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Direct Measurement of Optical Cross-talk in Silicon Photomultipliers Using Light Emission Microscopy Derek Strom, Razmik Mirzoyan, Jrgen Besenrieder Max-Planck-Institute for Physics, Munich, Germany 14 th Pisa Meeting, La Biodola, Isola dElba,


  1. Direct Measurement of Optical Cross-talk in Silicon Photomultipliers Using Light Emission Microscopy Derek Strom, Razmik Mirzoyan, Jürgen Besenrieder Max-Planck-Institute for Physics, Munich, Germany 14 th Pisa Meeting, La Biodola, Isola d’Elba, Italy Photo Detectors and PID May 28, 2018

  2. Outline • Motivation for Silicon Photomultiplier (SiPM) • Optical Cross-talk in SiPM • Light Emission Microscopy and Experimental Setup • Direct Measurement of Cross-talk in a sample SiPM • Summary and Outlook PM2018 May 28, 2018 Derek Strom MPI für Physik 2

  3. Silicon Photomultiplier (SiPM) Solid-state single-photon-sensitive device based on single-photon avalanche diode (SPAD) SPAD concept Single element detector Multi-element arrays Advantages Disadvantages Small cell sizes (10-100 um) High Dark Count Rates (wrt PMT) Nanosecond resolution Afterpulsing Low operating voltage Cross-talk B-field insensitive PDE greater than 40% Large dynamic range PM2018 May 28, 2018 Derek Strom MPI für Physik 3

  4. Optical Cross-talk in SiPMs Strong energy dependence of photon 2 neighboring SPADs absorption lengths in silicon Optical cross-talk • Probability for photons to trigger neighboring cells – Results in artificial increase in signal – Contributes to excess noise factor – Can be significant and problematic in applications – Objective: to learn about cross-talk probability from light emission in SiPMs • PM2018 May 28, 2018 Derek Strom MPI für Physik 4

  5. Optical Cross-talk in SiPMs How to measure cross-talk? By counting photons. • Avalanche Avalanche & cross-talk γ γ γ γ γ SiPM array Light emission microscopy (LEM) is a precise and powerful visual tool for directly • measuring optical cross-talk. Useful to also observe defects in cells, morphology of the avalanche process, etc. • PM2018 May 28, 2018 Derek Strom MPI für Physik 5

  6. Light Emission Microscopy LEM is a powerful root cause failure analysis technique for detecting low • light levels otherwise not visible to an observer. Utilizes resolving power of an objective lens and a low-noise camera to • detect weak light emission, e.g. from semiconductor devices such as SiPMs. γ Dark Box Integrated counts SiPM Light emission Magnification γ γ PM2018 May 28, 2018 Derek Strom MPI für Physik 6

  7. Direct Measurement of Cross-talk Illuminate one SiPM cell with small laser spot (<< cell size). • • Observe emission of photons from primary and secondary avalanche processes using a microscope and record with a low-noise CCD. • Count photons emitted from the central cell where laser is fired and from neighboring cells at distance 1 cell-unit away. SiPM Array • Assume the counts outside central cell are all cross-talk counts since the Laser spot laser is focused well within the central cell. • Measure cross-talk Cross-talk = Counts (out) / Counts (in) Counts (in) Counts (out) PM2018 May 28, 2018 Derek Strom MPI für Physik 7

  8. Setup PC CCD camera (Andor Clara) 1392 x 1040 sensor Function generator 2.5 e - readout noise 1 e - /hr thermal noise Tube lens Laser (440 nm) Long pass filter (495 nm) ~10 ps pulse width Pellicle beam splitter Single mode fiber Objective Lens (Olympus 10X, 0.25 NA) Collimating lens SiPM sample X-Y-Z translation stage Laser Light emission PM2018 May 28, 2018 Derek Strom MPI für Physik 8

