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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. Panagiotou CMS/Athens – CASTOR group. Heavy Ion Physics at the LHC with CMS. Central region. Forward region.

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NuPECC Annual Meeting Athens, 8 October, 2010 Apostolos D. Panagiotou CMS/Athens – CASTOR group

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  1. Searching for Deconfined Quark-Matter in HI collisions at the CERN LHC with CMS/CASTOR NuPECC Annual Meeting Athens, 8 October, 2010 Apostolos D. Panagiotou CMS/Athens – CASTOR group

  2. Heavy Ion Physics at the LHC with CMS Central region Forward region

  3. Energy & Particle Pseudorapidity Distributions 5.5 TeV 30% Net Baryon Number Pb+Pb @ 2.8 TeV All of Net Baryon Number in forward region  High Baryochemical Potential  Lower temperature

  4. A

  5. (Strangelet ?) 1.5 λI Hadron limit 3.6 λI 3.6 λI 3.2 λI Hadron limit

  6. What is a “Strangelet” ?

  7. “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 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. s s s 10

  8. Scaled Radius & Mean Free Path of Strangelets vr μq  λWπ ~ 7 cm  Collapsed nucleus quark quark 11

  9. MC simulation of Strangelets in CASTOR 12

  10. Characteristics of a “LFC” Event • 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 • Much smaller EEM / EHAD compared to HIJING • 4. Appearing in a very low multiplicity event compared to HIJING 13

  11. CMS/CASTOR Calorimeter Side View Front View 14 14 14

  12. LFC Signatures Azimuthal asymmetry in energy deposition Fluctuations longitudinal transition curves energy distribution per RU average distribution Large magnitude of energy fluctuations in RUs manifest in abnormal transition curves L. F. C. Identification Analysis • Event-by-event analysis in 3 steps: σsd = standard deviation of the distribution of the energies Ei <E> = mean energy in sectors (i = 1 – 16 sectors) 1 2 3 Examine Ratio EEM / EHAD of events

  13. Analysis (Ι) “LFC signature” Azimouthal Energy distribution Cascade Energy distribution - Event-by-event - Sector-by-sector (Central Pb+Pb collisions, b=0)

  14. 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

  15. Analysis (ΙI) Fluctuations on the (fa,fl) plane Strangelets E=6-15 TeV HIJING (2k events)‏ • 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

  16. Analysis (ΙII) 19

  17. Analysis (ΙII) 20

  18. Cross Section Estimation for LFC • 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) ΝLFC ~ 1-10 in 4 wks Pb+Pb (5M central events in 2010) 21

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