Methods and devices based on brillouin selective sideband amplification

• US 6,535,328 B2
• Filed: 12/18/2000
• Issued: 03/18/2003
• Est. Priority Date: 01/14/1997
• Status: Expired due to Fees

• Current Assignee: Yao X. Steve
• Original Assignee: California Institute of Technology
• Inventors: Yao, X. Steve
• Primary Examiner(s): Moskowitz, Nelson
• Application Number:
  US09/739,926
• Publication Number:
  US 20010030796A1
• Time in Patent Office: 820 Days
• Field of Search: 359/334, 359/156, 359/187, 359/327, 250/227.11
• US Class Current: 359/334
• CPC Class Codes: H04B 10/2916 using Raman or Brillouin amplifiers

Abstract

Opto-electronic devices and techniques using Brillouin scattering to select a sideband in a modulated optical carrier signal for amplification. Two lasers respectively provide a carrier signal beam and a Brillouin pump beam which are fed into an Brillouin optical medium in opposite directions. The relative frequency separation between the lasers is adjusted to align the frequency of the backscattered Brillouin signal with a desired sideband in the carrier signal to effect a Brillouin gain on the sideband. This effect can be used to implement photonic RF signal mixing and conversion with gain, conversion from phase modulation to amplitude modulation, photonic RF frequency multiplication, optical and RF pulse generation and manipulation, and frequency-locking of lasers.

Claims

1. An opto-electronic device, comprising:

an optical modulator operable to modulate an optical signal beam at an optical carrier frequency to produce modulated signal sidebands at different sideband frequencies;

an optical medium disposed to receive said signal beam from said optical modulator and operable to produce a Brillouin scattering process in response to optical excitation; and

a pump laser operable to produce at least one pump beam at an optical pump frequency to be coupled into said optical medium to propagate in an opposite direction to said signal beam, said pump beam having a power level sufficient to cause a stimulated Brillouin scattering process in said optical medium which produces a Brillouin scattering signal in the same direction as said signal beam,

wherein said optical carrier frequency and said optical pump frequency are selected relative to each other so that said Brillouin scattering signal is at a frequency of a selected sideband in said signal beam to amplify said selected sideband.

2. The device as in claim 1, wherein said optical modulator comprises an electro-optic modulator.

3. The device as in claim 2, wherein said electro-optic modulator includes a Mach-Zehnder modulator.

4. The device as in claim 1, wherein said optical modulator comprises an optical phase modulator which produces a phase modulation on said optical signal beam.

5. The device as in claim 1, wherein said optical modulator comprises an optical amplitude modulator which produces an amplitude modulation on said optical signal beam.

6. The device as in claim 1, wherein said optical modulator is configured to modulate said optical signal beam at two different modulation frequencies to respectively produce two sets of sidebands with respect to said optical carrier frequency.

7. The device as in claim 1, further comprising a photodetector and an optical coupler, said optical coupler disposed to couple said Brillouin scattering signal and said signal beam out of said optical medium and into said optical detector.

8. The device as in claim 1, wherein said sidebands in said signal beam are produced by a phase modulation and said amplification of said selected sideband effectuates a conversion from said phase modulation to an amplitude modulation in an electrical signal produced by said photodetector.

9. The device as in claim 8, wherein said selected sideband is a multiple-order sideband caused by said phase modulation at a modulation frequency and said amplification of said selected sideband produces a frequency multiplication in said electrical signal.

10. The device as in claim 1, wherein said optical medium includes an optical fiber loop.

11. The device as in claim 1, further comprising:

a signal laser to produce said signal beam into said optical modulator;

a photodetector disposed to receive a portion of said signal beam and said Brillouin scattering signal to produce an electrical signal indicative of at least one beat signal between two signals among said sidebands and said signal beam at said carrier frequency;

an electrical signal separator connected to said photodetector to receive said electrical signal and configured to separate a low-frequency signal from said electrical signal which represents an average optical power received by said photodetector and is indicative of a frequency separation between said Brillouin scattering signal and said selected sideband; and

a control circuit connected to said signal separator to receive said low-frequency signal and configured to control a frequency of said pump laser with respect to said carrier frequency based on said low-frequency signal to maintain said frequency separation within a predetermined frequency range.

12. The device as in claim 11, further comprising:

a second pump laser to produce a second pump beam at a second pump frequency different from said pump frequency, said second pump beam coupled into said optical medium to propagate against said signal beam and having a power level sufficient to cause a stimulated Brillouin scattering process in said optical medium which produces a second Brillouin scattering signal in the same direction as said signal beam, said second Brillouin scattering signal being at a frequency to overlap a second selected sideband to produce a Brillouin amplification.

13. The device as in claim 12, further comprising:

a second photodetector disposed to receive a portion of said signal beam and said second Brillouin scattering signal to produce a second electrical signal indicative of at least one beat signal between two signals among said sidebands and said signal beam at said carrier frequency;

a second electrical signal separator connected to said second photodetector to receive said second electrical signal and configured to separate a second low-frequency signal from said second electrical signal which represents an average optical power received by said second photodetector and is indicative of a second frequency separation between said second Brillouin scattering signal and said second selected sideband; and

a second control circuit connected to said signal separator to receive said low-frequency signal and configured to control said second pump frequency with respect said carrier frequency based on said low-frequency signal to maintain said second frequency separation within a predetermined frequency range.

14. A method, comprising:

modulating a phase of an optical carrier signal at a carrier frequency to produce a modulated signal having a carrier peak at the carrier frequency and a plurality of modulation sidebands at frequencies different from the carrier frequency;

directing the modulated signal and an optical pump signal at a pump frequency different from the carrier frequency to counter propagate and spatially overlap in a Brillouin medium;

controlling a power level of the optical pump signal to produce a Brillouin scattering signal through a stimulated Brillouin process in the medium;

controlling at least one of the pump frequency and the carrier frequency to overlap a frequency of the Brillouin scattering signal with a selected modulation sideband to amplify only the selected modulation sideband; and

using a photodetector to receive the optical carrier signal and the sideband-amplified modulated signal and hence to convert the phase modulation into an amplitude modulation.

15. The method as in claim 14, further comprising using an amplitude of the sideband-amplified modulated signal to control either of the pump frequency and the carrier frequency to maintain the frequency overlap between the Brillouin scattering signal and the selected sideband.