Photonic RF Frequency Conversion

• US 20110150485A1
• Filed: 10/26/2010
• Published: 06/23/2011
• Est. Priority Date: 10/26/2009
• Status: Active Grant

• Current Assignee: Oewaves Incorporated
• Original Assignee: Oewaves Incorporated
• Inventors: Ilchenko, Vladimir S., Matsko, Andrey B., Seidel, David
• Granted Patent: US 8,538,270 B2
• Time in Patent Office: Days
• US Class Current: 398/115
• CPC Class Codes: G02F 2/002 using optical mixing
• CPC Class Codes: H03D 9/00 Demodulation or transference of modulation of modulated electromagnetic waves demodulating light, transferring modulation in light waves G02F2/00
• CPC Class Codes: H04B 2210/006 Devices for generating or processing an RF signal by optical means

Abstract

Devices and techniques for frequency conversion of radio frequency (RF) or microwave signals based on photonic processing.

Claims

1. A method for converting a frequency of a signal based on photonic processing, comprising:

producing a modulated optical signal that is at an optical carrier frequency and carries an input radio frequency (RF) signal;

coupling light of the modulated optical signal into an optical resonator that supports optical resonator modes and exhibits a frequency difference between two adjacent optical resonator modes that is different from an RF frequency of the input RF signal;

coupling light out of the optical resonator as an optical output signal that carries a first set of optical sidebands corresponding to the RF signal and a second set of optical sidebands corresponding to the optical resonator modes; and

using an optical detector to convert the optical output signal into an output electrical signal that is a replica of the input RF signal at an output electrical signal frequency that is shifted from the RF frequency of the input RF signal.

2. The method as in claim 1, wherein the output electrical signal frequency is down shifted from the RF frequency of the input RF signal.

3. The method as in claim 1, wherein the output electrical signal frequency is up shifted from the RF frequency of the input RF signal.

4. The method as in claim 1, comprising:

using an optical bandpass filter to filter the optical output signal out of the optical resonator to control the output electrical signal frequency that is shifted from the RF frequency of the input RF signal.

5. The method as in claim 4, wherein the optical bandpass filter is used to select a first sideband from the first set of optical sidebands corresponding to the RF signal and a second sideband from the second set of optical sidebands corresponding to the optical resonator modes to transmit through the optical bandpass filter to reach the optical detector while blocking other optical sidebands from reaching the optical detector.

6. The method as in claim 1, comprising:

using an optical notch filter to filter the optical output signal out of the optical resonator to remove light at the optical carrier frequency in the optical output signal.

7. The method as in claim 1, wherein the optical resonator is part of an opto-electronic oscillator.

8. A device for converting a frequency of a signal based on photonic processing, comprising:

an electrical to optical conversion module that receives an input radio frequency (RF) signal and produces a modulated optical signal that is at an optical carrier frequency and carries the input RF signal;

an optical resonator that supports optical resonator modes and exhibits a frequency difference between two adjacent optical resonator modes that is different from an RF frequency of the input RF signal;

an optical coupler that couples light of the modulated optical signal into the optical resonator and couples light out of the optical resonator as an optical output signal that carries a first set of optical sidebands corresponding to the RF signal and a second set of optical sidebands corresponding to the optical resonator modes; and

an optical detector located to receive the optical output signal coupled out of the optical resonator, the optical detector converting the received optical output signal into an output electrical signal that is a replica of the input RF signal at an output electrical signal frequency that is shifted from the RF frequency of the input RF signal.

9. The device as in claim 8, wherein the electrical to optical conversion module includes a laser that produces a continuous wave laser beam at the optical carrier frequency and an optical modulator that applies the input RF signal to modulate the laser beam to produce the modulated optical signal.

10. The device as in claim 8, wherein the electrical to optical conversion module includes a laser that produces a laser beam at the optical carrier frequency and applies the input RF signal to directly modulate the laser beam, without a separate optical modulator, to produce the modulated optical signal.

11. The device as in claim 8, comprising:

an optical bandpass filter located in an optical path between the optical resonator and the optical detector to filter the optical output signal out of the optical resonator to control the output electrical signal frequency that is shifted from the RF frequency of the input RF signal.

12. The device as in claim 11, wherein the optical bandpass filter is used to select a first sideband from the first set of optical sidebands corresponding to the RF signal and a second sideband from the second set of optical sidebands corresponding to the optical resonator modes to transmit through the optical bandpass filter to reach the optical detector while blocking other optical sidebands from reaching the optical detector.

13. The device as in claim 8, comprising:

an optical notch filter located in an optical path between the optical resonator and the optical detector to filter the optical output signal out of the optical resonator to remove light at the optical carrier frequency in the optical output signal.

14. The device as in claim 8, comprising:

an opto-electronic oscillator that includes a closed opto-electronic loop having an optical part that includes the optical resonator, an electrical part and a loop optical detector coupled between the optical part and the electrical part to convert light received from the optical part into an electrical signal to the electrical part.

15. The device as in claim 14, wherein the optical resonator exhibits an electro-optic effect and receives an electrical control signal from the electrical part of the closed opto-electronic loop.

16. A device for converting a frequency of a signal based on photonic processing, comprising:

an electrical to optical conversion module that receives an input radio frequency (RF) signal and produces a modulated optical signal that is at an optical carrier frequency and carries the input RF signal;

a photonic oscillator that includes a closed opto-electronic loop having an optical part that includes an optical resonator, an electrical part and a loop optical detector coupled between the optical part and the electrical part to convert light received from the optical part into an electrical signal to the electrical part, the optical resonator configured to support optical resonator modes and to exhibit a frequency difference between two adjacent optical resonator modes that is different from an RF frequency of the input RF signal;

an optical coupler that couples light of the modulated optical signal into the optical resonator and couples light out of the optical resonator as an optical output signal that carries a first set of optical sidebands corresponding to the RF signal and a second set of optical sidebands corresponding to the optical resonator modes; and

an optical detector located to receive the optical output signal coupled out of the optical resonator, the optical detector converting the received optical output signal into an output electrical signal that is a replica of the input RF signal at an output electrical signal frequency that is shifted from the RF frequency of the input RF signal.

17. The device as in claim 16, wherein the electrical to optical conversion module includes a laser which produces laser light at the optical carrier frequency and is optically coupled to the optical resonator via the optical coupler to be optically locked to an optical resonator mode via injection locking.

18. The device as in claim 16, wherein the optical resonator supports optical whispering gallery modes and the optical coupler is an evanescent optical coupler.

19. The device as in claim 18, wherein the optical resonator is made of an electro-optic crystal and structured to support optical whispering gallery modes in two orthogonally polarized transverse electric (TE) modes and transverse magnetic (TM) modes circulating near a rim of the optical resonator, and

wherein the device comprises:

electrodes formed on the optical resonator to receive an electrical signal from the electrical part in an electric field polarization oriented relative to a crystal axis of the electro-optic crystal to effectuate coupling between an optical whispering gallery mode in the TE mode and another optical whispering gallery mode in the TM mode to produce an optical single sideband on light in the optical resonator at a frequency different from the optical carrier frequency; and

a frequency control mechanism coupled to the optical resonator to tune a frequency spacing between the optical single sideband and the optical carrier frequency.

20. The device as in claim 19, comprising:

an optical polarizer located in an optical path between the optical resonator and the optical detector to reject the light at the optical carrier frequency and to transmit light of the optical single sideband.