High-repetition-rate single-photon receiver and method therefor

• US 8,796,605 B2
• Filed: 05/04/2012
• Issued: 08/05/2014
• Est. Priority Date: 05/04/2012
• Status: Active Grant

• Current Assignee: LG Innotek Company Limited (LG Corporation)
• Original Assignee: Princeton Lightwave, Inc. (Ford Motor Company)
• Inventors: Mordarski, William Paul, Itzler, Mark Allen
• Primary Examiner(s): Legasse, Jr., Francis M
• Application Number:
  US13/464,629
• Publication Number:
  US 20140027607A1
• Time in Patent Office: 823 Days
• Field of Search: 327/514, 327/584, 327/535, 398/189, 398/196, 398/206, 398/210
• US Class Current: 250/206
• CPC Class Codes: G01J 1/44 Electric circuits for command of an exposure part G03B7/02
• CPC Class Codes: H01L 31/02027 for devices working in avalanche mode

Abstract

A single-photon receiver and method for detecting a single-photon are presented. The receiver comprises a SPAD that receives a gating signal having a fundamental frequency in the 100 MHz to multiple GHz range. The receiver further comprises a two-stage frequency filter for filtering the output of the SPAD, wherein the filter has: (1) a notch filter response at the fundamental frequency; and (2) a low-pass filter response whose cutoff frequency is less than the first harmonic of the fundamental frequency. As a result, the frequency filter removes substantially all the frequency components in the SPAD output without significant degradation of the signal quality but with reduced complexity, cost, and footprint requirement relative to receivers in the prior art.

Claims

1. An apparatus comprising:

a voltage source operative to bias a single-photon avalanche diode with a gating signal that is characterized by a fundamental frequency; and

a first filter that is dimensioned and arranged to provide an output signal based on an input signal from the avalanche photodiode, the first filter having a filter response characterized by (1) a low-pass filter response having a rejection frequency that is less than twice the fundamental frequency and (2) a notch filter response centered at a center frequency, wherein the notch filter response attenuates a first frequency range that includes the fundamental frequency.

2. The apparatus of claim 1 further comprising the single-photon avalanche diode.

3. The apparatus of claim 1 wherein the fundamental frequency is controllable and the center frequency is controllable.

4. The apparatus of claim 3 wherein the rejection frequency is controllable.

5. The apparatus of claim 4 wherein each of the fundamental frequency and the center frequency is controllable over a frequency range that is equal to or greater than one octave.

6. The apparatus of claim 1 wherein the gating signal is a sinusoidal signal.

7. The apparatus of claim 1 wherein the rejection frequency is greater than or equal to approximately 1.9 times the fundamental frequency.

8. The apparatus of claim 1 wherein the width of the first frequency range is controllable.

9. An apparatus comprising:

a voltage source operative to bias a single-photon avalanche diode with a gating signal that is non-sinusoidal and is characterized by a fundamental frequency; and

a first filter that is dimensioned and arranged to provide an output signal based on an input signal from the avalanche photodiode, the first filter having a filter response characterized by (1) a low-pass filter response having a rejection frequency that is less than twice the fundamental frequency and (2) a notch filter response centered at a center frequency, wherein the notch filter response attenuates a first frequency range that includes the fundamental frequency.

10. The apparatus of claim 9 wherein each of the fundamental frequency and first frequency range is controllable, and wherein the rejection frequency is substantially fixed.

11. The apparatus of claim 9 wherein each of the fundamental frequency, first frequency range, and rejection frequency is controllable.

12. The apparatus of claim 11 wherein each of the fundamental frequency and the center frequency is controllable over a frequency range that is equal to or greater than one octave.

13. An apparatus comprising:

a single-photon avalanche diode;

a voltage source operative to bias the avalanche photodiode with a gating signal that is characterized by a fundamental frequency; and

a first filter that is dimensioned and arranged to provide an output signal based on an input signal from the single-photon detector, the first filter being characterized by a rejection threshold and a filter response that attenuates by at least the rejection threshold (1) frequencies in a first frequency range that includes the fundamental frequency and (2) all frequencies above a first frequency that is less than twice the fundamental frequency.

14. The apparatus of claim 13 wherein the gating signal is a non-sinusoidal signal and each of the fundamental frequency, the first frequency range, and the first frequency is fixed.

15. The apparatus of claim 13 wherein each of the fundamental frequency and first frequency range is controllable, and wherein the first frequency is substantially fixed.

16. The apparatus of claim 15 wherein the gating signal is a sinusoidal signal.

17. The apparatus of claim 13 wherein each of the fundamental frequency, first frequency range, and the first frequency is controllable.

18. The apparatus of claim 17 wherein the fundamental frequency is controllable over a frequency range that is equal to or greater than one octave.

19. The apparatus of claim 18 wherein the gating signal is a sinusoidal signal.

20. The apparatus of claim 13 wherein the first frequency is greater than or equal to approximately 1.9 times the fundamental frequency.

21. A method comprising:

providing a gating signal to a single-photon avalanche diode, the gating signal being characterized by a fundamental frequency; and

filtering an output signal provided by the single-photon avalanche diode with a filter having a filter response characterized by (1) a low-pass filter response that attenuates frequencies greater than a rejection frequency that is less than twice the fundamental frequency, and (2) a notch filter response that attenuates frequencies within a first frequency range that includes the fundamental frequency.

22. The method of claim 21 further comprising:

controlling the first frequency over a second frequency range; and

controlling the first frequency range.

23. The method of claim 22 further comprising controlling the rejection frequency.

24. The method of claim 23 wherein the second frequency range is equal to or greater than one octave, and wherein the first frequency range includes a center frequency that is controlled over the second frequency range.

25. The method of claim 24 wherein the gating signal is provided such that it is a sinusoidal signal.

26. The method of claim 23 wherein the gating signal is provided such that it is a sinusoidal signal.

27. The method of claim 22 wherein the output signal is filtered such that the rejection frequency is greater than or equal to approximately 1.9 times the fundamental frequency.

28. A method comprising:

providing a gating signal to a single-photon avalanche diode, the gating signal being characterized by a fundamental frequency, and the gating signal being a non-sinusoidal signal; and

filtering an output signal provided by the single-photon avalanche diode with a filter having a filter response characterized by (1) a low-pass filter response that attenuates frequencies greater than a rejection frequency that is less than twice the fundamental frequency, and (2) a notch filter response that attenuates frequencies within a first frequency range that includes the fundamental frequency.

29. The method of claim 28 further comprising:

controlling the fundamental frequency over a second frequency range; and

controlling the first frequency range.

30. The method of claim 29 further comprising controlling the rejection frequency.

31. The method of claim 30 wherein the second frequency range is equal to or greater than one octave, and wherein the first frequency range includes a center frequency that is controlled over the second frequency range.

32. The method of claim 28 further comprising:

controlling each of the fundamental frequency, a center frequency, and the rejection frequency over a second frequency range that is equal to or greater than one octave, wherein the first frequency range is centered at the center frequency.