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Explore the high-tech experiments and setups on cosmic calibration and charged particle triggers by EMC SuperModule. Dive deep into VHMPiD R&D status and discover the advanced technologies being tested at Yale Physics Department. Uncover the intricate details of the Triple GEM Detector and its role in detecting high Pt charged particles. Learn about the latest developments and simulations in particle physics research, including innovative detector responses and efficient track detection methods.
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EMC SuperModule Cosmic Calibration, VHMPiD R&D status, and A High Pt Charged Particle Trigger. N. Smirnov Physics Department, Yale University, Oct, 06. ALICE-USA collaboration meeting at Yale U.
EMC SM cosmic calibration; possible set-up. • We need a simple set-up to select a “single MIP through a tower” • Must be: compact, easy to move ( many strips), reliable (low rate). ~ 10 cm ~ 0.1 s-1 rate ~10000 tracks / 24 hours / Module ~ 1 Month / SuperModule
One EMC Module ( top view ) Triple GEM Detector (“active” surface ) 10 cm 12 cm 4 read-out pads to cover each tower 10 cm 12 cm Possible Set-up 4 Scintillation Counters ( ~ 75x14 cm2 ) 4 + 2 x { 12 x 4 } = 100 Read-out channels / EMC strip 10 cm 12 triple GEM detectors with pad read-out
Triple GEM Detector • Simple in construction ( NO: strong frame, wires, high precision parts ) • Reliable (discharge-free, but high gain in “all” gas mixtures ) • Efficient as a track detector 98% mip efficiency, ~20 ns response COMPASS experience • R&D, test and “production” Lab at Yale “Tech-Etch” (MA) mass-production ~ 1 cm One EMC Module ( top view ) Triple GEM Detector (“active” surface ) 10 cm 12 cm 4 read-out pads to cover each tower It needs: 2 x 12 x 3 = 72 GEM foils 2 x 12 x 4 = 96 FEE channels 10 cm 12 cm
VHMPiD R&D and Simulation Status • Group inside of ALICE ( >10 people) • CERN, Hungary, Italy, Mexico, USA (Yale U, BNL(?)) first HI collision ? start of LHC yesterday HMPID 3σ p/K limit HMPID TDR ALICE Club - May 2, 2005 Paolo Martinengo
GEANT Simulation Double sided Read-out plane Triple GEM foils with CsI UV Mirror, spherical shape in ZY AeroGel, 10cm 50 cm CF4 gas Detector response: GEANT hits(π+, Pt~10. GeV/c; local coordinate system, cm) Y 50 cm UV photoelectrons from “CF4 + Mirror” side C4F10 gas X Z R position: ~450 cm. Bz: 0.5 T CaF2 Window Particle track & UV photons MIP For all materials; n, transmission, absorption, reflection, Qw.Eff, - F(E = 5.5 – 11. eV) UV photoelectrons from “C4F10 + Window” side
Simulation for high Pt π+ Flat mirror Spherical mirror AeroGel, 10cm UV Mirror, spherical shape in ZY Double sided Read-out plane Triple GEM foils with CsI CF4 gas CaF2 Window C4F10 gas R Z In saturation: <N ph.e.> 25. (C4F10); 30. (CF4)
Detector response: GEANT hits(π+, Pt~10. GeV/c; local coordinate system, cm) UV photoelectrons from CF4 + Mirror MIP z x UV photoelectrons from C4F10 + Window
PiD table • Radiators: thickness L, refractive index n, angle θc, UV-light threshold AeroGel C4F10 CF4 L 10 50 50 cm n 1.008 1.0014 1.0005 θc ~100. 53. 32. mrad π 1.2 2.6 4.4 GeV/c K 4.2 9.3 15.6 GeV/c p 8.3 19.5 31.3 GeV/c P, GeV/c π/μ/e K p 5. – 9.3 ArG Y YN Ch1 YN N Ch2 YN N 9.3 - 15.6 ArG Y Y Y Ch1 Y Y N Ch2 YN N 15.6 – 20. ArG Y Y Y Ch1 Y Y N Ch2 Y Y N >20. ArG Y Y Y Ch1 Y Y Y Ch2 Y YN UV photoelectrons ring for CF4 + Mirror,Circle Fit, Nhits > 5. R, cm π K π/K PiD – ring radius P, GeV/c
~ 2m ALICE Club - May 2, 2005 Paolo Martinengo
One detector response on “standard central ALICE event”. X - MIP position - Track “reflection” from mirror; “circle center” - Photo-electrons from “bottom” gas UV light + window. Red circle – track has hits in TPC - Photo-electrons from “top” gas UV light + mirror green means Sc. Light from CF4
GEANT Simulation, ALICE set-up VBHC Realistic material budget and position for: Si Vertex, TPC*, TRD, ToF + 100 modules of HMPiD (100 x 100 x 100 cm3 ) GEM D. AeroGel, 10cm UV Mirror, spherical shape in ZY CF4 gas Double sided Read-out plane Triple GEM foils with CsI CaF2 Window C4F10 gas *For TPC all “read-out” stuff is as realistic as possible to simulate dE/dX performance GEM D. 30 x 30 cm2 COMPAS read-out strip structure R Z
High Pt trigger using “fast” tracking data (?!) “R2D” Does not need primary Vertex position Sigma (cm): 0.02 0.2 0.02 0.9 “ALICE” Needs primary Vertex with ~n cm resolution ~1 m ToF hit R fit, DCA to Vertex in XY SLFtoBLine Straight Line Fit in RZ “Z” DCA to Vertex cut ~4 m Y Y SLDtoV X X
Track finding and selection for HMPiD only(plus Primary Vertex) SLDtoV, cm With cuts selected: (~ > 6. GeV/c ) I. 32 π+ /event; Pt = (8. – 10.) GeV/c 80% efficiency II. 32 π+ & Central PbPb HJ event ( ~ 2200 particles / rapidity) 70% efficiency (the SAME tracks that were found in step I ) III. “Standard Central ALICE” event ( ~ 8000 particles / rapidity ) 1 track was found, Pt = 5.6 GeV/c Pt, GeV/c This “high Pt trigger approach” can be checked / tested with “available” equipments and in reasonable short period of time
ALICE TPC: 159 pad-rows; 63x (0.75x0.4) + 64x(1.x0.6) + 32x(1.5x0.6)Ne+CO2 (10%), B=0.5 T, Dl = Dt = 220 μm/cm-1Drift <= 250 cm. Vdr = 2.84 cm/μs (88 μs max) Simulation approach:N inter./cm; N el. / cluster; For each e- : (Ekin, range, Drift, wire position, timing, gas amplification, charge on pads); FEE shaping and noise; Hit position and Q reconstruction. dE/dX dE/dX Cluster efficiency – 85%, Truncated – 60% π, K, p P, Gev/c P, Gev/c “Perfect” in simulation: gas amplification calibration, P – reconstruction, one particle / event, |η| < 0.9; No “tail subtraction” problem; FADC approach.