Single tube detection efficiency BIS-MDT

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Single tube detection efficiency Single tube detection efficiency BIS-MDT BIS-MDT

description

Single tube detection efficiency BIS-MDT. GARFIELD 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. GARFIELD Simulation. Longitudinal diffusion coefficient. - PowerPoint PPT Presentation

Transcript of Single tube detection efficiency BIS-MDT

Page 1: Single tube detection efficiency BIS-MDT

Single tube detection efficiencySingle tube detection efficiency BIS-MDTBIS-MDT

Page 2: Single tube detection efficiency BIS-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

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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

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Drift VelocityDrift Velocity

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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

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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

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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

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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

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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

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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

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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)

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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

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Energy SpectrumEnergy Spectrum

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MDT time spectrum MDT time spectrum

dx

dN

dt

dx

dx

dN

dt

dN

ConstantVelocity DependenceTDC Spectrum

ttmaxmax ttmaxmax

ttoottoo

tt11tt11