Strangeness analysis in ALICE
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Transcript of Strangeness analysis in ALICE
Strangeness analysis in ALICE
o genuine p+p physicso PbPb physicso analysis status, studies in PPR2o prospects
K0s and hyperons
Ludovic Gaudichet, INFN TorinoVietri sul Mare 30/05/2006
p+p analysis
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Ludovic Gaudichet INFN, Torino 3
p+p collisions at LHC
Yields and pt spectra at mid-rapidity of K0s, Λ, Ξ and Ω and their anti-particles
Baryon asymmetry :Is the baryon number carried by gluons also ? (comparison to gluonic baryon junction models) Particle production mechanisms, in soft / intermediate / hard regimesBeside gluons, u and d, strange quark is the only component of low pt multiparticle interaction which is statistically significant
- comparison with pythia, HERWIG, ...- minimum bias / underlying events- Λ/Λbar and jets
Feed-down corrections : needed to determine yield of proton ! Comparison to thermal models, interesting by itself and will serve heavy ion analysis Baseline for the analysis of heavy ion collisions
2A
p+p analysis
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“day one” analysis
Provided that we understand our detector, we could publish : K0
s yield and spectrum at mid-rapidity Rough yields of Λ and Λbar
130 Λ
Already interesting for constraining pythia and understanding baryons production mechanisms
Estimation with pythia 6.2 and ATLAS tuning.Could be more !
104 events
p+p analysis
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Results of first run 7.107 events (200h at 100Hz)
K0s yield and spectrum at mid-rapidity
Λ and Λbar yields and pt spectra up to pt = 8 GeV/c Ξ and Ξbar yields and pt spectra up to pt = 4 GeV/c 190 Omegas ... or hopefully more !
926k Λ 19k Ξ
p+p analysis
PbPb analysis
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Strangeness enhancement
Tounsi et al.
PbPb analysis
B. Hippolyte,Moriond 2004
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Strangeness enhancement
J. Rafelski
Statistical Equilibrium / non-equilibrium ?Difficult to know at RHIC, but big difference at LHC :
However :• Hard processes will compete with soft processes. 2 sources of strangeness, one equivalent to p+p !
• In p+p an increase of the volume could also gives some more phase space for strangeness production !
• Canonical to Grand Canonical transition still have to be there !?
• Scaling with Nbin ?
PbPb analysis
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Intermediate transverse momentum
between soft (hydrodynamics) and hard (pQCD) regimes 2-3 GeV/c and 6-7 GeV/c at RHIC
Little known, between collective effects and hard scatteringa lot to learn about hadronisation and its dynamics
What :
Why :
PbPb analysis
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Intermediate pt PbPb analysis
Constituent quark scaling :
P.R. Sorensen QM05 talk
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Rcp in heavy ion collisionsperipheral 2 centralbinary T
CP central 2 peripheralbinary T
N /
N /
d N dp dyR
d N dp dy
PbPb analysis
K0s and hyperons in
ALICE
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2nd vertex reconstruction
K0s -
DCA to primary vertex
Daughter DCA
Angle between V0 momentum and primary vertex
-
V0 cuts, selecting Λ
Bachelor DCA to primary vertex
DCA V0-Bachelor
4 parameters 5 parameters
Angle between cascade momentum and primary vertex
+ vertex radius +
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Performance of topology reconstructionin PPR2 : p+p collisions
Even without charged track PID !No limit in pt other than statistic !
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Effect of event multiplicityIn p+p collisions the reconstruction rate is a function of the multiplicity :
Small dependence from the primary vertex resolution + pt hardening of hyperon spectra
in PPR2 : p+p collisions
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Reconstruction factors & raw spectra 109 eventsin PPR2 : p+p collisions
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Reconstruction in PbPb collisions
Λ
Ξ
Ω
in PPR2 : PbPb collisions
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Raw spectra in PbPb at 5.5 TeVin PPR2 : PbPb collisions
Λ
Ξ
Ω
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Signal selection by the LDA
LDANeural netClassical cuts
LDA is :Faster than anything else, more reliable than neural networks Significance increases by 20% Amount of selected signal increases by 60%
Λ Ξ
Linear Discriminant Analysis+ succession of cuts in the n-dim space of parameters
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Conclusion Hadron production at LHC energy Baseline for the analysis of heavy ion collisions
Soft physics : thermal production, hydrodynamics a perfect fluid at LHC ? Strangeness is a good probe
Intermediate transverse momentum : key regime for the understanding of the collision dynamics large portion of produced particle at LHC striking advantage of Strangeness
Analysis of K0s and hyperons tested in p+p and PbPb collisions
Strange objects (V0 and cascades) available for any analysis like tracks Room for improvement : Linear Discriminant Analysis Next Data Challenge on the way : preparing analysis of p+p ! Analysis code within the PWG2 of ALICE : to be discussed ...
p+p
PbPb
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Backup slides
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To do next : Physics Data Challenge 06Lacks in PPR2 : systematic from the primary vertex resolution
full study of Omega reconstruction efficiency
What PDC 06 will provide :
• 108 events• More realistic simulations
• calibration (dead channels, mis-alignment, ...)• Trigger simulation
Ξ reconstruction rate, scaled by the difference seen in PbPb
Last Data Challenge : test of the analysis speed and the CPU requirement !
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Event cocktail for PDC 06PDC 06
Minimum bias events, as defined by pythia 6.2, ATLAS tuning Events enriched with Ω and Ωbar
Have enough statistic Compensate for pythia possible underestimation of strangeness75000 enriched events with Ω, 75000 with Ωbar
STAR
UA5
SPS
Pythia6.36.2
bar
√s
dN/dy (-0.5<y<0.5)
K0s
SPS
CDF
STAR
UA5
Pythia
6.36.2
√s
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Event cocktail for PDC 06PDC 06
Minimum bias events, as defined by pythia 6.2, ATLAS tuning Events enriched with Ω and Ωbar
Have enough statistic Compensate for pythia possible underestimation of strangeness75000 enriched events with Ω, 75000 with Ωbar
SPS
RHIC
Pythia
6.2
6.3
√s
K0s, Λ and Ξ estimation are
acceptable, but Ω
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Baryon excess : Λ/K0s
• Low pt limit can be define by the validity range of Hydro.
• At high pt limit, the baryon and meson should merge again.
• BUT seen in p+p too ! (UA1 & CDF)
PbPb analysis
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Λ/K0s in pythia
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<pT> versus mass in p+p at RHIC
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thermal particle production
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RAA in heavy ion collisions
We can also do RAA
Several effects here :• shadowing at low pt• Cronin effect • strangeness enhancement• jet quenching
H. Caines, STAR
PbPb analysis
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Azimuthal correlation at high pT