Balanced Optical-Radiofrequency Phase Detector

• US 20080024787A1
• Filed: 12/11/2006
• Published: 01/31/2008
• Est. Priority Date: 12/09/2005
• Status: Active Grant

• Current Assignee: Massachusetts Institute of Technology
• Original Assignee: Massachusetts Institute of Technology
• Inventors: Kaertner, Franz, Kim, Jung-Won
• Granted Patent: US 7,397,567 B2
• Time in Patent Office: Days
• US Class Current: 356/460
• CPC Class Codes: G01J 9/02 by interferometric methods using interferometers for measuring optically the linear dimensions of objects G01B9/02
• CPC Class Codes: G01J 9/04 by beating two waves of a same source but of different frequency and measuring the phase shift of the lower frequency obtained
• CPC Class Codes: G02F 1/0123 Circuits for the control or stabilisation of the bias voltage, e.g. automatic bias control [ABC] feedback loops
• CPC Class Codes: G04G 7/00 Synchronisation radio-controlled time-pieces G04R
• CPC Class Codes: H01S 3/1304 by using an active reference, e.g. second laser, klystron or other standard frequency source H01S3/139 takes precedence; automatic control of electronic generators H03L7/00
• CPC Class Codes: H01S 3/2383 Parallel arrangements

Abstract

A balanced optical-RF phase detector for the extraction of low-jitter radiofrequency (RF) signals from optical pulse trains is demonstrated. The extraction of the low-jitter radiofrequency signals is based on the precise phase detection by use of a differentially biased Sagnac-loop interferometer and synchronous detection. The phase-error signal from this balanced optical-RF phase detector, which is robust against drifts and photodetector nonlinearities, is used to regenerate low-jitter radiofrequency signals from optical pulse trains. Alternatively, the phase-error signal is used to generate a low-jitter optical pulse train, synchronized with a master radiofrequency signal or to synchronize multiple modelocked lasers with each other.

Claims

1. A method for optical-radiofrequency phase detection, the method comprising:

a) generating an optical pulse train;

b) generating a radiofrequency electrical signal;

c) detecting a portion of the optical pulse train and generating a first synchronous electrical detection signal;

d) directing a second portion of the optical pulse train into a differentially biased Sagnac-loop interferometer;

e) modulating the phase of the second portion of the optical pulse train in the differentially biased Sagnac-loop interferometer as a function of the frequency of the radiofrequency electrical signal;

f) detecting an amplitude-modulated output of the Sagnac-loop interferometer and generating a second synchronous electrical detection signal; and

g) synchronously detecting the second electrical detection signal with the help of the first electrical detection signal and generating a phase-error electrical signal having an amplitude proportional to the phase difference between the optical pulse train and zero-amplitude crossings of the radiofrequency electrical signal.

2. The method of claim 1, further comprising:

h) using the phase-error electrical signal to govern an oscillator in generating the radiofrequency electrical signal; and

i) using a portion of the radiofrequency electrical signal to govern the modulation of the phase of the optical pulse train in the differentially biased Sagnac-loop interferometer.

3. The method of claim 2, wherein steps (a)-(i) are performed in a master apparatus;

the method further comprising;

j) delivering a second portion of the radiofrequency electrical signal to a slave apparatus;

k) repeating steps (a)-(g) in the slave apparatus, wherein the radiofrequency electrical signal used in step (b) in the slave apparatus is the second portion of the radiofrequency electrical signal in the first apparatus;

l) using the radiofrequency electrical signal to govern the modulation of the phase of the second portion of the optical pulse train in the differentially biased Sagnac-loop interferometer in the slave apparatus; and

m) using the phase-error electrical signal generated in the slave apparatus to govern a mode-locked laser in generating the optical pulse train in the slave apparatus.

4. The method of claim 1, further comprising:

h) using the radiofrequency electrical signal to govern the modulation of the phase of the second portion of the optical pulse train in the differentially biased Sagnac-loop interferometer; and

i) using the phase-error electrical signal to govern a mode-locked laser in generating the optical pulse train.

24. The method of claim 1, wherein the steps are performed in an integrated electronic-photonic integrated circuit.

25. The method of claim 24, further comprising utilizing the electronic-photonic integrated circuit for optical clock distribution on electronic chips or boards.

