LENA Photosensor R&D Marc Tippmann Lothar Oberauer, Michael Wurm, Gyorgy Korga, Quirin Meindl, Michael Nöbauer, Thurid Mannel, Martin Zeitlmair, German Beischler Technische Universität München DPG-Frühjahrstagung 2011, Karlsruhe 2011/03/31 Overview LENA photosensor requirements PMT characterization • Measurements at the Laboratori Nazionali del Gran Sasso Outlook • Munich test stand • Optical module development Summary LENA photosensor requirements LENA photosensor requirements: Overview Requirements on photo sensors • Sensor performance • Environmental properties • Availability until start of construction • Cost-performance-ratio Desired energy resolution for low energies: → Light yield ≥ 200 photoelectrons/MeV → 30% optical coverage → 3000m² effective photosensitive area needed → Current standard configuration: Liquid scintillator detector: 63,000 PMTs (8“) with Winston Cones (area ×1.75) Water cherenkov muon veto: 6,000 PMTs (8“) 1/9 LENA photosensor requirements: List Timing TTS (spe, FWHM) <3.0ns Early pulses <1% Late pulses <4% 2/9 LENA photosensor requirements: List Timing TTS (spe, FWHM) <3.0ns Early pulses <1% Late pulses <4% Photo detection efficiency PDE for λpeak=420nm >20% Dynamic range spe – 0.3pe/cm² 2/9 LENA photosensor requirements: List Timing TTS (spe, FWHM) <3.0ns Early pulses <1% Late pulses <4% Michael Wurm, TUM, LENA - PMm² meeting 07/04/2009 Photo detection efficiency PDE for λpeak=420nm >20% Dynamic range spe – 0.3pe/cm² Noise (for PMTs) Gain >3∙106 spe p/V >2 Dark count per area <15Hz/cm² Ionic afterpulses (0.1-200 μs) <5% Fast afterpulses (5-100 ns) <5% 2/9 LENA photosensor requirements: List Teresa Marrodán, PhD thesis Timing TTS (spe, FWHM) <3.0ns Early pulses <1% Late pulses <4% Photo detection efficiency PDE for λpeak=420nm >20% Dynamic range spe – 0.3pe/cm² Noise (for PMTs) Gain >3∙106 spe p/V >2 Dark count per area <15Hz/cm² Ionic afterpulses (0.1-200 μs) <5% Fast afterpulses (5-100 ns) <5% Photon Fast afterpulse 2/9 LENA photosensor requirements: List Teresa Marrodán, PhD thesis Timing TTS (spe, FWHM) <3.0ns Early pulses <1% Late pulses <4% Photo detection efficiency PDE for λpeak=420nm >20% Dynamic range spe – 0.3pe/cm² Noise (for PMTs) Environmental properties Gain >3∙106 Pressure resistance >10bar spe p/V >2 238U <3∙10-8 g/g Dark count per area <15Hz/cm² 232Th Ionic afterpulses (0.1-200 μs) <5% natK Fast afterpulses (5-100 ns) <5% Detector lifetime content content content <1∙10-8 g/g <2∙10-5 g/g >30yrs 2/9 LENA photosensor requirements Fast afterpulses (fAP): Ongoing measurements of fAP time distribution for candidate PMT series → • Investigate causes • Currently studying their influence on the efficiency of the p decay coincidence: Bachelor thesis by Thurid Mannel • Possible methods of discrimation from photons? Bachelor thesis by Martin Zeitlmair 3/9 PMT characterization Measurements at the LNGS, Gran Sasso Borexino PMT testing facility • Pulsed ps laser diode light source: 410nm, light pulse FWHM <30ps • Total time resolution <140ps • Can measure up to 32 PMTs simultaneously • Measure transit time distribution (TDC), fast + ionic afterpulse time distribution (MTDC), charge spectrum (ADC) Measured 1 sample each of: • Hamamatsu: R6091(3“), R6594(5“), R5912(8“) and R7081(10“) • ETEL: 9351(8“) 4/9 Measurements @LNGS: R6594 vs. R7081 5“ 10“ R6594 (5“) R7081 (10“) Voltage +1670V +1520V Gain 1.0∙107 1.3∙107 Photoelectrons (pe) per trigger 5.53% 2.91% Threshold 0.2pe 0.2pe TTS (FWHM) (Hamamatsu) 1.91ns (1.5ns) 3.05ns (3.5ns) Early pulses (all non-gaussian) 2.95% 0.57% Late pulses (after photon pulse peak) 3.13% 3.09% 5/9 Measurements @LNGS: R6594 vs. R7081 R6594 (5“) R7081 (10“) Voltage +1670V +1520V Gain 1.0∙107 1.3∙107 Photoelectrons (pe) per trigger 5.53% 2.91% Threshold 0.2pe 0.2pe TTS (FWHM) (Hamamatsu) 1.91ns (1.5ns) 3.05ns (3.5ns) Early pulses (all non-gaussian) 2.95% 0.57% Late pulses (after photon pulse peak) 3.13% 3.09% (5.23kHz) 2.64kHz (46.3 Hz/cm²) 5.26 Hz/cm² 0.94% 5.12% Dark count Dark count per area Ionic afterpulses 5/9 Measurements @LNGS: R6594 vs. R7081 R6594 (5“) R7081 (10“) Voltage +1670V +1520V Gain 1.0∙107 1.3∙107 Photoelectrons (pe) per trigger 5.53% 2.91% Threshold 0.2pe 0.2pe TTS (FWHM) (Hamamatsu) 1.91ns (1.5ns) 3.05ns (3.5ns) Early pulses (all non-gaussian) 2.95% 0.57% Late pulses (after photon pulse peak) 3.13% 3.09% (5.23kHz) 2.64kHz (46.3 Hz/cm²) 5.26 Hz/cm² 0.94% 5.12% 3.88 3.09 Dark count Dark count per area Ionic afterpulses Peak-to-valley ratio 5/9 Measurements @ LNGS: Results Parameters + Constraints R6091 (3“) with 1.8“ aperture R6594 (5“) R5912 (8“) R7081 (10“) ETL9351 (8“) no. 1732 ETL9351 (8“) average Voltage +1760V +1670V +1425V +1520V +1500V ≈+1450V Gain 1.0∙107 1.0∙107 1.3∙107 1.3∙107 1.0∙107 1.0∙107 pe/trigger (npe) 2.21% 5.53% 1.83% 2.91% 4.78% 5.19% TTS (FWHM) <3.0ns (manufacturer) 1.89ns (2.0ns) 1.91ns (1.5ns) 2.04ns (2.4ns) 3.05ns (3.5ns) 2.16ns 2.76ns EP (all nongauss.) <1% 0.14% 2.95% 1.93% 0.57% 1.23% 0.75% (3σ) LP (after PP peak) <4% 6.26% 3.13% 2.88% 3.09% 4.08% 7.90% (3σ) 0.192kHz (5.23kHz) 1.62kHz 2.64kHz 1.72kHz 2.48kHz 12.1 Hz/cm²(eff.) (46.3 Hz/cm²) 5.1 Hz/cm² 5.3 Hz/cm² 5.3 Hz/cm² 7.7 Hz/cm² 0.14% 0.94% 6.62% 5.12% 2.57% 4.9% 2.04 3.88 2.99 3.09 2.25 2.10 DN DN/area <15Hz/cm² Ionic AP < 5% p/V >2 At the moment no conclusive decision possible: Need to measure ≈10 PMTs/series and determine limits + implications on physics from simulations 6/9 Outlook Outlook: Munich photosensor test stand • FADC: Acqiris DC282, 10bit, 8 GHz • Light sources: • Pulsed ps diode laser: Edinburgh Instruments EPL-405-mod, 403nm, pulse width 48ps • Fast LED driven by avalanche diode: 430nm, time jitter (FWHM) <≈1ns Currently being set up Done: Light sources implemented and working, electronics running Next steps: include fiber and beam widening optics, finish online analysis software based on Labview Plan to study: PMTs: time distribution, fast AP, ionic AP, pulse shape, dynamic range, surface scans; also SiPMs 7/9 Outlook: Optical module development Light Concentrators (Winston Cones) Borexino Winston Cone • MC simulations of light concentrators with geant4 • Incorporate results into optical model of detector (geant4 MC) → determine optimum light concentrator • Build prototype + scan with laser over aperture and incident angles Diploma thesis by Michael Nöbauer Pressure encapsulations • Design pressure encapsulations with FEM pressure simulation, e.g. spherical shape or conical shape, integrate Winston Cones + Mu-metal shielding into design • Build + test prototypes Bachelor thesis by German Beischler 8/9 Summary • Approximate limits on photosensor properties known → do simulations to refine values • Have tested promising PMT series from Hamamatsu @ LNGS → repeat for more samples of Hamamatsu + ETEL PMTs in Munich • Also test SiPMs and Hybrid Phototubes • Have started development of pressurewithstanding optical modules for PMTs incorporating Winston Cones and Mu-metal 9/9
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