Polarization mode dispersion compensation

• US 6,271,952 B1
• Filed: 08/18/1998
• Issued: 08/07/2001
• Est. Priority Date: 08/18/1998
• Status: Expired due to Term

• Current Assignee: RPX Clearinghouse LLC (RPX Corporation)
• Original Assignee: Nortel Networks Limited (Nortel Networks Corporation)
• Inventors: Epworth, Richard Edward
• Primary Examiner(s): NEGASH, KINFE MICHAEL
• Application Number:
  US09/135,967
• Time in Patent Office: 1,085 Days
• Field of Search: 359/161, 359/140, 359/156, 359/122, 359/130, 250/227.12, 385/37
• US Class Current: 398/147
• CPC Class Codes: H04B 10/2569 due to polarisation mode dispersion [PMD]

Abstract

Polarization mode dispersion in an optical signal transmitted through a waveguide of a communications system is compensated by separating the dispersed signal into components corresponding to principal polarization states. The components are delayed by respective delays differing by a delay increment which is controlled to correspond to the dispersion delay and the delayed components are recombined to provide a dispersion compensated optical output signal. Each of the delays is provided by an chirped Bragg reflector forming part of a delay line, the Bragg reflectors comprising optical fibres with chirped intracore index gratings. Transducers or temperature controllers acting on one of the fibres allows dimensional control of the grating periodicity such that the position of Bragg reflection is variable. Wavelength division multiplexed optical signals are compensated using sampled gratings which allow a common Bragg reflection position for each wavelength.

Claims

1. Apparatus for compensating for polarisation mode dispersion in an optical signal transmitted via an optical waveguide of an optical communications system, the apparatus comprising;

separating means operable to separate the optical signal into first and second components having a dispersion delay therebetween;

delay means operable to delay the first and second components by respective delays differing by a delay increment;

recombining means operable to recombine the delayed first and second components to form an output signal; and

control means operable to control the delay increment such that in the output signal the dispersion delay is substantially compensated by the delay increment;

wherein the delay means comprises at least one delay line having a chirped Bragg reflector extending longitudinally of the delay line, wherein said respective delay results from a time taken for said respective component to traverse the delay line to and from a reflection position at which Bragg reflection occurs, and wherein the control means is operable to variably regulate at least one parameter determining the conditions under which Bragg reflection occurs to variably define the reflection position relative to the Bragg reflector.

2. Apparatus as claimed in claim 1, wherein the parameter controlled by the control means is a characteristic of spatial periodicity as a function of position of a chirped refractive index grating formed in an optical medium of the Bragg reflector.

3. Apparatus as claimed in claim 2, wherein the control means comprises strain producing means operable to produce a variable strain in the optical medium of the Bragg reflector.

4. Apparatus as claimed in claim 3, wherein the Bragg reflector comprises an optical fibre and wherein said refractive index grating is defined in a core of the fibre constituting said optical medium.

5. Apparatus as claimed in claim 4, wherein the strain producing means comprises an actuator operable to apply variable tension to the fibre in the direction of its longitudinal extent.

6. Apparatus as claimed in claim 4, wherein the control means comprises an actuator operable to apply a variable bending moment to the fibre.

7. Apparatus as claimed in claim 2, wherein the control means comprises temperature control means operable to vary the characteristic of spatial periodicity as a function of position by thermal expansion and contraction of the optical medium.

8. Apparatus as claimed in claim 7, wherein the Bragg reflector comprises an optical fibre defining the refractive index grating and wherein the temperature control means comprises an electrically conductive surface layer of the fibre and a heater control circuit operable to maintain the fibre at a controlled temperature.

9. Apparatus as claimed in claim 2, wherein said delay means comprises first and second delay lines having respective first and second Bragg reflectors.

10. Apparatus as claimed in claim 9, wherein said first and second Bragg reflectors are constituted by respective first and second optical fibres having respective intra-core refractive index gratings.

11. Apparatus as claimed in claim 10, wherein said first and second fibres are fused together in side by side relationship and wherein said control means comprises an actuator operable to effect bending of the fused fibres such that respective periodicities of the index gratings are varied by different amounts.

12. Apparatus as claimed in claim 9, wherein said first and second Bragg reflectors define respective spatial periodicities of refractive index gratings which vary with position according to respective chirp characteristics which at least partially compensate for chromatic dispersion in the first and second components respectively.

13. Apparatus as claimed in claim 3, wherein the optical medium is constituted by a polarisation maintaining optical fibre having an intracore refractive index grating, the delay means comprising means for directing the first and second components into the polarisation maintaining fibre so as to propagate in orthogonal first and second modes.

