Diffraction compensation of FBG phase masks for multi-channel sampling applications

• US 6,654,521 B2
• Filed: 01/23/2002
• Issued: 11/25/2003
• Est. Priority Date: 01/23/2002
• Status: Expired due to Term

• Current Assignee: TeraXion, Inc. (indie Semiconductor, Inc.)
• Original Assignee: TeraXion, Inc. (indie Semiconductor, Inc.)
• Inventors: Wang, Ying, Li, HongPu, Zweiback, Jason, Rothenberg, Joshua E., Sheng, Yunlong
• Primary Examiner(s): Stafira, Michael P.
• Assistant Examiner(s): VALENTIN, JUAN D
• Application Number:
  US10/056,575
• Publication Number:
  US 20030138206A1
• Time in Patent Office: 671 Days
• Field of Search: 385/37, 359/566, 654/25, 653/92, 430/290, 264/1.27
• US Class Current: 385/37
• CPC Class Codes: G02B 6/02085 characterised by the grating profile, e.g. chirped, apodised, tilted, helical
• CPC Class Codes: G02B 6/02138 based on illuminating a phase mask

Abstract

The present invention is directed to a system and method for designing efficient multi-channel FBG gratings using a pre-compensated phase mask for diffracting light for side-writing the grating on an optical fiber core. A desired phase function of the FBG is generated, specifically tailored to an effective spacing between the phase mask and the optical fiber core. From the phase function a phase mask is pre-compensated to offset diffraction effects associated with each longitudinal position of the FBG receiving light from two corresponding longitudinal positions of the phase mask substantially symmetrically spaced longitudinally relative to each particular longitudinal position of the FBG. The two corresponding longitudinal positions of the phase mask are spaced longitudinally from each other by a spacing determined by the effective spacing between the phase mask and fiber core and by the first order diffraction angle of light through the phase mask.

Claims

1. A method of designing a pre-compensated phase mask for side-writing a fiber Bragg grating (FBG) on an optical fiber core, said method comprising the steps of:

determining an effective spacing between said phase mask and said optical fiber core for said side-writing; and

calculating a phase mask design, such that a desired FBG phase function is written on said fiber core by a pattern of light diffracting from said designed phase mask through said effective spacing, said designed phase mask being pre-compensated to offset diffraction effects associated with each longitudinal position on said FBG receiving light from two corresponding longitudinal positions on said phase mask, said two corresponding longitudinal positions on said phase mask being substantially symmetrically spaced longitudinally relative to each said longitudinal position on said FBG.

2. The method of claim 1 wherein said two corresponding longitudinal positions on said phase mask are spaced longitudinally relative to each said longitudinal position on said FBG at a longitudinal shift determined by said effective spacing and a first order diffraction angle of light from said phase mask.

3. The method of claim 1 wherein said desired FBG phase function produces a multi-channel reflectance spectra having an arbitrarily selectable set of channel amplitudes.

4. The method of claim 3 wherein said multi-channel reflectance spectra contains a selectable plurality of channels having substantially uniform reflectance amplitudes.

5. The method of claim 3 wherein said multi-channel reflectance spectra contains a selectable plurality of channels having substantially zero reflectance amplitudes.

6. The method of claim 1, further comprising the step of generating said desired FBG phase function.

7. The method of claim 1 wherein the phase at said each longitudinal position on said FBG is substantially the sum of phases at said two corresponding longitudinal positions on said phase mask being substantially symmetrically spaced longitudinally relative to each said longitudinal position on said FBG.

8. The method of claim 6 wherein said step of calculating further comprises the steps of:

performing a Fourier transform of said desired FBG phase function, said Fourier transform having spatial frequency components;

multiplying each said spatial frequency component of said Fourier transform by a predetermined transfer function to obtain a phase mask phase function spectrum for said pre-compensated phase mask; and

performing an inverse Fourier transform of said phase mask phase function spectrum to obtain said designed pre-compensated phase mask phase function.

9. The method of claim 8 wherein said step of multiplying by said predetermined transfer function increases high spatial frequency components of said Fourier transform relative to low spatial frequency components of said Fourier transform.

10. The method of claim 9 wherein said predetermined transfer function has an inverse cosine spatial frequency dependence.

11. The method of claim 10 wherein said spatial frequency components are limited to frequencies appreciably below those at which said predetermined transfer function has a singularity.

12. The method of claim 10 wherein said spatial frequency components include frequencies appreciably above and below those at which said predetermined transfer function has a singularity and are limited to exclude only frequencies closely adjacent those frequencies at which said predetermined transfer function has a singularity.

