The Light Detection System
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The Light Detection System of protoDune DP Thorsten Lux On behalf - - PowerPoint PPT Presentation
The Light Detection System of protoDune DP Thorsten Lux On behalf of CIEMAT and IFAE Outline Motivation Baseline design Components of the light readout system: PMTs Bases Support structure Wavelength shifter High
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PMTs (provide t0) Cathode (~600 kV) Drift field 0.5 – 1 kV/cm Grid Extraction field 2-3kV/cm Anode (strips) 0V 1 cm 2 mm Collection field 5kV/cm e-
S1: 128 nm
6 m
S2: 128 nm
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Qeff of IFAE reference PMT
Positive base was selected: 1 cable base (positive HV) + ext. splitter
Front-end Splitter Positive power supply GND +HV Decoupling capacitor & power supply filter ,+HV +HV
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Bases currently produced for starting PMT characterization (see Antonio Verdugo’s talk in next session)
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Power supply filter Signal decoupling
Front-end Splitter HV power supply
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800 mm
Stainless Steel support base of the PMTs: 4 PTFE Ø30 mm contact pieces on the membrane floor.
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Weight of the PMT +support & base ~6,5 kg. Buoyancy force of the system ~5,5 kg. => Apparent weight when immersed ~1 kg Tests in 1 bar overpressure (corresponding to 7 m of LAr) and cryogenic temperatures performed.
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The PMT will be placed on the ‘square’ position between the membrane corrugations.
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36 CIEMAT-IFAE PMTs will be installed
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To connect the PMT with the HV power supply and the electronics the following cables are needed:
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Air X2 X2 Cryostat
fibers (~200 m thick)
cryostat or at bottom of cryostat
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Laser (Class 3b):
sensor and PMTs
box and cryostat LED with Kaputschinsky driver:
LED for 18 PMTs
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Light sources:
Optical fibers/bundles under consideration
– Fan-Out Fiber Optic Bundles (Thorlabs) – Bare multi-fiber (i-fiberoptics) Reference sensors (still optional):
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– Safety regulations in the case of the usage of a laser – Accessibility during operation for maintenance – Costs
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0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 2.5 2.6 2.7 2.8 2.9 3 3.1 3.2 3.3
Measured power [nW] at end of each fiber vs LED voltage Light pulse at end of bundle fiber (width: ~12 ns)
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Laser (405 nm) Optical fiber Filters box Fixed Filter LED & Laser controller Fiber splitter Dewar for LN2 PMT monitor R6041-506 @ room temp (to keep track of possible variations in the lighting system) Diffuser (to provide homogeneous illumination) PMT under test R5912-02 QDC Signal from PMTs LabView
configurable amount of light
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Laser pulsed with =< 1 ns pulses
Dark current (DC)
Positive base lower DC than negative base at RT DC at CT higher than at RT
Threshold = 3 mV Threshold = 3 mV
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PMT response vs pulsed light frequency
There is a characteristic saturation curve. Over-linearity effect is observed previous to the PMT saturation. Negative base saturates at lower frequency than the positive base. High frequency decreases the PMT gain at cryogenic temperature.
RT saturation curve Over-linearity
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FP1000ERT i-fiberoptics
Thorlabs (ordered)
– Powermeter (default if sensitive enough for pulsed mode) – PMT or SiPM (alternative)
this week to IFAE, further tests at CIEMAT:
– Mechanical / robustness with the final mounting – Attenuation / Maximum light transmission – Light distribution over the different fibers – Long terms stability – Direct coupling to feedthrough or at bottom
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Goal: Decide if the bundle at the bottom of the detector or directly attached to the flange at the top.
to determine the light output difference among fibers (bundle ordered). Measurement: Study the relative light loss due do adding an extra connector (on-going). Preliminary results: Big light loss observed, studying systematics. Will measure it also with a power sensor
Laser Fiber
LN2 dewar
Laser Filters box PMT @ RT LN2 dewar Fiber w or w/o connector(s) PMT
vs.
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The fiber remains in the same position as before being submerged in LN2 and the light transmission looks fine.
Single fiber testing at LN2 on-going at CIEMAT
Goal: check that the fibers stay in place at cryogenic temperature. Two configuration tested: one as it is, and the other, with a groove and a strip of Teflon → Both worked fine. We plan to measure if there is any light loss due to mechanical stress
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2 optical feedthroughs: 2 main fibers from top to bottom of the detector Each main fiber is split in 18 fibers distributed to half of PMTs
PMTs layout in the detector:
to center the PMTs in the cathode frame structure.
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4.7nF/3KV 4.7nF/3KV
2 + HV & signal
Real Simplified
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– Test of the PD system up to 1 bars (overpressure) (equivalent to ~7m LAr) – Test of PMT response in cold with single wire base: dark current, pulse shape, gain
33 Before immersion 16 h after immersion
Gain evolution with time Mechanical and pressure tests @CIEMAT
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Coated PMT uncoated
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The PMT can be placed on the centre of the ‘square’ position between the stiffener of the shell .
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800 mm Stainless Steel support base of the PMTs: 4 PTFE Ø30 mm contact pieces on the shell.
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Weight of the PMT +support & base ~6,5 kg. Buoyancy force of the system ~5,5 kg. From Adamo
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