14. Apparatus as claimed in claim 13, wherein said strain producing means comprises an actuator operable to effect bending of the fibre in a direction which varies the amount of birefringence between the first and second modes.

15. Apparatus as claimed in claim 1, wherein the separating means is operable to separate the first and second components so as to correspond substantially to principal polarisation states of the optical signal with respect to the optical waveguide in which said polarisation mode dispersion occurs.

16. Apparatus as claimed in claim 15, wherein the separating means comprises a polarisation controller receiving the optical signal, and a polarisation beam splitter receiving the output of the polarisation controller and outputting the first and second components.

17. Apparatus as claimed in claim 16 comprising, a dispersion measurement circuit operable to measure the dispersion delay between the first and second components, and a controller responsive to the measurement of dispersion delay and operable to control the polarisation controller such that the dispersion delay measurement is maximised.

18. Apparatus as claimed in claim 17, wherein the first and second components output from the polarisation beam splitter are input to respective directional couplers operable to direct the respective components into first and second delay lines, the directional couplers being further operable to direct the delayed components to the recombining means.

19. Apparatus as claimed in claim 17, wherein the input signal is directed to the polarisation controller via a directional coupler and wherein the first and second components output from the polarisation beam splitter are input to said respective delay lines, the delayed first and second components being returned via the polarisation beam splitter and polarisation controller to the directional coupler which is further operable to direct the delayed components to an output waveguide, whereby said recombining means is constituted by said polarisation beam splitter.

20. Apparatus as claimed in claim 16 comprising mesurement means responsive to the output signal form the reconbining means to provide a feedback signal representative of the effect of polarization mode dispersion in the output signal, and a controller responsive to the feedback signal to control the polarization controller and the delay means so as to minimize the measured effect of polarization mode dispersion.

21. Apparatus as claimed in claim 20 wherein the measurement means comprises a receiver operable to provide an electrical output representative of the output signal from the recombining means and a measurement circuit responsive to the electrical output to provide said feedback signal.

22. Apparatus as claimed in claim 2, wherein the spatial periodicity is a linear function of longitudinal position relative to the optical medium.

23. Apparatus as claimed in claim 2, wherein the refractive index grating comprises a chirped periodic modulation of refractive index as a function of position along the optical medium and wherein the modulation has an amplitude envelope which is modulated with respect to position such that the grating constitutes a sampled grating, whereby reflection at a common reflection position occurs for a plurality of wavelength components of the optical signal.

24. Apparatus as claimed in claim 1 wherein the parameter controlled by the control means is constituted by the values of one or more wavelengths of the optical signal, said control means comprising means for varying the values of one or more wavelengths of the optical signal transmitting via a waveguide in which the polarisation mode dispersion occurs.

25. A method of compensating for polarisation mode dispersion in an optical signal transmitted via an optical waveguide of an optical communications system, the method comprising the steps of;

separating the optical signal into first and second components having a dispersion delay therebetween;

delaying the first and second components by respective delays differing by a delay increment;

recombining the delayed first and second components to form an output signal; and

controlling the delay increment such that in the output signal the dispersion delay is substantially compensated by the delay increment;

wherein the delaying step comprises delaying at least one component by transmission via a delay line having a chirped Bragg reflector extending longitudinally of the delay line, wherein said respective delay results from a time taken for said respective component to traverse the delay line to and from a reflection position at which Bragg reflection occurs, and wherein the controlling step variably regulates at least one parameter determining the conditions under which Bragg reflection occurs to variably define the reflection position relative to the Bragg reflector.

26. A method as claimed in claim 25, wherein the parameter controlled by the controlling step is a characteristic of spatial periodicity as a function of position of a chirped refractive index grating formed in an optical medium of the Bragg reflector.

27. A method as claimed in claim 26, wherein the controlling step comprises producing a variable strain in the optical medium of the Bragg reflector.

28. A method as claimed in claim 27, wherein the Bragg reflector comprises an optical fibre and wherein said refractive index grating is defined in a core of the fibre constituting said optical medium.

29. A method as claimed in claim 28, wherein the strain is produced by an actuator applying variable tension to the fibre in the direction of its longitudinal extent.

30. A method as claimed in claim 28, wherein the controlling step comprises operating an actuator to apply a variable bending moment to the fibre.

31. A method as claimed in claim 26, wherein the controlling step comprises varying the characteristic of spatial periodicity as a function of position by thermal expansion and contraction of the optical medium.

32. A method as claimed in claim 31, wherein the Bragg reflector comprises an optical fibre defining the refractive index grating and wherein the controlling step regulates electrical current in an electrically conductive surface layer of the fibre to maintain the fibre at a controlled temperature.