13. The method of claim 6 wherein said desired FBG phase function is generated in the form of a truncated Fourier series expansion having a preselected number of terms and representing a preselected number of spatial frequency components.

14. The method of claim 13 wherein each said term of said truncated Fourier series expansion contains at least one free parameter.

15. The method of claim 14 wherein each said term of said truncated Fourier series expansion contains two free parameters.

16. The method of claim 14 further comprising the steps of:

applying an optimization algorithm to said truncated Fourier series expansion to evaluate said at least one free parameter, such that said truncated Fourier series expansion is optimized;

evaluating said truncated Fourier series expansion for the value of said at least one free parameter that results from applying said optimization algorithm; and

multiplying each term of said evaluated truncated Fourier series expansion by a predetermined transfer function to obtain an optimized phase function for said pre-compensated phase mask.

17. The method of claim 16 wherein said step of multiplying by said predetermined transfer function increases high spatial frequency components of said truncated Fourier series expansion relative to low spatial frequency components of said truncated Fourier series expansion.

18. The method of claim 17 wherein said predetermined transfer function has an inverse cosine spatial frequency dependence.

19. The method of claim 16 further comprising the step of varying said preselected number of terms of said truncated Fourier series expansion.

20. The method of claim 16 wherein said optimization algorithm is a nonlinear optimization procedure.

21. The method of claim 20 wherein said nonlinear optimization procedure is selected from the group consisting of simulated thermal annealing nonlinear optimization procedures, simplex method, Powell'"'"'s method, conjugate gradient method, variable metric method, linear programming methods, and Dammann optimization procedures.

22. The method of claim 1 further comprising the steps of:

generating an initial mask phase function in the form of a truncated Fourier series expansion having a preselected number of terms containing at least one free parameter and representing at least one spatial frequency component;

calculating an initial FBG index variation from the intensity of said pattern of light diffracted from said designed phase mask;

performing a transform of said FBG index variation to obtain an initial spectral reflectivity envelope; and

applying an optimization algorithm to said transformed FBG index variation to evaluate said at least one free parameter, such that said FBG spectral reflectivity envelope is optimized.

23. The method of claim 22 wherein said step of calculating is performed using a procedure selected from the group consisting of angular plane wave spectrum, scalar diffraction, and finite difference in time domain vector diffraction.

24. The method of claim 22 wherein said step of performing a transform is performed using a procedure selected from the group consisting of Fourier transforms and transfer matrices.

25. The method of claim 22 wherein said optimization algorithm is a nonlinear optimization procedure.

26. The method of claim 25 wherein said nonlinear optimization procedure is selected from the group consisting of simulated thermal annealing nonlinear optimization procedures, simplex method, Powell'"'"'s method, conjugate gradient method, variable metric method, linear programming methods, and Dammann optimization procedures.

27. The method of claim 2 wherein said step of calculating further comprises the step of generating said desired FBG phase function, wherein a preliminary phase mask design includes at least one discontinuous π

/2 phase shift.

28. The method of claim 27 wherein said step of calculating further comprises:

replacing each of said at least one discontinuous π

/2 phase shift in said phase mask design with a pair of π

/2 phase shifts in said FBG design, said pair of π

/2 phase shifts having a longitudinal separation equal to said longitudinal shift;

replacing consecutive +π

/2 phase shift pairs in said FBG design with alternating +π

/2 and −

π

/2 phase shift pairs in said FBG design; and

generating a channel spectrum of said desired FBG phase function incorporating said replacement phase shift pairs.

29. The method of claim 28 further comprising the step of applying an optimization algorithm to said channel spectrum to determine the optimum longitudinal positioning of said replacement phase shift pairs, such that said longitudinal separation between said phase shifts within a pair is maintained and such that said channel spectrum is optimized.

30. The method of claim 29 further comprising the step of calculating said designed mask phase function from the location of said ±

π

/2 phase shift pairs of said optimized FBG phase function, such that each said ±

π

/2 FBG phase shift pair having said longitudinal separation is incorporated in said designed mask phase function as a single ±

π

/2 phase shift, said single ±

π

/2 phase shift being located symmetrically half-way between said paired ±

π

/2 FBG phase shifts.

31. The method of claim 30 wherein said optimization algorithm is a nonlinear optimization procedure.

32. The method of claim 31 wherein said nonlinear optimization procedure is selected from the group consisting of simulated thermal annealing nonlinear optimization procedures, simplex method, Powell'"'"'s method, conjugate gradient method, variable metric method, linear programming methods, and Dammann optimization procedures.

