trd technology at alice matthias hartig johann-wolfgang goethe universität frankfurt/main
TRANSCRIPT
TRD Technology at ALICE
Matthias Hartig
Johann-Wolfgang Goethe Universität
Frankfurt/Main
Overview
ALICE Experiment
ALICE TRD
Chamber Design
Front End Electronic
Performance
TRD Overview
HERMES TRD
NOMAD TRD
AMS TRD
Summary / Outlook
Large Hadron Collider
Genf
Mont Blanc
CERN
ALICE Experiment
PHOS,0
MUON -pairs PMD
multiplicity
ITSVertexingLow pt tracking
TPCTracking, PID
TRDElectron ID
TOFPID
HMPIDPID (RICH) @ high pt
EMCAL (not shown)Jet-calorimetry
FMD, V0, T0, ZDC (not shown)Trigger,multiplicity,centrality
The ALICE Experiment
ALICE Experiment
Requirements
Robust tracking performance
Needs to digest highest multiplicities (O(105) tracks !)
Need to cover low pt region (~100 MeV/c )
Soft physics important for event characterization
But the high pt region as well (>100 GeV/c )
Hard probes transmit information about early phase
Good PID capabilities over large pt-range essential
Many effects are flavour dependent
Sensitivity to rare probes
Heavy flavour, quarkonia, photons, ...
ALICE Experiment
PID Capabilities
(relativistic rise)
TPC: (dE/dx) = 5.5(pp) – 6.5(Pb-Pb) %TOF: < 100 psTRD: suppression 10-2 @ 90% e-efficiency
Transition Radiation Detector
Transition Radiation
Produced by fast charged particles
crossing the boundary between
materials with different dielectrical
constants
production probability ~ 1/ per
boundary
Characteristic:
energy spectrum in keV region
angel of emission ~1/
Spectrum determined by:
number and distance of the surfaces
thickness and plasmafrequence of the
material
Velocity of the charged particle
()
Radiator:
Regular foils
Fibre material
Foam
Measured spectrumof 2 GeV/c electrons
Transition Radiation Detector
Schematic View
Radiator:• irregular structure - Polypropylen fibers - Rohacel foam (frame)• 4.8 cm thick• self supporting
Gas:• Xe/CO2 85/15 %
Drift region:• 3 cm length• 700 V/cm• 75 m CuBe wires
Amplification region:• W-Au-plated wires 25 m• gain ~ 10000
Readout:• cathode pads• 8 mm (bending plane)• 70 mm in z/beam-direction• 10 MHz
Transition Radiation Detector
Design
Large area chambers (1-1,7 m²)
-> need high rigidity
Low rad. length (15%Xo)
-> low Z, low mass material
Transition Radiation Detector
Setup
TRD in Numbers:
540 Chambers
6 Layers
18 Sectors
(Supermodule)
Total Area: 736 m2
Gasvolume: 27,2 m3
Auflösung (r) 400 m
Number of Readout
Channels:
1,2 Millionen
TRD Supermodul
TPC
TRD SupermoduleTOF supermodule
Electron Identification Performance
Result of Test Beam Data
LQ Method:
Likelihood with total charge
LQX Method:
total charge + position of max. cluster
Typical signal of single particle
PID with neural network
e/-discrimination < 10-2
For 90% e-efficiency
Front End Electronic
Overview
Readout Board (ROB)Readout Board (ROB)•8 (6) ROBs per chamber•7 different ROBs•16+1 MCM per Board•Readout of 18 channels per MCM
2 x Optical Readout Interfaces
Detector ControlSystem
Front End Electronic
Readout Board / Multi-chip Module
120cm 160cmAnalog part (PASA):• Preamplifier/shaper• Convrsion gain 12.4 mV/fC• Shaping time 120 ns (FWHM)• Equivalent noise ~700 e
Digital Part (TRAP):• ADC• Preprocessor, digital filters• Hit selection• Tracklet processing at 120 MHz
• 260 000 CPUs working in parallel during readout
• Measured Noise on the chamber ~1200 e
Front End Electronic
Detector Control System
160cm
1 DCS board per chamber:
• FPGA and ARM core running Linux OS
• Control of voltage regulators
• MCM configuration
• Clock and trigger distribution
• Also used for other detectors
Front End Electronic
Optical Readout Interface
120cm 160cm
2 ORI boards per chamber:
• Connects 4 (3) ROBs to GTU
• High speed readout: 2.5 GBit optical link
TRD Trigger
Online Tracking
Trigger Requirements:• electron and electron pairs• with high pt (> 2GeV/c)
Challenges:• tracking of all charge particles • time budget of 6.1 s
Local Tracking Unit (LTU)• on each chamber• linear tracklets fit• ship tracklets to GTU
Global Tracking Unit (GTU)• find high momentum tracks through all 6 layers• generate trigger
Offline TRD Tracking
Standalone Track Resolution
Cluster reconstruction:• charge sharing between pads• pad response function• tail cancellation• TR absorption
Track positionTrack angel
In bending plane:• Hit resolution < 400 mm (for each time bin)• Angular resolution < 1 deg. (for each plane)
Track angular resolution: < 0.4 deg.
dNch/dy = 6000
Offline Tracking Performance
Efficiency and Resolution for Pb+Pb
Efficiency:• high software track-finding efficiency• lower combined track efficiency (geometrical acceptance, particle decay )• Efficiency independent of track multiplicity
Momentum resolution:• long lever arm ITS + TPC +TRD (4cm <r<370cm)• resolution better for low multiplicity (p+p)• pt/pt 5 % at 100 GeV/c and B = 0.5 T
HERMES TRD
Lepton Scattering Experiment
• DIS measurement at 27 GeV at HERA• electron identification:
• TRD, preshower, calorimeter• (RICH,TOF)
HERMES TRD
Lepton Scattering Experiment
• Aktive area 0.75 x 3.25 m2 • 2 x 6 modules• Irregular radiator
• polypropylen fibers• 6.35 cm thick
• Readout• MWPC• flexible windows• Gaps to keep MWPC thickness• 90/10 % Xe/CH4
Result:• dismantled 2007• PRF > 102 for > 2 GeV/c• more than 10 years successful operation
NOMAD TRD
Neutrino Oscillation Experiment
• Appearance of
Xe- +
• Background from e in neutrino beam• Total pion rejection > 105 at 90% electron efficienty at 1-50 GeV/c • TRD 103, preshower, EM calorimeter• End of operation 1999
• Aktive Area 2.85 x 2.85 m2 • 9 modules• Regular radiator
• 315 polypropylen foils• 15 m thick• 250 m space
• Readout• 176 straw tubes• 3 m long• 16 mm diameter• 80/20 % Xe/CH4
AMS TRD
Antimatter Search in the Universe
• Space based Detector• AMS 1: space shuttle• AMS 2: 3 y on the ISS
• 6 modules • Irregular radiator
• polypropylen fibers• 2.00 cm thick
•80/20 % Xe/CH4
Summary / Outlook
Summary
ALICE TRD chambers 80 %
ready
FEE Integration / SM production
30 % ready
MCM configuration needs fine
tuning
4 SM installed
At least 3 successful TRDs
TRD powerful tool to identify
electrons from 1 – 100 GeV/c
Outlook
Gas detector for TR
measurement ?
Slow
Xe is expensive
Xe difficult to get
New development of radiator
material ?