  9. Setup SiPM Sample Hamamatsu LCT4 single element • Device size = 3 mm x 3 mm • Cell size = 75 um x 75 um • Breakdown voltage = 51.10V • Cross-talk measured as function of • overvoltage PM2018 May 28, 2018 Derek Strom MPI für Physik 9

  10. SiPM under 10X Magnification 1040 px Hamamatsu 75 um Ambient light conditions 116 px 1392 px PM2018 May 28, 2018 Derek Strom MPI für Physik 10

  11. CCD Imaging Steps Step 1: Dark image Step 2: Background image with laser light only • To account for any reflections o ff surface of SiPM Step 3: Background image with bias voltage only applied to SiPM • To account for light emission from powered device Step 4: Signal image with laser light and bias voltage applied to SiPM Integration time for each step is 30 seconds PM2018 May 28, 2018 Derek Strom MPI für Physik 11

  12. Beam Profile Measured with CMOS camera 1px = 3.8 um X Y FWHM: 11 um FWHM: 11 um PM2018 May 28, 2018 Derek Strom MPI für Physik 12

  13. Observed Light Emission Overvoltage = 5V Integration time = 30s Hot spots? Laser fired here Cross-talk emission PM2018 May 28, 2018 Derek Strom MPI für Physik 13

  14. Observed Light Emission • The laser light is focused on a single cell. • Light is observed from the fired cell and also neighboring cells. PM2018 May 28, 2018 Derek Strom MPI für Physik 14

  15. Direct Measurement of Cross-talk COUNTS_IN = Σ ☐ COUNTS_OUT = Σ ☐ Cross-talk = COUNTS_OUT / COUNTS_IN Overvoltage 5V Cross-talk = ~23% PM2018 May 28, 2018 Derek Strom MPI für Physik 15

  16. Optical Cross-talk vs. Overvoltage LEM Method - Preliminary Standard Method (i.e. theshhold) [NIM A 806 (2016), 383-394] PM2018 May 28, 2018 Derek Strom MPI für Physik 16

  17. Summary and Outlook SiPMs are attractive photo-detectors for high-energy and astroparticle physics • experiments. Compact in size – Fast (few ns) response time – Low operating voltages compared to classical PMTs – Insensitive to magnetic fields – Photon detection e ffi ciencies greater than 40%. – Crucial to reduce/eliminate cross-talk between neighboring cells. • Light emission microscopy is a powerful visual tool for measuring and • understanding the physics behind optical cross-talk, as well as for observing defects, avalanche morphology, etc. LEM method is the most precise measurement of cross-talk. • Plans to measure cross-talk: • – in new batches of SiPMs. – in cells > 1 unit distance away from center. – at di ff erent regions of the cell. – near the borders of the device. PM2018 May 28, 2018 Derek Strom MPI für Physik 17

  18. sense-pro.org See us at the poster session Consortium Members UNIGE: A. Nagai, D. della Volpe, T. Montaruli KIT: A. Haungs, K. Link DESY: K. Henjes-Kunst MPI: R. Mirzoyan, D. Strom PM2018 May 28, 2018 Derek Strom MPI für Physik 18

  19. Backup PM2018 May 28, 2018 Derek Strom MPI für Physik 19

  20. Low Intensity Background Rejection Background region PM2018 May 28, 2018 Derek Strom MPI für Physik 20

  21. Low Intensity Background Rejection Signal region PM2018 May 28, 2018 Derek Strom MPI für Physik 21

  22. Hot Spot Bkg: Laser Only Bkg: Bias Only Signal Emission observed in signal image only PM2018 May 28, 2018 Derek Strom MPI für Physik 22

  23. SiPM under 10X Magnification 1040 px Hamamatsu 100um Ambient light conditions 155 px 1392 px PM2018 May 28, 2018 Derek Strom MPI für Physik 23

  24. Scope Trace Laser pulse 500 kHz SiPM output PM2018 May 28, 2018 Derek Strom MPI für Physik 24

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