Optical spectrum analysis using optical interferometry

• US 7,693,419 B1
• Filed: 11/22/2006
• Issued: 04/06/2010
• Est. Priority Date: 11/23/2005
• Status: Active Grant

• Current Assignee: Luna Innovations, Inc.
• Original Assignee: General Photonics Corporation (General Cable Corporation)
• Inventors: Chen, Xiaojun, Yan, Lianshan, Yao, X. Steve
• Primary Examiner(s): Vanderpuye; Ken N
• Assistant Examiner(s): Dobson; Daniel G
• Application Number:
  US11/562,961
• Time in Patent Office: 1,231 Days
• Field of Search: 359/583, 359/584, 356/451, 356/452, 356/453, 356/477, 398/25, 398/34, 398/202, 398/212, 398/213, 398/214
• US Class Current: 398/25
• CPC Class Codes: H04B 10/07955 Monitoring or measuring power
• CPC Class Codes: H04B 10/07957 Monitoring or measuring wavelength

Abstract

Techniques and devices that use polarization rotation and optical interferometry to provide optical spectrum analysis of an optical signal.

Claims

1. A method for operating the an optical spectrum analyzer which comprises:

an optical input port to receive an optical input signal;

an optical output port to output an optical output signal;

an optical coupler which receives the optical input signal and splits the received optical input signal into a first optical input signal and a second optical input signal;

a first optical path to receive the first optical input signal and to reflect the first optical input signal back to the optical coupler as a first reflected signal, wherein the first optical path comprises a first optical reflector which includes a first mirror and a first nonreciprocal polarization rotator to produce the first reflected signal;

a second optical path to receive the second optical input signal and to reflect the first optical input signal back to the optical coupler as a second reflected signal wherein the second optical path comprises a second optical reflector which includes a second mirror and a second nonreciprocal polarization rotator to produce the second reflected signal wherein the optical coupler receives and mixes the first and the second reflected signals to produce an interference signal as the optical output signal;

a control unit to control a relative optical path difference between the first and the second optical paths;

an optical detector to receive the output optical signal and to convert the received optical output signal into an electronic signal; and

a processing unit that applies a Fast Fourier Transform to the electronic signal to extract spectral information from the optical output signal to obtain spectral information of the optical input signal the method comprising;

operating the control unit to scan the relative optical path difference between the first and the second optical paths;

controlling the first and the second polarization rotators to produce a positive rotation angle in polarization of light in both the first and the second polarization rotators to obtain a first measurement of the electronic signal from the optical detector;

controlling (1) the first polarization rotator to produce the positive rotation angle in polarization of light and (2) the second polarization rotator to produce a negative rotation angle in polarization of light that is equal in magnitude to the positive rotation angle and is opposite in direction of rotation to obtain a second measurement of the electronic signal from the optical detector;

controlling the first and the second polarization rotators to produce the negative rotation angle in polarization of light in both the first and the second polarization rotators to obtain a third measurement of the electronic signal from the optical detector;

controlling (1) the first polarization rotator to produce the negative rotation angle in polarization of light and (2) the second polarization rotator to produce the positive rotation angle in polarization of light to obtain a fourth measurement of the electronic signal from the optical detector; and

operating the processing unit to produce a combination measurement signal that is equal to a difference between (1) a sum of the first and third measurements and (2) a sum of the second and the fourth measurements and to process the combination measurement signal in extracting the spectral information of the optical input signal.

2. The method as in claim 1, further comprising:

calibrating the electronic signal from the detector to account for a power variation in the device.

3. The method as in claim 1, further comprising performing a fast Fourier Transform (FFT) on the combination measurement signal in extracting the spectral information of the optical input signal.

4. The method as in claim 1, comprising using a Faraday rotator to implement each of the first and second nonreciprocal polarization rotators.

5. The method as in claim 4, wherein the Faraday rotator comprises an optical material that exhibits an magneto-optic effect and a conductor coil surrounding the optical material.

6. The method as in claim 4, wherein the Faraday rotator further comprises a permanent magnetic cylinder placed between the optical material and the conductor coil.

7. The method as in claim 1, comprising using a fiber stretcher in the control unit to control the relative optical path difference.

8. The method as in claim 1, comprising using an optical delay line as part of the control unit to control the relative optical path difference.

9. The method as in claim 1, further comprising:

using an optical coupler in one of the first and second optical paths to split a fraction of light in two directions to produce two optical monitor signals; and

using first and second optical detectors to covert the two optical monitor signals into two detector signals; and

operating the processing unit to receive the two detector signals and processes the two detector signals to calibrate a power variation in light in the first and second optical paths in extracting the spectral information.

10. The method as in claim 1, wherein the optical input port is a first fiber, the optical output port is a second fiber, the first optical path is a third fiber and the second optical path is a fourth fiber;

and

wherein the optical coupler is a fiber coupler that is coupled to the first, the second, the third and the fourth fibers.

11. The method as in claim 1, comprising:

operating the processing unit to perform a fast Fourier Transform (FFT) on the electronic signal.

12. The method as in claim 1, comprising:

operating the processing unit to control the first and the second polarization rotators to change polarization rotations produced by the first and the second polarization rotators.

13. The method as in claim 1, comprising:

in processing the combination measurement signal in extracting the spectral information of the optical input signal, performing a processing to calibrate a wavelength-dependent effect on the spectral information caused by one or more optical components in the optical spectrum analyzer.

14. The method as in claim 13, wherein the processing to calibrate the wavelength-dependent effect includes a wavelength dependence of rotation angle of at least one of the first and second nonreciprocal polarization rotators.

15. The method as in claim 13, wherein the processing to calibrate the wavelength-dependent effect includes a wavelength dependence loss of an optical delay line in the optical spectrum analyzer.

16. The method as in claim 13, wherein the processing to calibrate the wavelength-dependent effect includes a wavelength dependence of an optical coupler in the optical spectrum analyzer.

17. The method as in claim 13, wherein the processing to calibrate the wavelength-dependent effect includes a wavelength dependence in response of the optical detector in the optical spectrum analyzer.