Creating a System to Test Single Photon Avalanche Diodes Introduction Single Photon Avalanche Diodes (SPADs) are optical sensing amplifiers which make use of an ionization mechanism in which incoming photons trigger an avalanche current. The trigger of the avalanche current indicates a photon has impacted the device which allows SPAD sensors to detect weak optical signals. Single Photon Avalanche Diodes have many practical applications in fields such as medical imaging, astronomy, astrophysics, and other sensitive vision systems. In this project, the researchers improve a system to test SPAD chip devices by automating the data acquisition using MATLAB. Methodology 1.) Developing a Printed Circuit Board In order to test the Single Photon Avalanche Diode, the researchers used Eagle PCB to develop a Printed Circuit Board in which any fabricated DIP40 packaged chips could be tested. The resistor acts as a passive quencher for the SPAD. Figure 4 shows the optical sensing capabilities from the SPAD. Each spike in voltage corresponds to the impact of a photon on the device. The return to the baseline after each spike represents the passive quenching process. Conclusion • Automating the process of testing Single Photon Avalanche Diode devices helps make the process faster and more efficient. • This project provides insight into potential improvements for the testing of Single Photon Avalanche Diodes. Results Alex Chan 1 , Geneva Doak 2 , Mohammad Habib Ullah Habib 2 , Dr. Nicole McFarlane 2 Farragut High School 1 , University of Tennessee 2 2.) Data acquisition using MATLAB To automate the voltage and current measurements from the SPAD, an MATLAB code was used to interface with a Keithley 2400 sourcemeter to collect and plot current vs source voltage data. To prove the code is accurate, it was tested with a 100k ohm resistor and Ohm's Law was used to confirm accuracy. \ Figure 3 is a graph from the electrical testing of the sourcemeter depicting relationship between voltage and current of the SPAD chip. At around -14 Volts, the reverse-bias voltage caused the breakdown. Figure 3: Graph of the applied voltage vs measured current of the SPAD Figure 4: Optical data of SPAD from the oscilloscope Figure 1: Design of the Printed Circuit Board Figure 2: Graph of current vs voltage Applied Voltage (V) Keithley 2400: Sweeps V (1V to -18V) & Measure current through SPADs Measured Current (I) Keithley 2400: Sweeps V (1V-10 V) & Measure I Measured Current (I) Source Voltage (V) Acknowledgements: This work was supported primarily by the Engineering Research Center Program of the National Science Foundation and the Department of Energy under NSF Award Number EEC- 1041877 and the CURENT Industry Partnership Program. • Electrical testing of the SPAD was done using the data acquisition code for the sourcemeter. A voltage was supplied and the current was measured • Optical testing of the SPAD was done using the data acquisition MATLAB code for the oscilloscope. The SPAD was excited by photons from daylight to generate voltage spikes. These were quenched by a 100 Ohm resistor.

Creating a System to Test Single Photon Avalanche Diodes Introduction Single Photon Avalanche Diodes (SPADs) are optical sensing amplifiers which make

Download PPTX Report

Upload
lynette-peters
View
215
Download
3

Embed Size (px)

Citation preview

Creating a System to Test Single Photon Avalanche Diodes

IntroductionSingle Photon Avalanche Diodes (SPADs) are optical sensing amplifiers which make use of an ionization mechanism in which incoming photons trigger an avalanche current. The trigger of the avalanche current indicates a photon has impacted the device which allows SPAD sensors to detect weak optical signals. Single Photon Avalanche Diodes have many practical applications in fields such as medical imaging, astronomy, astrophysics, and other sensitive vision systems. In this project, the researchers improve a system to test SPAD chip devices by automating the data acquisition using MATLAB.

Methodology1.) Developing a Printed Circuit BoardIn order to test the Single Photon Avalanche Diode, the researchers used Eagle PCB to develop a Printed Circuit Board in which any fabricated DIP40 packaged chips could be tested. The resistor acts as a passive quencher for the SPAD.

Figure 4 shows the optical sensing capabilities from the SPAD. Each spike in voltage corresponds to the impact of a photon on the device. The return to the baseline after each spike represents the passive quenching process.

Conclusion• Automating the process of testing Single Photon

Avalanche Diode devices helps make the process faster and more efficient.

• This project provides insight into potential improvements for the testing of Single Photon Avalanche Diodes.

Results

Alex Chan1, Geneva Doak2, Mohammad Habib Ullah Habib2, Dr. Nicole McFarlane2

Farragut High School1, University of Tennessee2

2.) Data acquisition using MATLABTo automate the voltage and current measurements from the SPAD, an MATLAB code was used to interface with a Keithley 2400 sourcemeter to collect and plot current vs source voltage data. To prove the code is accurate, it was tested with a 100k ohm resistor and Ohm's Law was used to confirm accuracy.

Figure 3 is a graph from the electrical testing of the sourcemeter depicting relationship between voltage and current of the SPAD chip. At around -14 Volts, the reverse-bias voltage caused the breakdown.

Figure 3: Graph of the applied voltage vs measured current of the SPAD

Figure 4: Optical data of SPAD from the oscilloscope

Figure 1: Design of the Printed Circuit Board

Figure 2: Graph of current vs voltage

Applied Voltage (V)

Keithley 2400: Sweeps V (1V to -18V) & Measure current through SPADs

Mea

sure

d C

urre

nt (

Keithley 2400: Sweeps V (1V-10 V) & Measure I

Mea

sure

d C

urre

nt (

Source Voltage (V)

Acknowledgements:This work was supported primarily by the Engineering Research Center Program of the National Science Foundation and the Department of Energy under NSF Award Number EEC-1041877 and the CURENT Industry Partnership Program.

• Electrical testing of the SPAD was done using the data acquisition code for the sourcemeter. A voltage was supplied and the current was measured

• Optical testing of the SPAD was done using the data acquisition MATLAB code for the oscilloscope. The SPAD was excited by photons from daylight to generate voltage spikes. These were quenched by a 100 Ohm resistor.