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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
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
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
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)!
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
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
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)!
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!
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!
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!
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
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!
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
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
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%!
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%!
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%!
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
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!
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
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!
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!
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
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!
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
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
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!
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
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
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!
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
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
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!
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!
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
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!
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!
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!
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!
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!
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!
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!
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!
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!
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
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)
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!
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!
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!
Cracow School of Physics Zakopane, June 13, 2011
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!
Cracow School of Physics Zakopane, June 13, 2011
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!
Cracow School of Physics Zakopane, June 13, 2011
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!
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!
Cracow School of Physics Zakopane, June 13, 2011
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”.
Cracow School of Physics Zakopane, June 13, 2011
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.
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!