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Status of the Photosensor Testing Facility (PTF) at TRIUMF Tom - PowerPoint PPT Presentation

Status of the Photosensor Testing Facility (PTF) at TRIUMF Tom Feusels for Team PTF University of British Columbia 6th Open Meeting for the Hyper-Kamiokande Project Jan 30, 2015 T. Feusels (UBC) PTF Status 30/01/2015 1 / 30 Table of


  1. Status of the Photosensor Testing Facility (PTF) at TRIUMF Tom Feusels for Team PTF University of British Columbia 6th Open Meeting for the Hyper-Kamiokande Project Jan 30, 2015 T. Feusels (UBC) PTF Status 30/01/2015 1 / 30

  2. Table of Contents PTF 1 8” HPD Performance at PTF 2 PTF Measurements 3 T. Feusels (UBC) PTF Status 30/01/2015 2 / 30

  3. Table of Contents PTF 1 8” HPD Performance at PTF 2 PTF Measurements 3 T. Feusels (UBC) PTF Status 30/01/2015 3 / 30

  4. Objectives Y.Nishimura Characterize and study optical properties of PMTs under consideration for HK and near detector. Measure PMT acceptance. Map reflectivity of PMT: important for reconstruction algorithms. Measure wavelength and magnetic field dependence. ... T. Feusels (UBC) PTF Status 30/01/2015 4 / 30

  5. The PTF setup y x z gantry 1 gantry 0 tilt φ rotation θ water- level photo- receiver cathode PMT 5 stepping motors for each of two manipulator arms (gantries) ⇒ 5D (x,y,z, rotation, tilt) Optical box contains USB powered board with 3-axis magnetometer, accelerometer and gyroscope ( Phidget ). Active cancellation with Helmholtz coil, passive cancellation with two layers of g-iron. Light shielding with dark curtains. T. Feusels (UBC) PTF Status 30/01/2015 5 / 30

  6. The PTF setup Receiver PMT Light source Monitor PMT Phidget Waterproof optical box with laser, monitor and receiver PMT attached to the head of the gantry arm. Multiple light sources: 405 and 467nm pulsed laser, Xe lamp with several filters. Collimator, polarizer and beam splitter. T. Feusels (UBC) PTF Status 30/01/2015 6 / 30

  7. Mechanical system: alignment Improvement of mechanical stability and reliability. Alignment of boundaries of X, Y and Z motion for both gantries with respect to each other up to 2 mm and maximize phase space. Alignment of rotation axis: needs to be improved. February: Full survey and realignment using laser trackers. Alignment measurements and measurement accuracy studies under development. T. Feusels (UBC) PTF Status 30/01/2015 7 / 30

  8. DAQ software DAQ and control of PTF through MIDAS. Improvements of the DAQ software: increase of phase space for scans and reliability of long scans. User friendly interface for taking measurements. New measurement sequences being tested: alignment, reproducibility, normal incidence scans,... Automatic conversion of MIDAS files to ROOT files with a flat tree structure. Automatic run logging. T. Feusels (UBC) PTF Status 30/01/2015 8 / 30

  9. Water system venturi vacuum systemfor degassing 2stage 1mm, 50nmultrafilter UV sterilizer Water pumping and purification system ready. Tests in the PTF for early March when tank is in place. Particle counters for water quality monitoring installation at end of March. T. Feusels (UBC) PTF Status 30/01/2015 9 / 30

  10. Table of Contents PTF 1 8” HPD Performance at PTF 2 PTF Measurements 3 T. Feusels (UBC) PTF Status 30/01/2015 10 / 30

  11. HPD setup in PTF: noise control July 2014: 8” HPD prototype arrives at TRIUMF. Proper shielding and grounding of power supply cables crucial for noise reduction. Motors switched off during measurement to limit noise from motor controller. Increased AD bias voltage to almost maximum rating (340V) by increasing LV control voltage (2.33 to 2.8V). T. Feusels (UBC) PTF Status 30/01/2015 11 / 30

  12. HPD signal Motors switched off during measurement to limit noise from motor controller. Properly shielding and common grounding of power supply cables crucial for noise reduction. Increased AD bias voltage to almost maximum rating (340V) by increasing LV control voltage (2.33 to 2.8V). T. Feusels (UBC) PTF Status 30/01/2015 12 / 30

  13. 8” HPD pedestal and single PE distribution 4 10 1 PE resolution: 11.24% Peak to Valley ratio: 5.25 5000 Signal to noise ratio: 12.27 10 3 4000 1 PE resolution: 11.24% Peak to valley ratio: 5.25 2 10 3000 Signal to noise ratio: 12.27 2000 10 1000 1 0 100 150 200 250 300 350 400 100 150 200 250 300 350 400 ADC value ADC value Excellent 1pe resolution. Very good peak to valley ratio and signal to noise 1 ratio. 1 Signal to noise ratio = ratio of SPE peak to pedestal sigma T. Feusels (UBC) PTF Status 30/01/2015 13 / 30

  14. 8” HPD pedestal and single PE distribution AD Bias Dependence 20 400 1PE re solution(%) 18 S/N ra tio 350 P/V ra tio 16 300 14 250 12 10 200 8 150 6 100 4 50 2 0 0 200 400 600 800 1000 1200 2.3 2.4 2.5 2.6 2.7 2.8 LV (V) ADC value Optimal 8” HPD performance at PTF at LV control voltage of about 2.75-2.8V. Individual PE peaks become very clear up to 5 PE in charge distribution. T. Feusels (UBC) PTF Status 30/01/2015 14 / 30

