(Lam+LamBar)

0.00

0.05

0.10

0.15

0.20

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

7 TeV

NSD (all pT)

CMS DataPYTHIA Tune Z1 & Z1C

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)/(ΛΛΛΛ+ΛΛΛΛ)_ _

Proton Proton

“Minimum Bias” Collisions

Wow! PYTHIA Tune Z1C looks very nice here!

Page 43: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 43

Transverse Momentum Transverse Momentum DistributionsDistributions

� CMS NSD dataon the Kshort transverse momentum distribution at 7 TeV compared with PYTHIA Tune Z1 & Z1C . The plot shows the average number of particles per NSD collision per unit pT, (1/NNSD) dN/dpTfor |Y| < 2.

PT Distribution: Kshort

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

1.0E+01

0 1 2 3 4 5 6 7 8 9 10

PT (GeV/c)

dN

/dP

T (

1/G

eV/c

)

CMS DataPYTHIA Tune Z1 & Z1C

NSD (|Y| < 2)) Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

7 TeV

PT Distribution: Lam+LamBar

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

0 1 2 3 4 5 6 7 8 9 10

PT (GeV/c)

dN

/dP

T (

GeV

/c)

CMS DataPYTHIA Tune Z1 & Z1C

NSD (|Y| < 2))

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

7 TeV

(ΛΛΛΛ+ΛΛΛΛ)_

� CMS NSD dataon the Lambda+AntiLambdatransverse momentum distribution at 7 TeVcompared with PYTHIA Tune Z1 & Z1C . The plot shows the average number of particles per NSD collision per unit pT, (1/NNSD) dN/dpT for |Y| < 2.

Proton Proton

“Minimum Bias” Collisions

PYTHIA Tune Z1 & Z1C are a bit off on the pT dependence!

Page 44: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 44

Transverse Momentum Transverse Momentum DistributionsDistributions

PT Distribution: Cas+CasBar

1.0E-04

1.0E-03

1.0E-02

1.0E-01

0 1 2 3 4 5 6 7

PT (GeV/c)

dN

/dP

T (

1/G

eV/c

)

CMS DataPYTHIA Tune Z1 & Z1C

NSD (|Y| < 2))

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

7 TeV

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

Cas+CasBar PT Distribution: dN/dPT

1.0E-03

1.0E-02

1.0E-01

1.0E+00

0 1 2 3 4 5 6 7

PT (GeV/c)

Pro

bab

ility

CMS DataPYTHIA Tune Z1 & Z1C

NSD (|Y| < 2))

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

7 TeV

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

Normalized to 1

� CMS NSD dataon the Cascade-+AntiCascade-

transverse momentum distribution at 7 TeVcompared with PYTHIA Tune Z1 & Z1C . The plot shows the average number of particles per NSD collision per unit pT, (1/NNSD) dN/dpT for |Y| < 2.

� CMS NSD dataon the Cascade-+AntiCascade-

transverse momentum distribution at 7 TeV(normalized to 1) compared with PYTHIA Tune Z1 & Z1C.

Proton Proton

“Minimum Bias” Collisions

PYTHIA Tune Z1 & Z1C are a bit off on the pT dependence!

Page 45: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 45

Particle Ratios versus PTParticle Ratios versus PT

Proton Proton

“Minimum Bias” Collisions

(ΛΛΛΛ + ΛΛΛΛ)

2Kshort = Single-strange Baryon

Strange Meson

PT Particle Ratio: (Lam+LamBar)/(2Kshort)

0.0

0.2

0.4

0.6

0.8

0 1 2 3 4 5 6 7 8 9 10

PT (GeV/c)

PT

Par

ticl

e R

atio

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

7 TeVNSD (|Y| < 2)

CMS DataPYTHIA Tune Z1 & Z1C (ΛΛΛΛ+ΛΛΛΛ)/(2Kshort)

_

Particle Ratio: (Lam+LamBar)/(2Kshort)

0.0

0.2

0.4

0.6

0.8

0 1 2 3 4 5 6

PT (GeV/c)

Rat

io

ALICE DataPYTHIA Tune Z1 & Z1C

INEL (|Y| < 0.75) 900 GeV

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(ΛΛΛΛ+ΛΛΛΛ)/(2Kshort)_

� CMS NSD dataon the Lambda+AntiLambdato 2Kshort ratio versus pT at 7 TeV (|Y| < 2) compared with PYTHIA Tune Z1 & Z1C .

