sci-fi tracker for it replacement
DESCRIPTION
Lausanne 9. December 2010. Sci-Fi tracker for IT replacement. [email protected]. Commercial available SiPMs ( MPPCs ) from Hamamatsu. Customized 128 CH MPPC array for Sci-Fi tracker use. Array optimized for small dead aera between modules - PowerPoint PPT PresentationTRANSCRIPT
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Sci-Fi tracker for IT replacement
Lausanne 9. December 2010
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Commercial available SiPMs (MPPCs) from Hamamatsu
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Customized 128 CH MPPC array for Sci-Fi tracker use
• Array optimized for small dead aera between modules
• Optimized for high channel number on one module
• For the use in LHCb and PEBS• Atotal= 0.25mm x 1.2mm x 128
• Apixel=50um x 50um
• Npixel=88• G=0.75x106 e/PE• Nchannel = 128
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32mm
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Fiber tracker for LHCb IT
4Bonding wires
Rectangular channels
Cross section view
Reduce epoxy layer to decrease diffusion
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Fiber tracker for LHCb IT
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IT replacement detector box
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Measurements with 25,50 and 100um pixel detectors
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1mm2, 50umx50umFdark=0.4MHz 1mm2, 50umx50um
9mm2, 100umx100umFdark=10MHz
2mm2, 25umx25umFdark=0.6MHz
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Adaptation of the Beetle input circuit for the use with an SiPM
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Silicon strip SiPM 0.25mmx1.2mm 50um pixel
Detector capacitance 10-15pF 10pF
Gain 22ke/MIP (300um Si)
0.75*106/Pe (15Pe /MIP)
Rel Gain / MIP 1 511
Load resister required for fast readout (25ns)
~1kOhm 100-200 Ohm
Dynamic range 0..5MIP 0..3MIP (reduce signal by 300)
Why do we need an adaption? Difference between the SiPM and the silicon strip readout.
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Model of SiPM (1mmx1mm, 50um pixel) voltage on Rs
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Adjusted the model of the SiPM to the measured pulses, the graphs show voltage on Rs
Note that the pulse height is different for different Rs.
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Model of SiPM (1mmx1mm, 50um pixel) Charge Q
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Adjusted the model of the SiPM to the measured pulses, the graphs show the current and the charge injected to the Beetle from the
120fC = 0.75*106e
The simulation shows the values for different Rs.
The charge is equal for all Rs
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Beetle response for different injection time
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The arrival of several photons on the detector slows down the rise time of the pulse of the detector measured at Rs, this doesn’t result in a different charge injected. The falling edge fast time constant is responsible for a partial discharge during the arrival of the different photons.
Note that the pulse height is different for different length o interval of injection time.
NOT LICENSED FOR COMMERCIAL USE
Transient - , sipm_model_adapted_to_measurement.sch + sipm_model_adapted_to_measurement.Anl, 10 December 2009
TPv1 (right)
Time0 1.00n 2.00n 3.00n 4.00n 5.00n 6.00n 7.00n 8.00n 9.00n 10.0n
-100u
0
100u
200u
300u
400u
500u
600u
700u
800u
900u
1.00m
y 4.18850E-5x 1.00000E-8
RS=20RS=31.429RS=42.857RS=54.286RS=65.714RS=77.143RS=88.571RS=100
Select
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Beetle response with SiPM signalDifferent injection interval (0.5ns, 1ns, 2ns, 4ns, and 10ns) to observe the effect of the
arrival of a pulse with different arrivals of the photons.
Only with 10ns some degradation is observed. Response height is almost the same.
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R-R current divider is used.
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Injection prototype with Beetle FE chip
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• Use the IT hybrid with Beetle 1.3• Using the Velo analog data signal chain for DAQ (repeater, analog cable, ADC on Tell1• Attenuator test circuit
bonded to pitch adapter
Beetle 1.3 IT hybrid
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Use very low number of photons
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R1=200R2=10KG=1/50
R1=200R2=15KG=1/75
R1=200R2=20KG=1/100
R1=200R2=30KG=1/150
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Inject more photons
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R1=200R2=10KG=1/50
R1=200R2=15KG=1/75
R1=200R2=20KG=1/100
R1=200R2=30KG=1/150
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Inject more photons, saturation for the highest gain channels sets in
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R1=200R2=10KG=1/50 R1=200
R2=15KG=1/75
R1=200R2=20KG=1/100
R1=200R2=30KG=1/150
Gain Dynamic rangeSiPM
CH 4 26 ADC/Pe 0…9 Pe
CH 5 18 ADC/Pe 0…13 Pe
CH6 12 ADC/Pe 0…19 Pe
CH7 8 ADC/Pe 0…28 Pe
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Outlook (electronics view)
• Designing new IT hybrids with current divider integrated
• Designing flex PCB modules for 128CH MPPC modules• Characterize electronics performance (noise and
dynamic range) • Integrating Sci-Fi modules with IT replacement
dimensions produced by Aachen PEBS group• Further radiation tests
– Testing shielded box– Testing SiPM irradiated by LHCb
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