NuPECC Annual Meeting Athens, 8 October, 2010 Apostolos D. Panagiotou CMS/Athens – CASTOR group
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Transcript of NuPECC Annual Meeting Athens, 8 October, 2010 Apostolos D. Panagiotou CMS/Athens – CASTOR group
Searching for Deconfined Quark-Matter in HI collisions at the CERN LHC with CMS/CASTOR
NuPECC Annual Meeting Athens, 8 October, 2010
Apostolos D. PanagiotouCMS/Athens – CASTOR group
Heavy Ion Physics at the LHC with CMS
Central region
Forward region
30%
5.5 TeV
Energy & Particle Pseudorapidity Distributions
Net Baryon Number Pb+Pb @ 2.8 TeV
All of Net Baryon Number in forward region High Baryochemical Potential Lower temperature
A
(Strangelet ?)
3.6 λI
3.2 λI
3.6 λI
1.5 λI Hadron limit
Hadron limit
What is a “Strangelet” ?
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“Stable” Strangelet interaction in CASTORMC-algorithm
Strangelet is considered with radius:
Mean interaction path:
Strangelets passing through the detector collide with W nuclei: Spectator part is continuing its passage. Wounded part produces particles in a standard way.
Particles produced in successive interactions initiate electromagnetic-nuclear cascades. Process ends when strangelet is destroyed.E. Farhi, R. Jaffe, Phys.Rev.D30(1984)2379; M. Berger, R. Jaffe, Phys.Rev.C 35(1987)213, G.Wilky, Z.Wlodarczyk, J.Phys.G22(1996)L105; E. Gładysz, Z. Włodarczyk, J.Phys.G23(1997)2057
31
23223s
str310
mμμπ2a12
A3πArR
231str0
31W
NWWstr
ArA1.12πmAλ
nstrstr NAA'
The rescaled r0 is determined by the number density of the strange matter: n = A/V = (1/3)(nu+nd+ns)where ni=- ∂Ωi/∂μi; Ω(mi,μi,αs), taking into account the QCD corrections O(αs) to the properties of SQM.
ss s
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31
23223s
str310
mμμπ2a12
A3πArR
231
str031
W
NWWstr
ArA1.12πmAλ
Scaled Radius & Mean Free Path of Strangelets vr μq
Collapsed nucleus
λWπ ~ 7 cm
quark quark
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MC simulation of Strangelets in CASTOR
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1. Sector with much higher energy than the average: Strong azimuthal asymmetry in energy deposition
2. Strong penetration of the longitudinal cascade in a sector:Strong fluctuations in longitudinal transition curves
3. Much smaller EEM / EHAD compared to HIJING
4. Appearing in a very low multiplicity event compared to HIJING
Characteristics of a “LFC” Event
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CMS/CASTOR Calorimeter
Front View
Side View
LFC Signatures
Azimuthal asymmetryin energy deposition
Fluctuations longitudinaltransition curves
sd
iE
EE
Event-by-event analysis in 3 steps:
average distribution energy distribution per RU
Large magnitude of energyfluctuations in RUs manifestin abnormal transition curves
L. F. C. Identification Analysis
(i = 1 – 16 sectors)<E> = mean energy in sectors
nsfluctuatio
σsd = standard deviation of the distribution of the energies Ei
Examine Ratio EEM / EHAD of events
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3
2
Analysis (Ι)“LFC signature” Azimouthal Energy
distribution
Cascade Energy distribution
- Event-by-event- Sector-by-sector(Central Pb+Pb collisions, b=0)
Analysis (Ι)“Strangelet
signature”Azimouthal Energy
distribution
Cascade Energy distribution
- Event-by-event- Sector-by-sector(central Pb+Pb collisions, b=0)
Select φ-sector containing LFC
Fluctuations on the (fa,fl) plane
Statistical fluctuations of HIJING events with similar characteristics Strangelets with higher energies are separated from conventional HIJING
events Distinction of conventional events with similar fluctuations
EEM/EHD
HIJING(2k events)
StrangeletsE=6-15 TeV
Analysis (ΙI)
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Analysis (ΙII)
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Analysis (ΙII)
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• Probability for a hadron-rich ‘Centauro-type’ event is about 3%, estimated from statistics of Chacaltaya and Pamir experiments for cosmic ray families with visible energy greater than 100 TeV.• In about 10% of hadron-rich events, strongly penetrating cascades, clusters, or “halo” were observed. Assume total probability for “Long Flying Component” (LFC) production in central nucleus-nucleus collisions to be approximately: 0.03 x 0.1 ~ O(10−3).• At LHC kinematics, the percent of LFCs in CASTOR phase space is at least ~ 1% of total number of LFCs produced in central Pb-Pb collisions, depending on their mass and energy (CENGEN). • An order of magnitude estimation of the total probability for LFC detection in CASTOR is:
PCASTORLFC ≈ 10−3 × 0.01 ≈ O(10−5)
Cross Section Estimation for LFC
ΝLFC ~ 1-10 in 4 wks Pb+Pb (5M central events in 2010)