� ALICE INEL data on the Lambda+AntiLambdato 2Kshort ratio versus pT at 900 GeV (|Y| < 0.75) compared with PYTHIA Tune Z1 & Z1C .

Tune Z1C is not too bad but a bit off on the pT dependence!

(ΛΛΛΛ + ΛΛΛΛ)

2Kshort = Single-strange Baryon

Strange Meson

Page 46: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 46

Particle Ratios versus PTParticle Ratios versus PT

Proton Proton

“Minimum Bias” Collisions

PT Particle Ratio: (Cas+CasBar)/(2Kshort)

0.00

0.05

0.10

0.15

0 1 2 3 4 5 6 7 8

PT (GeV/c)

PT

Par

ticl

e R

atio

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.87 TeVNSD (|Y| < 2)

CMS DataPYTHIA Tune Z1 & Z1C

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)/(2Kshort)_

PT Particle Ratio: (Cas+CasBar)/(Lam+LamBar)

0.00

0.05

0.10

0.15

0.20

0.25

0.30

0 1 2 3 4 5 6 7 8

PT (GeV/c)

PT

Par

ticl

e R

atio

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.87 TeVNSD (|Y| < 2)

CMS DataPYTHIA Tune Z1 & Z1C (ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)/(ΛΛΛΛ+ΛΛΛΛ)

_ _

� CMS NSD dataon the Cascade-+AntiCascade-

to 2Kshort ratio versus pT at 7 TeV (|Y| < 2) compared with PYTHIA Tune Z1 & Z1C .

� CMS NSD dataon the Cascade-+AntiCascade-

to Lambda+AntiLambda ratio versus pT at 7 TeV (|Y| < 2) compared with PYTHIA Tune Z1 & Z1C .

Tune Z1C is not too bad but a bit off on the pT dependence!

(ΞΞΞΞ + ΞΞΞΞ)

2Kshort = Double-strange Baryon

Strange Meson

(ΞΞΞΞ + ΞΞΞΞ) =

Double-strange Baryon

Single-strange Baryon (ΛΛΛΛ + ΛΛΛΛ)

Page 47: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 47

Particle Ratios versus PTParticle Ratios versus PT

Proton Proton

“Minimum Bias” Collisions

PT Particle Ratio: Kaons/Pions

0.00

0.20

0.40

0.60

0 1 2 3 4

PT (GeV/c)

PT

Par

ticl

e R

atio

(K++K-)/(ππππ++ππππ-)ALICE Data

PYTHIA Tune Z1 & Z1C

INEL (|Y| < 0.75) 900 GeV

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

Rapidity Distribution Ratio: Kaons/Pions

0.0

0.1

0.2

0.3

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

ALICE DataPYTHIA Tune Z1 & Z1C

INEL (all pT) 900 GeV

(K++K-)/(ππππ++ππππ-)

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

� ALICE INEL data on the charged kaon to charged pion rapidity ratio at 900 GeVcompared with PYTHIA Tune Z1 .

� ALICE INEL data on the charged kaons to charged pions ratio versus pT at 900 GeV (|Y| < 0.75) compared with PYTHIA Tune Z1 & Z1C .

Tune Z1C is not too bad but a way off on the pT dependence!

(K++ K-)

(ππππ++ ππππ-) =

Strange Meson

Non-strange Meson

Tails of the pT distribution. Way off due to the wrong pT!

