Single tube detection efficiency BIS-MDT
description
Transcript of Single tube detection efficiency BIS-MDT
Single tube detection efficiencySingle tube detection efficiency BIS-MDTBIS-MDT
GARFIELD SimulationGARFIELD Simulation
Anode wire voltage as a function of the distance from the
wire
Electric field as a function of the drift
path
Muon track in a distance of 0.1 cm from the anode
wire
Electron drift velocity (in cm/μsec) as a function of the
drift path
Ion mobility as a function of the electric
field
Diffusion coefficients (transverse and
longitudinal) as a function of the electric field
GARFIELD SimulationGARFIELD Simulation
Longitudinal diffusion coefficient
Transverse diffusion coefficient
Drift VelocityDrift Velocity
Operation PrincipleOperation Principle
A muon with pT=1ΤeV/c has a track sag τροχιά of 500 μm in a magnetic field 0.4 Τ (mean value).
Momentum resolution of 10 requires precision of 50 μm in the muon track sag.
μμ
r
CVrE
1
2)(
0
0
rCV
rV ln2
)(0
0
Electronic SignalElectronic Signal
PM Analog Signal
Amplitude 400 mV
Time Width 20 ns
PM Logic Signal
Preamplifier
Discriminator (constant fraction)
Amplitude 600 mV
Time Width 14 ns
Hodoscope Logic Diagram Hodoscope Logic Diagram
Meantimer : Time resolution 1 ns
TDC: Time resolution 50 ps on 100 ns range
System time resolution 1,5-2,0 ns
Spatial resolution 20 cm
ChamberChamber BIS-MDT BIS-MDT
Gas Manifold
Parallel gas supply at each tube at each multilayer
Hedgehog cards
Decouple the signals from the wires and provide discharge protection for
the amplifier inputs
Mezzanine cards
4 Amplifier Shaper Discriminator chips 1 TDC chip
Time resolution of a Time resolution of a system of a scintillatorsystem of a scintillator
++
smallsmall (15(1515151 cm1 cm33) ) reference scintillatorreference scintillator
Small contribution to Small contribution to the overall time the overall time
resolutionresolution
Hodoscope time resolutionHodoscope time resolution
BIS-MDT ‘BEATRICE’ atBIS-MDT ‘BEATRICE’ at the X5/GIF areathe X5/GIF area
Cosmic muons
Cosmic muons in presence of the background of the source Cs137 Photons 662 keV, 740
GBq (3/1997), t1/2=30 y
Photon flux at 4 m = 0,86105 cm-2s-1
ChamberChamber BIS-MDT BIS-MDT electronics electronics
Pseudo-differential pair of preamplifiers (Active and Dummy)
Differential amplifier (gain) – Two stages of Differential Amplifiers (gain & bipolar shaping)
Shaper Discriminator ADC (leading edge slew correction timing resolution)
MDT Operation PrincipleMDT Operation Principle
Inefficiency due to a δ-δ-electronelectron shadowing the muon.
Probability Distance
Discreteness of the ionization mechanism Lower
resolution close to the wire
Decrement of the track-wire distance
Large fluctuations
Energy SpectrumEnergy Spectrum
MDT time spectrum MDT time spectrum
dx
dN
dt
dx
dx
dN
dt
dN
ConstantVelocity DependenceTDC Spectrum
ttmaxmax ttmaxmax
ttoottoo
tt11tt11