  15. HPD timing resolution Fire laser at HPD. Use 500 MHz digitizer (Caen V1730) for acquiring waveform of monitor PMT and HPD. Width of ∆t = fitted monitor PMT LE time - fitted HPD PMT LE time is resolution. T. Feusels (UBC) PTF Status 30/01/2015 15 / 30

  16. HPD performance at PTF 8” HPD @Kamioka 8” HPD @PTF (LV: 2.8V) 1PE resolution σ/µ 12% 11.2% Peak to valley ratio 5.2 5.25 Signal to Noise 12 12.3 Timing resolution σ (ns) 1.1 1.05 Same performance of 8” HPD in PTF as in Kamioka after improved noise control. Next: Dark noise, pulse shape and stability (gain, DN). PTF in good shape for 20” PMT measurements. T. Feusels (UBC) PTF Status 30/01/2015 16 / 30

  17. Table of Contents PTF 1 8” HPD Performance at PTF 2 PTF Measurements 3 T. Feusels (UBC) PTF Status 30/01/2015 17 / 30

  18. 8” HPD: first intensity map y HPD Mean charge response (PE) x 0.45 Y position (m) 3 z = fixed gantry 0 0.4 2.5 tilt φ = -90° 0.35 2 0.3 1.5 0.25 photo- 1 cathode 0.2 0.5 0.15 0 0 0.05 0.1 0.15 0.2 0.25 0.3 X position (m) Scanning the PMT with the laser pointing vertically downwards in 2cm steps. Using fixed pedestal subtraction and 1PE gain here to calculate average PE per point. Real asymmetry? → Rotate PMT. Actual acceptance should be measured with normal incidence: need PMT curvature and new measurement sequence. T. Feusels (UBC) PTF Status 30/01/2015 18 / 30

  19. HPD vertical 5mm scan with two HPD orientations HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) 0.45 0.45 3.5 3.5 Y position (m) Y position (m) 3 3 0.4 0.4 2.5 2.5 0.35 0.35 2 2 0.3 0.3 1.5 1.5 0.25 0.25 1 1 0.2 0.2 0.5 0.5 0.15 0.15 0 0 0 0.05 0.1 0.15 0.2 0.25 0.3 0 0.05 0.1 0.15 0.2 0.25 0.3 X position (m) X position (m) Fine grained scan shows interesting non uniform pattern with large local variation. Circle with increased intensity possibly from internal reflection on metal inside the PMT (also observed by Hamamatsu). Pattern rotates as HPD rotates. Next: low intensity scan to map gain dependency. T. Feusels (UBC) PTF Status 30/01/2015 19 / 30

  20. HPD vertical 5mm scan with two wavelengths HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) 0.45 0.45 3.5 Y position (m) Y position (m) 4.5 3 0.4 0.4 4 3.5 2.5 0.35 0.35 3 2 2.5 0.3 0.3 1.5 2 0.25 0.25 1.5 1 1 0.2 0.2 0.5 0.5 0.15 0.15 0 0 0 0.05 0.1 0.15 0.2 0.25 0.3 0 0.05 0.1 0.15 0.2 0.25 0.3 X position (m) X position (m) 405nm 467nm Different laser intensity for both! Similar pattern seen in both wavelengths. T. Feusels (UBC) PTF Status 30/01/2015 20 / 30

  21. HPD vertical 5mm scan with 5 ◦ tilt HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) y 0.45 Y position (m) x 3.5 z = fixed 0.4 gantry 0 3 tilt φ = - 8 5° 0.35 2.5 2 0.3 1.5 0.25 photo- cathode 1 0.2 0.5 0.15 0 0 0.05 0.1 0.15 0.2 0.25 0.3 X position (m) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) 0.45 0.45 Y position (m) Y position (m) 3.5 3.5 0.4 0.4 3 3 0.35 0.35 2.5 2.5 2 2 0.3 0.3 1.5 1.5 0.25 0.25 1 1 0.2 0.2 0.5 0.5 0.15 0.15 0 0 0 0.05 0.1 0.15 0.2 0.25 0.3 0 0.05 0.1 0.15 0.2 0.25 0.3 X position (m) X position (m) Similar pattern seen, although different HPD cross section scanned. T. Feusels (UBC) PTF Status 30/01/2015 21 / 30

  22. HPD vertical 5mm scan with 5 ◦ tilt HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) 0.45 4 0.45 Y position (m) Y position (m) 3.5 3.5 0.4 0.4 3 3 0.35 0.35 2.5 2.5 2 0.3 2 0.3 1.5 1.5 0.25 0.25 1 1 0.2 0.2 0.5 0.5 0.15 0 0.15 0 0 0.05 0.1 0.15 0.2 0.25 0.3 0 0.05 0.1 0.15 0.2 0.25 0.3 X position (m) X position (m) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) HPD Mean charge response (p.e.) 0.45 0.45 Y position (m) Y position (m) 3.5 3.5 0.4 0.4 3 3 0.35 0.35 2.5 2.5 2 2 0.3 0.3 1.5 1.5 0.25 0.25 1 1 0.2 0.2 0.5 0.5 0.15 0.15 0 0 0 0.05 0.1 0.15 0.2 0.25 0.3 0 0.05 0.1 0.15 0.2 0.25 0.3 X position (m) X position (m) Similar pattern seen, although different HPD cross section scanned. T. Feusels (UBC) PTF Status 30/01/2015 22 / 30

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