Page 48: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 48

Particle Ratios versus PTParticle Ratios versus PT

Proton Proton

“Minimum Bias” Collisions

PT Particle Ratio: (P+Pbar)/Pions

0.0

0.1

0.2

0.3

0.4

0 1 2 3 4

PT (GeV/c)

PT

Par

ticl

e R

atio

ALICE DataPYTHIA Tune Z1 & Z1C

INEL (|Y| < 0.75) 900 GeV

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

(p+p)/(ππππ++ππππ-)_

Rapidity Distribution Ratio: (P+Pbar)/Pions

0.00

0.03

0.06

0.09

0.12

-4 -3 -2 -1 0 1 2 3 4

Rapidity Y

dN

/dY

Par

ticl

e R

atio

INEL (all pT) 900 GeV

(p+p)/(ππππ++ππππ-)_ALICE Data

PYTHIA Tune Z1 & Z1C

Z1

Z1C

Tune Z1Cqq/q: 0.1 -> 0.12us/s: 0.4 -> 0.8

� ALICE INEL data on the Proton+AntiProton to charged pions ratio versus pT at 900 GeV (|Y| < 0.75) compared with PYTHIA Tune Z1 & Z1C .

� ALICE INEL data on the Proton+AntiProtonto charged pion rapidity ratio at 900 GeVcompared with PYTHIA Tune Z1 & Z1C .

Tune Z1C is not too bad but way off on the pT dependence!

(p + p)

(ππππ++ ππππ-) =

Non-strange Baryon

Non-strange Meson

Tails of the pT distribution. Way off due to the wrong pT!

Page 49: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 49

MB versus UEMB versus UE

Proton Proton

“Minimum Bias” Collisions

CMSTune Z1 NSD = ND + DD

� CMS NSD dataon the charged particle rapidity distribution at 7 TeV compared with PYTHIA Tune Z1. The plot shows the average number of charged particles per NSD collision per unit ηηηη−−−−φφφφ, (1/NNSD) dN/dηηηηdφφφφ.

Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

pyZ1 ND = dashed

pyZ1 NSD = solid

CMS DataPYTHIA Tune Z1

NSD (all pT) 7 TeV

Transverse Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25

PT max (GeV/c)

Ch

arg

ed P

arti

cle

Den

sity

7 TeV ND

Charged Particles (|ηηηη| < 2, all pT)

RDF PreliminaryPYTHIA Tune Z1

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� Shows the density of charged particles in the “transverse” region as a function of PTmax for charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Tune Z1

Factor of 2!

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Rick Field – Florida/CDF/CMS Page 50

UE Particle TypeUE Particle Type

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

Transverse Charged Particle Density: dN/dηηηηdφφφφ

0.0

0.5

1.0

1.5

2.0

2.5

0 5 10 15 20 25

PT max (GeV/c)

Ch

arg

ed P

arti

cle

Den

sity

7 TeV ND

Charged Particles (|ηηηη| < 2, all pT)

RDF PreliminaryPYTHIA Tune Z1

� Shows the density of charged particles in the “transverse” region as a function of PTmax for charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Tune Z1

Transverse Particle Density: dN/dηηηηdφφφφ

0.001

0.010

0.100

1.000

10.000

0 5 10 15 20 25

PTmax (GeV/c)

Par

ticl

e D

ensi

ty

charged particles7 TeV ND

(|ηηηη| < 2, all pT)

RDF PreliminaryPYTHIA Tune Z1

(ΛΛΛΛ+ΛΛΛΛ)

_(p+p)_

(ΞΞΞΞ−−−−+ΞΞΞΞ−−−−)_

(K++K-)

(ππππ++ππππ-)

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� Shows the density of particles in the “transverse” region as a function of PTmaxfor charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Log Scale!

