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Low-Mass Drift Chambers for HADES

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The experimental approach: Spectroscopy of rare vector mesons ... toroid (0.7T) 2p in f, 18o J 85o. Tracking system. High acceptance ( 40% for pairs) ... – PowerPoint PPT presentation

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Title: Low-Mass Drift Chambers for HADES


1
Low-Mass Drift Chambers for HADES
C. Müntz, GSI Darmstadt
  • HADES High Acceptance Di-Electron Spectrometer
  • The major physics goal Properties of hadrons in
    hot and dense nuclear matter
  • The experimental approach Spectroscopy of rare
    vector mesons produced in heavy ion collisions
    via their decay in penetrating electron-positron
    pairs
  • Outline
  • Design constraints for the HADES tracking system
  • Choice of materials
  • The HADES planar Drift chambers
  • In-beam performance

C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
2
Present HADES Setup _at_ GSI
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
3
HADES The Heavy Ion Case
Simulation Central 1 AGeV AuAu reaction, all
(200) charged particles per event
Hadron-blind RICH
Electron pair from w decay
  • projected in-spill rates Hz 108 projectiles,
    106 reactions (1 target), 105 central reactions
  • rare r,w vector mesons branching production
    cross section 0.5 Hz
  • Electrons from conversion and p0 decay
    combinatorial background

C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
4
Hades Gross Properties
  • Electron ID
  • RICH
  • META Shower / ToF
  • ? Efficient selective
  • multi-stage trigger
  • Momentum measurement
  • Magnet, 6 coils
  • Supercond. toroid (0.7T)
  • 2p in f, 18o lt J lt 85o
  • Tracking system
  • High acceptance
  • ( 40 for pairs)
  • High invariant mass resolution
  • (ca. 1 in the r mass region)
  • This translates in
  • Maximum efficiency for MIPs
  • High resolution tracking
  • (intrinsic spatial cell resolution lt 140 mm)
  • Use of low-mass materials to minimize multiple
    scattering (x/X0 ? 5 ?10-4)

C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
5
Low-Mass Materials
  • Drift chamber gas
  • Balancing between
  • Low multiple scattering
  • Spatial resolution (dE/dx, vD uniformity)
  • Stability (gain, plateau)
  • Aging
  • Lorentz angle (B lt 0.05 T)
  • Physics-driven choice
  • Helium fill gas, avalanche
  • Isobutane primary ionization, quencher
  • He i-C4H10 6040
  • gain 510 ?105
  • vD 34.3 cm/ms
  • Wires
  • Balancing between
  • Low mass occupancy
  • Stability (self-sustained currents / Malter)
  • Tension loss (creeping, load on frames)
  • Our choice
  • Sense wires 20 / 30 mm Au/W)
  • Cathode, Field wires
  • 80 / 100 mm annealed Aluminum )
  • (I-III bare Al, IV gold-plated Al)

Other low-mass DCs CLEO, KLOE, FINUDA, BELLE,
CLAS, BaBar
) LUMA ) California fine wire
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
6
Long-Term Stability Aging

C.Garabatos
  • Accelerated aging
  • with X-rays (55Fe)
  • 2 prototypes

Io 6 nA/cm
  • Expected charge dose in HADES 10 mC/year/cm
  • No significant gain degradation (lt5) within an
    equivalent of 2 years running

C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
7
Long-Term Stability Creep of Al Wires
  • Bare Aluminum wires
  • (annealed)
  • systematic wire tension loss measurements
  • HADES MDC
  • 80 (100) mm
  • Low pre-tension 80 (100) cN

J.Hehner/H.Daues DL GSI
Measured tension loss 10 in 5 years
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
8
MDC Cross Properties
  • Gross properties
  • Active areas 0.35 3.2 m2
  • Gas vol. 15-260 l, flow 10-20 V/day
  • Cell Size 5x5 14x10 mm2
  • 6 Stereo angles 40, -20, 0,-0,20, -40
    deg., kick angle optimized, cathode wires at 90
    deg.
  • Max. occupancy 30 (8 average), 0.6 hits per
    cm
  • Materials
  • Sense wire 20/30mm Au/W
  • Cathode, Field wires 80/100 mm Al
  • Windows 12 mm Al-Mylar
  • Narrow Aluminum frames, 0.5 t load
  • Operating gas He-iC4H10 60-40

Publications Optimisation of low-mass drift
chambers for HADES, Nucl. Instr. Methods A 412
(1998) 38 Development of low-mass drift chambers
for the HADES spectrometer, Nucl. Instr. Methods
A 477 (2002) 387
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
9
Cell Properties
Drift velocity topology (MDC I)
Operating voltages Cathode/field -1.75 -2.3
kV Sense ground
MAGBOLZ / Garfield simulations
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
10
Comparison to Simulations
Drift time spectra
x-t correlation
Good agreement! ? Improvement of calibration
tracking algorithms
Intrinsic spatial resolution (proton beam, MDC
prototype, Silicon strip tracker)
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
11
Present MDC Setup
GSI plane I
ORSAY plane IV
Installed (5/2002) 17 out of 24 MDCs
  • In-beam experiences
  • Several commissioning and first
  • production runs,
  • CC, CrAl, 1-2 AGeV incident energy,
  • Moderate intensities
  • several 106 projectiles/spill

C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
12
Front-End Electronics
  • Analog Daughter Boards
  • Differential amplifier discriminator (ASD8
    chip)
  • 8 channels, 1 fC intr. noise,
  • 30 mW / channel,
  • adjustable threshold
  • (Straw Tubes, M.Newcomer, IEEE Trans. on Nucl.
    Sc. 40 (1993))

Signals from Sense wire
td
Dt
  • TDC Features
  • semi-customized ASIC
  • 8 ch., 0.5 ps/ch, common-stop, 1 ms full range
  • Multi-hit cap. (leading/trailing)
  • Spike suppression (Dt lt 20ns)
  • Zero suppression
  • Calibration Mode (mixed trigger)

Dt time above threshold
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
13
Time Above Threshold )
Time above threshold vs. drift time
  • Gas system
  • He Isobutane 6040
  • Re-circulating gas system,
  • with purification (Bosteels / CERN)
  • 500 l/h, ?10 fresh gas
  • (17 modules)
  • Monitoring
  • O2, _at_ input/output
  • Gas quality monitors (amplitude, drift velocity)

Time above threshold Lower ? higher O2
contamination
high
Lower O2 contamination
) efficient offline noise suppression!
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
14
In-Beam Performance
Hit pattern (central 1.8 AGeV CC) 6 sectors, 17
chambers
Time Resolution (ns)
Chamber Number
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
15
In-Beam Performance
Drift time residuals
Self correlation
Tracking with two chambers Target position
along beam axis
  • Intrinsic spatial resolution 80 - 130 mm
  • Layer efficiencies gt 98
  • (systematic studies in progress, cosmic runs)

C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
16
Summary
  • HADES High-resolution spectroscopy of
    low-momentum electrons and positrons
  • Low-mass planar drift chambers He / Aluminum
  • Customized read out electronics
  • Gradual completion 17 out of 24 chambers in
    operation
  • In-Beam performance according to design values

GSI Darmstadt LHE Dubna FZ Rossendorf IPN ORSAY
C. Müntz, GSI Darmstadt
SAMBA 2002, Trieste
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