Photonic system and method for tunable beamforming of the electric field radiated by a phased array antenna

• US 9,257,745 B2
• Filed: 12/09/2010
• Issued: 02/09/2016
• Est. Priority Date: 07/08/2010
• Status: Active Grant

• Current Assignee: Instituto de Telecomunicaes
• Original Assignee: Instituto de Telecomunicaes
• Inventors: Vidal Drummond, Miguel, Nunes Nogueira, Rogrio
• Primary Examiner(s): Phan, Dao
• Application Number:
  US13/808,996
• Publication Number:
  US 20130169483A1
• Time in Patent Office: 1,888 Days
• Field of Search: 342/368, 342/369, 342/373, 342/375, 250/227.12, 385/2, 385/3
• US Class Current: 1/1
• CPC Class Codes: H01Q 3/2676 Optically controlled phased array
• CPC Class Codes: H01Q 3/2682 Time delay steered arrays
• CPC Class Codes: H04B 10/25752 Optical arrangements for wireless networks
• CPC Class Codes: H04B 2210/006 Devices for generating or processing an RF signal by optical means

Abstract

This invention discloses a photonic system to beamform the electric field yield by a phased array antenna. The system function relies on a photonic tunable delay line, which consists on an optical Mach-Zehnder interferometer with a predefined time delay difference between arms. The time delay is tuned by adjusting the coupling ratio between the power applied to each one of the interferometer'"'"'s delay lines. Three embodiments are proposed, wherein one of them just uses a single delay line and a single monochromatic light source, independently of the quantity of the array elementary antennas.

Claims

1. A photonic system to perform tunable beamforming of an electric field radiated by a phased array antenna, the system comprising:

at least one monochromatic light source,

an electro-optic modulator, and

a 1 to N optical signal splitter, wherein each of N outputs of the 1 to N optical signal splitter is optically connected to at least one Mach-Zehnder delay interferometer, a photodetector and one of N elementary antennas that compose the phased array antenna.

2. The photonic system to perform the tunable beamforming of the electric field radiated by the phased array antenna according to claim 1,

wherein each Mach-Zehnder delay interferometer comprises an input optical coupler optically connected to at least two time delay lines with a time difference between them, which are optically connected to an output optical coupler;

and

wherein at least one of the input and output optical couplers of each Mach-Zehnder delay interferometer has a tunable coupling ratio.

3. The photonic system to perform the tunable beamforming of the electric field radiated by the phased array antenna according to claim 2,

wherein each one of the at least N Mach-Zehnder delay interferometers represents a tunable delay line;

and

wherein time delay tuning in said at least two time delay lines is performed through control of the coupling ratio of at least one of the two optical couplers.

4. The photonic system to perform the tunable beamforming of the electric field radiated by the phased array antenna according to claim 2, wherein the coupling ratio of at least one of the optical couplers of at least N Mach-Zehnder delay interferometers is controlled to permit tuning of the radiated electric field beamforming.

5. The photonic system to perform the tunable beamforming of electric field radiated by the phased array antenna according to claim 1, further comprising N variable optical attenuators placed after the outputs of the 1 to N optical splitter in order to enable controlling power of detected N optical signals.

6. A method to perform beamforming of an electric field radiated by a phased array antenna,

wherein at least one monochromatic light source is modulated by an RF signal, which is radiated using an electro-optic modulator;

and

wherein the at least one modulated signal is copied N times, where each copy is processed by at least one Mach-Zehnder delay interferometer with a tunable coupling ratio, being next converted to an electric domain through photodetection, and being then sent to the respective elementary antenna of the phased array antenna;

throughout controlling the interferometers coupling ratio, the time delay associated to each one of the N copies is varied, and therefore the beamforming of the electric field radiated by the phased array antenna is controlled.

7. The method to perform the beamforming of the electric field radiated by the phased array antenna according to claim 6, wherein a photonic system for beamforming comprises a monochromatic light source, an electro-optic modulator and N Mach-Zehnder delay interferometers with tunable coupling ratio, the method comprising:

the modulated signal is split with equal power by two propagation axes of a birefringent medium, obtaining at the output of the birefringent medium two polarization orthogonal optic signals, time delayed between each other by τ

;

the polarization orthogonal optic signals are copied N times by an 1 to N optic signal splitter;

the polarization orthogonal optic signals of each of the N copies are added using a polarizer;

the coupling ratio of each Mach-Zehnder delay interferometer, and

consequently the time delay of each copy, is tuned through the polarization controller, which is previous to the respective polarizer.

8. The method to perform the beamforming of the electric field radiated by a phased array antenna according to claim 6, wherein a photonic system for beamforming has N monochromatic light sources, multiplexed at the wavelength using a wavelength multiplexer optically connected to an electro-optic modulator which is optically connected to N Mach-Zehnder delay interferometers with tunable coupling ratio, the method comprising:

the N modulated signals are introduced into a birefringent medium;

the polarization of the N modulated signals introduced into the birefringent medium is adjusted using the polarization controllers which come after the N monochromatic sources;

at the output of the birefringent medium, each wavelength multiplexed signal is de-multiplexed using a wavelength de-multiplexer, and the orthogonally polarized signals which compose each de-multiplexed signal are added using a polarizer; and

the coupling ratio is defined by adjusting the polarization controllers which come after each monochromatic source and/or the polarization controllers which come before the polarizers.

9. The method to perform the beamforming of the electric field radiated by a phased array antenna according to claim 6, wherein a photonic system for beamforming has a monochromatic light source, an electro-optic modulator that converts the electric signal in an optic signal with single side band, and N optoelectric Mach-Zehnder delay interferometers with tunable coupling ratio, the method comprising:

the modulated signal is divided with equal power between the two propagation axes of a birefringent medium, obtaining at the output of the birefringent medium two polarization orthogonal optic signals, time delayed between each other by τ

;

the polarization orthogonal optic signals are copied N times by an 1 to N optic signal splitter;

the polarization orthogonal signals of each of the N copies are attenuated independently by an optically variable attenuator, sensitive to polarization; and

the coupling ratio, and consequently the time delay of each copy is tuned using optically variable attenuator, which is sensitive to polarization, that comes before the respective photodetector, which, in turn adds the polarization orthogonal signals detected simultaneously to the photodetection.

10. The method to perform the to perform the beamforming of the electric field radiated by a phased array antenna according to claim 6, wherein a photonic system for beamforming has N monochromatic light sources, multiplexed at wavelength using a wavelength multiplexer, optically connected to an electro-optic modulator, which converts the electric signal into an optical signal with single sideband, and in turn is optically connected to N Mach-Zehnder delay interferometers with tunable coupling ratio, the method comprising:

the modulated signals are divided with equal power between the two propagation axis of a birefringent medium, through the adjustment of the polarization controllers that come after the N monochromatic sources and through the adjustment of one polarization controller that comes before the birefringent medium;

at the output of the birefringent medium, each wavelength multiplexed signal is de-multiplexed using a wavelength de-multiplexer and the orthogonally polarized signals that compose each de-multiplexed signal are attenuated independently by an optically variable attenuator that is sensitive to polarization; and

the coupling ratio, and consequently the time delay of each copy is tuned using optically variable attenuator, which is sensitive to polarization, that comes before the respective photodetector, which, in turn adds the polarization orthogonal signals detected simultaneously to the photodetection.