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Rick Field – Florida/CDF/CMS Page 51

Charged Particle Density: dN/dηηηηdφφφφ

0.00

0.05

0.10

0.15

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

7 TeV ND

Kshort (all pT)

RDF PreliminaryPYTHIA Tune Z1

Kshort

"Transverse" Particle Density: dN/dηηηηdφφφφ

0.00

0.05

0.10

0.15

0 5 10 15 20 25

PT max (GeV/c)

Par

ticl

e D

ensi

ty

7 TeV ND

Kshort (|ηηηη| < 2, all pT)

RDF PreliminaryPYTHIA Tune Z1

Kshort

MB versus UEMB versus UE

Proton Proton

“Minimum Bias” Collisions

Tune Z1

� Shows the Kshort pseudo-rapidity distribution (all pT) at 7 TeV from PYTHIA Tune Z1. The plot shows the average number of particles per ND collision per unit ηηηη−−−−φφφφ, (1/NND) dN/dηηηηdφφφφ.

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� Shows the density of Kshort particles in the “transverse” region as a function of PTmaxfor charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Tune Z1

Factor of ~2!

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Rick Field – Florida/CDF/CMS Page 52

"Transverse" Particle Density: dN/dηηηηdφφφφ

0.00

0.04

0.08

0.12

0 5 10 15 20 25

PT max (GeV/c)

Par

ticl

e D

ensi

ty

(p+p)_

7 TeV ND (|ηηηη| < 2,all pT)

RDF PreliminaryPYTHIA Tune Z1

Charged Particle Density: dN/dηηηηdφφφφ

0.00

0.04

0.08

0.12

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

7 TeV ND (all pT)

RDF PreliminaryPYTHIA Tune Z1 (p+p)

_

MB versus UEMB versus UE

Proton Proton

“Minimum Bias” Collisions

Tune Z1

� Shows the P+antiP pseudo-rapidity distribution (all pT) at 7 TeV from PYTHIA Tune Z1. The plot shows the average number of particles per ND collision per unit ηηηη−−−−φφφφ, (1/NND) dN/dηηηηdφφφφ.

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� Shows the density of P+antiP particles in the “transverse” region as a function of PTmax for charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Tune Z1

Factor of ~2!

Page 53: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 53

"Transverse" Particle Density: dN/dηηηηdφφφφ

0.00

0.01

0.02

0.03

0.04

0 5 10 15 20 25

PT max (GeV/c)

Par

ticl

e D

ensi

ty

7 TeV ND (|ηηηη| < 2,all pT)

RDF PreliminaryPYTHIA Tune Z1

(ΛΛΛΛ+ΛΛΛΛ)_

Charged Particle Density: dN/dηηηηdφφφφ

0.00

0.01

0.02

0.03

0.04

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

7 TeV ND (all pT)

RDF PreliminaryPYTHIA Tune Z1 (ΛΛΛΛ+ΛΛΛΛ)

_

MB versus UEMB versus UE

Proton Proton

“Minimum Bias” Collisions

Tune Z1

� Shows the ΛΛΛΛ+antiΛΛΛΛ pseudo-rapidity distribution (all pT) at 7 TeV from PYTHIA Tune Z1. The plot shows the average number of particles per ND collision per unit ηηηη−−−−φφφφ, (1/NND) dN/dηηηηdφφφφ.

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� Shows the density of ΛΛΛΛ+antiΛΛΛΛ particles in the “transverse” region as a function of PTmax for charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Tune Z1

Factor of ~2!