5. An apparatus for synchronizing an optical pulse train and a radiofrequency electrical signal comprising:

a) a mode-locked laser for generating the optical pulse train;

b) an oscillator for generating the radiofrequency electrical signal; and

c) a balanced optical-radiofrequency phase detector comprising;

i) an oscillator for generating a radiofrequency electrical signal;

ii) a first optical coupler positioned and configured to split the optical pulse train from the mode-locked laser into a first and second portion of the optical pulse train;

iii) a first detector positioned and configured to receive the first portion of the optical pulse train and to generate a first electrical detection signal in response;

iv) a Sagnac-loop interferometer;

v) a second optical coupler positioned and configured to direct the second portion of the optical pulse train into the Sagnac-loop interferometer;

vi) a phase modulator mounted in the Sagnac-loop interferometer for modulating the phase of the second portion of the optical pulse train;

vii) a second detector positioned and configured to receive the second portion of the optical pulse train emitted from the Sagnac-loop interferometer and to generate a second electrical detection signal in response; and

viii) a double-balanced mixer positioned and configured to receive the first and second electrical detection signal and to generate a phase-error electrical signal that is a function of the comparison.

6. The apparatus of claim 5, wherein the oscillator is positioned and configured to receive the phase-error electrical signal from the double-balanced mixer and to adjust the frequency of the generated radiofrequency electrical signal as a function of the voltage of the phase-error electrical signal.

7. The apparatus of claim 6, wherein the phase modulator is positioned and configured to receive the radiofrequency electrical signal and to modulate the phase of the second portion of the optical pulse train in the Sagnac-loop interferometer.

8. The apparatus of claim 5, wherein the mode-locked laser is positioned and configured to receive the phase-error electrical signal from the double-balanced mixer and to adjust the frequency of the generated optical pulse train as a function of the voltage of the phase-error electrical signal.

9. The apparatus of claim 5, further comprising optical fiber joining:

the mode-locked laser with the first optical coupler;

the first optical coupler with the first detector;

the first optical coupler with the second optical coupler; and

the second optical coupler with the second detector.

10. The apparatus of claim 9, wherein the Sagnac-loop interferometer comprises optical fiber.

11. The apparatus of claim 5, further comprising:

a first electrically conductive pathway electrically coupled with the first detector; and

a second electrically conductive pathway electrically coupled with the first detector.

12. The apparatus of claim 11, further comprising a frequency divider in the first electrically conductive pathway.

13. The apparatus of claim 12, where the frequency divider is configured to divide the frequency of the electrical detection signal in half.

14. The apparatus of claim 12, further comprising a band-pass filter in the first electrically conductive pathway between the frequency divider and the first detector.

15. The apparatus of claim 14, wherein the band-pass filter in the first electrically conductive pathway is configured to pass a frequency at the fundamental repetition rate of the mode-locked laser and to block other frequencies.

16. The apparatus of claim 12, further comprising a band-pass filter in the second electrically conductive pathway.

17. The apparatus of claim 16, wherein the band-pass filter in the second electrically conductive pathway is configured to pass a frequency at an integer multiple of the fundamental repetition rate of the mode-locked laser and to block other frequencies.

18. The apparatus of claim 12, further comprising a frequency mixer electrically coupled with the first and second electrically conductive pathways, wherein the frequency mixer is configured to produce an electrical signal having a frequency that is the sum of the frequencies of the electrical signals received from the first and second electrically conductive pathways.

19. The apparatus of claim 18, further comprising an electrically conductive pathway from the frequency mixer to the phase modulator and further comprising a phase shifter in that electrically conductive pathway.

20. The apparatus of claim 19, further comprising a radiofrequency combiner in the electrically conductive pathway from the frequency mixer to the phase modulator, wherein the radiofrequency mixer is also electrically coupled with the oscillator that generates the radiofrequency frequency electrical signal.

21. The apparatus of claim 5, wherein the second optical coupler is configured to split the second portion of the optical pulse train into a pair of counter-propagating optical signals in the Sagnac-loop interferometer.

22. The apparatus of claim 21, wherein the phase modulator is located at a position in the Sagnac-loop interferometer where an optical delay between the counter-propagating pulses is set to Δ

t_delay=1/(2×

10.5 f_R) .

23. The apparatus of claim 5, wherein the balanced optical-radiofrequency phase detector is in the form of an integrated electronic-photonic integrated circuit.