33. A method as claimed in claim 26, wherein said delaying step comprises delaying the first and second components by transmission via first and second delay lines having respective first and second Bragg reflectors.

34. A method as claimed in claim 33, wherein said first and second Bragg reflectors are constituted by respective first and second optical fibres having respective intracore refractive index gratings.

35. A method as claimed in claim 34, wherein said first and second fibres are fused together in side by side relationship and wherein said controlling step operates an actuator to effect bending of the fused fibres such that respective periodicities of the index gratings are varied by different amounts.

36. A method as claimed in claim 33, wherein said first and second Bragg reflectors define respective spatial periodicities of refractive index gratings which vary with position according to respective chirp characteristics which at least partially compensate for chromatic dispersion in the first and second components respectively.

37. A method as claimed in claim 27, wherein the optical medium is constituted by a polarisation maintaining optical fibre having an intracore refractive index grating, the delaying step comprising directing the first and second components into the polarisation maintaining fibre so as to propagate in orthogonal first and second modes.

38. A method as claimed in claim 37, wherein said strain producing step comprises operating an actuator to effect bending of the fibre in a direction which varies the amount of biref ringence between the first and second modes.

39. A method as claimed in claim 25, wherein the separating step separates the first and second components so as to correspond substantially to principal polarisation states of the optical signal with respect to the optical waveguide in which said polarisation mode dispersion occurs.

40. A method as claimed in claim 39, wherein the separating step comprises operating a polarisation controller receiving the optical signal, and splitting the optical signal in a polarisation beam splitter receiving the output of the polarisation controller and outputting the first and second components.

41. A method as claimed in claim 40 comprising measuring the dispersion delay between the first and second components, and controlling the polarisation controller in response to the measurement of dispersion delay such that the dispersion delay measurement is maximised.

42. A method as claimed in claim 41, wherein the first and second components output from the polarisation beam splitter are input to respective directional couplers directing the respective components into first and second delay lines, the directional couplers further directing the delayed components to the recombining means.

43. A method as claimed in claim 41, wherein the input signal is directed to the polarisation controller via a directional coupler and wherein the first and second components output from the polarisation beam splitter are input to said respective delay lines, the delayed first and second components being returned via the polarisation beam splitter and polarisation controller to the directional coupler which further directs the delayed components to an output waveguide, whereby said recombining step is effected by said polarisation beam splitter.

44. A method as claimed in claim 40 comprising measuring the output signal from the recombining step to provide a feedback signal representative of the effect of polarization mode dispersion in the output signal, and controlling the polarization controller and the delay increment provided in said delaying step so as to minimise the measured effect of polarizatin mode dispersion.

45. A method as claimed in claim 44 wherein said measuring step comprises operating a receiver to provide an electrical output representative of the output signal from the recombining step and measuring the electrical output to provide said feedback signal.

46. A method as claimed in claim 26, wherein the spatial periodicity is a linear function of longitudinal position relative to the optical medium.

47. A method as claimed in claim 26, wherein the refractive index grating comprises a chirped periodic modulation of refractive index as a function of position along the optical medium and wherein the modulation has an amplitude envelope which is modulated with respect to position such that the grating constitutes a sampled grating, whereby reflection at a common reflection position occurs for a plurality of wavelength components of the optical signal.

48. A method as claimed in claim 25 wherein the parameter controlled by the controlling step is constituted by the values of one or more wavelengths of the optical signal, said controlling step varying the values of one or more wavelengths of the optical signal transmitted via a waveguide in which the polarisation mode dispersion occurs.

49. Delay apparatus for compensating for an unwanted delay between first and second components of an optical signal, the apparatus comprising;

first and second delay lines operable to delay the first and second components by respective delays differing by a delay increment;

recombining means operable to recombine the delayed first and second components to form an optical output signal; and

control means operable to control the delay increment such that in the output signal the dispersion delay is substantially compensated by the delay increment;

wherein at least one delay line comprises a chirped Bragg reflector extending longitudinally of the delay line, wherein said respective delay results from a time taken for said respective component to traverse the delay line to and from a reflection position at which Bragg reflection occurs, and wherein the control means is operable to variably regulate a characteristic of spatial periodicity as a function of position of a chirped refractive index grating formed in an optical medium of the Bragg reflector to thereby variably define the reflection position relative to the Bragg reflector.

50. Delay apparatus as claimed in claim 49 wherein each of the first and second delay lines comprises a respective chirped Bragg reflector and wherein the control means is operable to regulate the characteristic of spatial periodicity of only one of said delay lines.

51. Delay apparatus as claimed in claim 50 wherein said Bragg reflectors comprise respective sampled refractive index gratings.