Page 54: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

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Rick Field – Florida/CDF/CMS Page 54

"Transverse" Particle Density: dN/dηηηηdφφφφ

0.00

0.01

0.02

0.03

0.04

0 5 10 15 20 25

PT max (GeV/c)

Par

ticl

e D

ensi

ty

7 TeV ND (|ηηηη| < 2,all pT)

RDF PreliminaryPYTHIA Tune Z1

(ΛΛΛΛ+ΛΛΛΛ)_

Charged Particle Density: dN/dηηηηdφφφφ

0.00

0.01

0.02

0.03

0.04

-4 -3 -2 -1 0 1 2 3 4

Pseudo-Rapidity ηηηη

Ch

arg

ed P

arti

cle

Den

sity

7 TeV ND (all pT)

RDF PreliminaryPYTHIA Tune Z1 (ΛΛΛΛ+ΛΛΛΛ)

_

MB versus UEMB versus UE

Proton Proton

“Minimum Bias” Collisions

Tune Z1

� Shows the ΛΛΛΛ+antiΛΛΛΛ pseudo-rapidity distribution (all pT) at 7 TeV from PYTHIA Tune Z1. The plot shows the average number of particles per ND collision per unit ηηηη−−−−φφφφ, (1/NND) dN/dηηηηdφφφφ.

Proton Proton

PT(hard)

Outgoing Parton

Outgoing Parton

Underlying Event Underlying Event

Initial-State Radiation

Final-State Radiation

� Shows the density of ΛΛΛΛ+antiΛΛΛΛ particles in the “transverse” region as a function of PTmax for charged particles (All pT, |ηηηη| < 2) at 7 TeV from PYTHIA Tune Z1.

Tune Z1

Factor of ~2!

Coming soon!Measurements from CMS,ATLAS, and ALICE on the strange

particles and baryons in the “underlying event”.

Page 55: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

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Rick Field – Florida/CDF/CMS Page 55

Fragmentation SummaryFragmentation Summary�Not too hard to get the overall yields of

baryons and strange particles roughly right at 900 GeV and 7 TeV. Tune Z1C does a fairly good job with the overall particle yields at 900 GeV and 7 TeV.

�PT Distributions: PYTHIA does not describe correctly the pT distributions of heavy particles (MC softer than the data). None of the fragmentation parameters I have looked at changes the pT distributions. Hence, if one looks at particle ratios at large pT you can see big discrepancies between data and MC (out in the tails of the distributions)!

�ATLAS Tuning Effort: Fragmentation flavor tuning at the one of the four stages.

Proton Proton

“Minimum Bias” Collisions

K+

u s

K -

u s

K short

d s s d + p

u u d

ΛΛΛΛ

u d s

ΞΞΞΞ−−−−

d s s

�Other Fragmentation Tuning: There is additional tuning involving jet shapes, FSR, and ISR that I did not have time to include in this talk.

Page 56: 51 Cracow School of Theoretical PhysicsCracow School of ...rfield/cdf/Zakopane2_RickField_6-13-11.pdf · 6/13/2011  · Zakopane, June 13, 2011 Rick Field – Florida/CDF/CMS Page

Cracow School of Physics Zakopane, June 13, 2011

Rick Field – Florida/CDF/CMS Page 56

Fragmentation SummaryFragmentation Summary�Not too hard to get the overall yields of

baryons and strange particles roughly right at 900 GeV and 7 TeV. Tune Z1C does a fairly good job with the overall particle yields at 900 GeV and 7 TeV.

�PT Distributions: PYTHIA does not describe correctly the pT distributions of heavy particles (MC softer than the data). None of the fragmentation parameters I have looked at changes the pT distributions. Hence, if one looks at particle ratios at large pT you can see big discrepancies between data and MC (out in the tails of the distributions)!

�ATLAS Tuning Effort: Fragmentation flavor tuning at the one of the four stages.

Proton Proton

“Minimum Bias” Collisions

K+

u s

K -

u s

K short

d s s d + p

u u d

ΛΛΛΛ

u d s

ΞΞΞΞ−−−−

d s s

�Other Fragmentation Tuning: There is additional tuning involving jet shapes, FSR, and ISR that I did not have time to include in this talk.

Warning! The Tune Z1C fragmentationparameters may cause problems

fitting the LEP data. If sowe must understand why!

We do not want one tune for e+e- and another one for

hadron-hadron collisions!