javier caravaca, benjamin land, gabriel orebi …javier caravaca, benjamin land, gabriel orebi gann....
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E L E C T R O N I C R E Q U I R E M E N T S F O R T H E I A R & D AT B E R K E L E Y
J A V I E R C A R A VA C A , B E N J A M I N L A N D , G A B R I E L O R E B I G A N N
A T O U R F O R T H E I A R & D AT B E R K E L E Y
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2) Light setup Measures the scintillation
light yield 6 10inch-PMTs R7081
1) Timing setup Cherenkov/Scintillation
separation from vertical cosmics 12 1inch-PMTs H11934
Veto panel
Veto
pan
el
Veto panels underneath
FE panel
A T O U R F O R T H E I A R & D AT B E R K E L E Y
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2) Light setup CAEN digitizer V1730 (500MHz)
1) Timing setup CAEN digitizer V1742 (5GHz)
Buffer limited to 1024 samples → ~200ns event window
VME crate
FE panel
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T H E T I M I N G S E T U P
Target filled with WBLS
Muon tagsOptical propagation
medium
PMTs
Trigger off the muon tags on vertical cosmics
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T H E T I M I N G S E T U P
Target filled with WBLS
Muon tagsOptical propagation
medium
PMTs
Trigger off the muon tags on vertical cosmics
LAB+PPO simulation
P R O J E C T E D P E R F O R M A N C E S O F O U R C U R R E N T S E T U P
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LAB+PPO
Detected PE time, ToF corrected (ns)
Simulation includes most of the DAQ effects → PMT TTS, realistic pulses,
electronic noise, …
Simulation
C H E R E N K O V V S S C I N T I L L AT I O N
t(ns)∆0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
PE/E
vent
/20p
s
0
0.1
0.2
0.3
0.4
0.5
0.6
t(ns)∆5.5 6 6.5 7 7.5
PE/E
vent
/20p
s
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
t(ns)∆0 50 100 150 200 250 300 350 400 450 500
PE/E
vent
/20p
s
3−10
2−10
1−10
1
10
Solid - Cherenkov Dash - Scintillation
Typically <ns difference
Scintillation tails extendsto ~400ns
With PMT TTS (0.3ns)W/o PMT TTS
Detected PE time
Detected PE time
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C H E R E N K O V V S S C I N T I L L AT I O N
t(ns)∆0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
PE/E
vent
/20p
s
0
0.1
0.2
0.3
0.4
0.5
0.6
t(ns)∆5.5 6 6.5 7 7.5
PE/E
vent
/20p
s
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
t(ns)∆0 50 100 150 200 250 300 350 400 450 500
PE/E
vent
/20p
s
3−10
2−10
1−10
1
10
Solid - Cherenkov Dash - Scintillation
Typically <ns difference
Scintillation tails extendsto ~400ns
With PMT TTS (0.3ns)W/o PMT TTS
Detected PE time
Large buffers > 400ns
Detected PE time
Fast sampling rate ~10GHz (0.1ns)
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C R I T I C A L P O I N T S
• Sampling rate
• Currently working at 5GHz → 0.2ns resolution
• The current limiting factor is the PMT TTS ~ 0.3ns
• Getting to 0.1ns would neglect the source of error coming from the electronics
• Buffer size
• Not catching the whole scintillation light (~400ns) would lead to systematics in the light yield measurements
• Preferably larger than 400ns to allow for direct pedestal correction
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D Y N A M I C R A N G E
• Handling single and multi PE at a time requires a broad range with a good enough resolution
• A 2V range with 12 bits resolution (0.5mV) has demonstrated to be sufficient
Coincidence event
<0.5mV
~10mV (gain dependent)
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T R I G G E R I N G C A PA B I L I T I E S
• Customizable global trigger
• Issue from any of the channels
• Coincidence & anti-coincidence from two or more channels
• Rising or falling edges
• Configurable threshold
• On-board pedestal correction
• Trigger delay: useful for synchronization with external triggers
• Clock
• Synchronization capabilities: for event correlation between devices
• Timestamp rollover>hours → 50bit 10GHz would be ideal
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S U M M A R Y
• Fast digitization is crucial for this project as well as a large enough buffer
• Scalability is a plus → Currently using 25 channels. Might be extended to >30.
• Requirements
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