Four Channels Data Acquisition System for Silicon Photomultipliers - PowerPoint PPT Presentation

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Four Channels Data Acquisition System for Silicon Photomultipliers

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Title: Four Channels Data Acquisition System for Silicon Photomultipliers


1
Four Channels Data Acquisition System for Silicon
Photomultipliers
Mateusz Baszczyk, Piotr Dorosz, Sebastian
Glab,Wojciech Kucewicz, Lukasz Mik, Maria Sapor
Department of Electronics, AGH University of
Science and Technology, Al. Mickiewicza 30,
30-059 Krakow, Poland e-mail kucewicz_at_agh.edu.pl s
glab_at_agh.edu.pl
2
Agenda
  • Fluorescence
  • Silicon Photomultiplier description
  • Description of previous measurement system
  • Four channel data acquisition system
  • Results
  • Summary
  • Future work.

3
Why do we measure fluorescence light intensity?
  • Dye-labelled cells can be count by fluorescence
    light intensity measurement
  • At low concentrations the fluorescence intensity
    is generally proportional to the concentrations
    of fluorophore.

4
Fluorescein and Bio-Tek filters spectra
fluorescein
resorufin
5
Optical block
6
Silicon Photomultiplier
  • The idea appears in the late 90-ties
  • Photon Detection with High Gain Avalanche
    Photodiode Arrays S. Vasile, P. Gothoskar, R.
    Farrell, D. Sdrulla
  • Silicon avalanche photodiodes on the base of
    metal-resistor-semiconductor (MRS) structures V.
    Saveliev, V. Golovin

7
Structure
8
Current - Voltage Characteristic
9
Photodiode Operation Mode
1 photon generates 1 electron-hole pair
10
Avalanche Operation Mode
1 photon generates 10-200 electron-hole pairs
11
Geiger Operation Mode
1 photon generates 105 - 106 electron-hole pairs
12
Typical SiPM Parameters
sensL s1020 Hamamatsu S10362-11-025C
Spectral Range (?) 400-1100 nm 320-900 nm
Peak Spectral Response (?) 490 nm 440 nm
Breakdown Voltage (Vbr) 28.6 V ---
Operating Voltage (V) 30.6 V 70.82 V
Microcell Gain 106 2.75 105
SPM Pixel Active Area F 1 mm F 1 mm
Number of Pixels 400 1600
Dark Rate (MHz) 0.42 0.3
13
Previous Measurement System For Fluorescence
Agilent 33250 generator
trigger signal
gate pulses
Picosecond 2600C generator
Cuvette holder with specimen
GPA amplifier
QDC device
PC with Labview application
excitation filter
emission filter
14
First Measurement System For Fluorescence
15
Acquisition System
16
Acquisition System
17
Front-end ASIC
18
Front-end ASIC
19
Front-end ASIC
20
Linearity high gain
21
Linearity low gain
22
Measurement results
23
Measurement results
24
Measurement results
25
Measurement results
26
Measurement results
27
Measurement results
28
Light Intensity
29
Light Intensity
30
Light Intensity
31
Without Coincidence
32
Coincidence
33
Results of fluorescence light measurements
y -572500 x² 223.6 x 6458000
fluorescein y -373800 x² 170.3 x 14030000
resorufin
34
Influence of Temperature and Bias
35
Dark Current Rate
36
Influence of Temperature and Bias
37
Conclusions
  • We have designed, built and optimized readout
    system for detection of single photons
  • We have tested readout circuit with light and
    confirmed that it is linear
  • We can distinguish a dozen or so photons and
    eliminate thermal generation from measurement
    data
  • System with silicon photomultiplier has a good
    sensitivity and can be used to measure
    fluorescence light intensity for fluorescein
    concentration from 1ug/ml to about 60pg/ml and
    resorufin at the level of 1ng/ml up to 1ug/ml.

38
Future work
  • Stabilization system compensating temperature
    influence on SiPM gain by varying supply voltage
  • Measurements of fluorescent dyes in
    microbioreactors.

scanning probe
micro-bioreactor
39
Thank you for your attention
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