METHODS AND SYSTEMS FOR POLARIZATION CONTROL AND POLARIZATION MODE DISPERSION COMPENSATION FOR WIDEBAND OPTICAL SIGNALS

• US 20080212980A1
• Filed: 03/28/2008
• Published: 09/04/2008
• Est. Priority Date: 05/24/2000
• Status: Active Grant

• Current Assignee: Purdue Research Foundation (Purdue University)
• Original Assignee: Purdue Research Foundation (Purdue University)
• Inventors: Weiner, Andrew M.
• Granted Patent: US 7,689,125 B2
• Time in Patent Office: Days
• US Class Current: 398/184
• CPC Class Codes: H04B 10/2569 due to polarisation mode dispersion [PMD]

Abstract

An optical processing method includes: receiving an optical signal from an optical system, wherein the optical signal is distorted by frequency-dependent polarization effects in the optical system; spatially dispersing frequency components of the distorted optical signal on a spatial light modulator (SLM); and independently adjusting the polarization transfer matrix of multiple regions of the SLM to reduce the distortion of the optical signal. A related optical processing method includes: providing a precompensation signal indicative of frequency-dependent polarization effects in a downstream optical system; spatially dispersing frequency components of an optical signal on a spatial light modulator (SLM); and independently adjusting the polarization transfer matrix of multiple regions of the SLM to at least partially precompensate the optical signal for distortions caused by the frequency-dependent polarization effects in the downstream optical system. Another related optical processing method includes: providing a model of the frequency-dependent polarization effects; spatially dispersing frequency components of the optical signal on a spatial light modulator (SLM); and independently adjusting the polarization transfer matrix of multiple regions of the SLM based on the model to emulate the optical signal transmission.

Claims

1. A method for representing transmission of an optical signal through an optical system having frequency-dependent polarization effects, the method comprising:

providing a model of the frequency-dependent polarization effects, wherein the frequency-dependent polarization effects cause wavelength dependent changes in the state of polarization (SOP) of the optical signal;

spatially dispersing frequency components of the optical signal on at least one spatial light modulator (SLM); and

independently adjusting the polarization transfer matrix of multiple regions of the at least one SLM based on the model to represent the optical signal transmission.

2. The method of claim 1, wherein the frequency-dependent polarization effects include polarization mode dispersion (PMD) effects.

3. The method of claim 2, wherein the polarization mode dispersion effects can be represented by a frequency-dependent polarization transfer matrix characterized by a frequency-dependent differential delay and principal states of polarization.

4. The method of claim 2, wherein the model of the PMD effects is a statistical model comprising a statistical representation of PMD effects in the optical system that differs from the statistics of an optical fiber having PMD.

5. The method of claim 2, wherein the model of the PMD effects is a statistical model comprising a statistical representation of PMD effects in the optical system that is similar to the statistics of an optical fiber having PMD.

6. The method of claim 1, wherein the optical signal comprises multiple signals on separate wavelength bands.

7. The method of claim 1, further comprising recombining the spatially dispersed frequency components following the adjustments by the at least one spatial light modulator.

8. The method of claim 1, wherein the spatial dispersion of the frequency components comprises using a grating, a prism, an arrayed waveguide grating, or a virtually imaged phase array.

9. The method of claim 1, wherein the at least one spatial light modulator comprises at least one liquid crystal layer.

10. The method of claim 9, wherein the at least one spatial light modulator comprises at least two liquid crystal (LC) layers, wherein the LC molecules in each of the LC layers are oriented along an axis, and wherein the axis for one of the LC layers is different from the axis of another of the LC layers.

11. The method of claim 10, wherein the axes differ from one another by an absolute amount of about 45 degrees.

12. The method of claim 11, wherein the absolute amount is in the range of 42 degrees to 48 degrees.

13. The method of claim 10, wherein the at least one spatial light modulator comprises at least three layers.

14. The method of claim 13, wherein the orientation axis of a first of the LC layers differs from the orientation axis of a second of the LC layers by absolute amount of about 45 degrees, and wherein the orientation of the second of the LC layers differs from the orientation axis of a third of the LC layers by an absolute amount of about 45 degrees.

15. The method of claim 1, wherein the adjustments to the polarization transfer matrix are selected to cause an adjustment to at least one of the phase, state of polarization (SOP), and amplitude of each of multiple subsets of the spatially dispersed frequency components.

16. The method of claim 1, wherein the adjustments to the polarization transfer matrix are selected to cause an adjustment to at least one of the phase and the state of polarization (SOP) of each of multiple subsets of the spatially dispersed frequency components.

17. The method of claim 1, wherein the adjustments to the polarization transfer matrix are selected to cause an adjustment to the state of polarization (SOP) of each of multiple subsets of the spatially dispersed frequency components.

18. The method of claim 1, wherein the adjustments to the polarization transfer matrix are selected to cause independent adjustments to the phase and the state of polarization (SOP) of each of multiple subsets of the spatially dispersed frequency components.

19. The method of claim 1, wherein the adjustments are selected to independently delay a selected polarization component of each of multiple subsets of the spatially dispersed frequency components.

20. The method of claim 1, wherein the model of the PMD effects comprises a non-statistical model of PMD effects in the optical system that differs from PMD effects in an optical fiber.

21. The method of claim 1, wherein the model of the PMD effects comprises a non-statistical model of PMD effects in the optical system that is similar to PMD effects in an optical fiber.

22. An optical system for representing transmission of an optical signal through a device having frequency-dependent polarization effects, the optical system comprising:

a dispersive module positioned to receive the optical signal and spatially separate frequency components of the optical signal;

at least one spatial light modulator (SLM) having multiple regions with an independently adjustable polarization transfer matrix, the at least one SLM positioned to receive the spatially separated frequency components on the multiple regions; and

a controller coupled to the at least one SLM,

wherein during operation the controller causes the at least one SLM to independently adjust the polarization transfer matrix of the multiple regions to represent the optical signal transmission based on a model of the frequency-dependent polarization effects, and

wherein the frequency-dependent polarization effects cause wavelength dependent changes in the state of polarization (SOP) of the optical signal.

23. The system of claim 22, wherein the optical system is a PMD emulator and the model is a statistical model comprising a statistical representation of PMD effects in the device.

24. The system of claim 22, wherein the optical system is a PMD source and the model is a non-statistical model comprising a non-statistical representation of PMD effects in the device.