33. A phase mask operable to side-write a fiber Bragg grating (FBG) on an optical fiber core by a pattern of light diffracting from said phase mask through an effective spacing to said fiber core, said phase mask being pre-compensated to offset diffraction effects associated with each longitudinal position of said FBG receiving said light in said pattern from two corresponding positions of said phase mask, said two corresponding longitudinal positions of said phase mask being substantially symmetrically spaced longitudinally relative to each said longitudinal position of said FBG, wherein said FBG is operable to generate a channel spectrum.

34. The phase mask of claim 33 wherein said pre-compensation includes increasing high spatial frequency components relative to low spatial frequency components in the phase function of said phase mask using a predetermined transfer function.

35. The phase mask of claim 34 wherein said predetermined transfer function has an inverse cosine spatial frequency dependence.

36. The phase mask of claim 35 wherein said spatial frequency components in said predetermined transfer function are limited to frequencies appreciably below those at which said predetermined transfer function has a singularity.

37. The phase mask of claim 35 wherein said spatial frequency components in said predetermined transfer function include frequencies appreciably above and below those at which said predetermined transfer function has a singularity and are limited to exclude only frequencies closely adjacent those frequencies at which said predetermined transfer function has a singularity.

38. The phase mask of claim 33 wherein said two corresponding longitudinal positions of said phase mask are spaced longitudinally relative to each said longitudinal position of said FBG with a longitudinal spacing determined by said effective spacing and by a first order diffraction angle of light through said phase mask.

39. The phase mask of claim 38 wherein a preliminary design of said phase mask comprises at least one discontinuous π

/2 phase shift.

40. The phase mask of claim 39 wherein said at least one discontinuous π

/2 phase shift in said preliminary phase mask design is replaced in said FBG with a π

/2 phase shift pair, each said π

/2 phase shift pair maintaining a longitudinal separation equal to said longitudinal shift, and wherein consecutive +π

/2 phase shift pairs are replaced with alternating +π

/2 and −

π

/2 phase shift pairs.

41. The phase mask of claim 40 wherein the longitudinal positioning of said replacement phase shifts is optimized, such that said channel spectrum is optimized.

42. The phase mask of claim 41 wherein each of said optimized ±

π

/2 FBG phase shift pairs separated by said longitudinal shift is incorporated in said phase mask phase function as a single ±

π

/2 phase shift, said π

/2 phase shift in said phase mask located symmetrically half-way between said pair of said ±

π

/2 FBG phase shifts.

43. The phase mask of claim 33 further operable to generate a multi-channel FBG reflectance spectra.

44. A method of side-writing a fiber Bragg grating (FBG) on an optical fiber core, said method comprising the steps of:

positioning a phase mask substantially parallel to and at an effective spacing relative to said optical fiber core; and

diffracting light from said phase mask through said effective spacing to said optical fiber core to create a desired FBG phase function, such that each longitudinal position of said fiber core receives light from two corresponding longitudinal positions of said phase mask, said two corresponding positions of said phase mask being substantially symmetrically spaced longitudinally relative to each said longitudinal position of said fiber core, said phase mask being pre-compensated to offset diffraction effects associated with each longitudinal position of said FBG receiving said light in said pattern from two corresponding longitudinal positions of said phase mask, said two corresponding longitudinal positions of said phase mask being substantially symmetrically spaced longitudinally relative to each said longitudinal position of said fiber core.

45. The method of claim 44 wherein said two corresponding longitudinal positions of said phase mask are spaced longitudinally relative to each said longitudinal position of said FBG with a longitudinal shift determined by said effective spacing and a first order diffraction angle of light from said phase mask.

46. The method of claim 44 wherein said desired FBG phase function produces a multi-channel reflectance spectra having an arbitrarily selectable set of channel amplitudes.

47. The method of claim 46 wherein said multi-channel reflectance spectra contains a selectable plurality of channels having substantially uniform reflectance amplitudes.

48. The method of claim 46 wherein said multi-channel reflectance spectra contains a selectable plurality of channels having substantially zero reflectance amplitudes.

49. The method of claim 44 wherein the phase at said each longitudinal position on said FBG is substantially the sum of phases at said two corresponding longitudinal positions on said phase mask being substantially symmetrically spaced longitudinally relative to each said longitudinal position on said FBG.

50. The method of claim 44 wherein said pre-compensating of said phase mask comprises the steps of:

performing a Fourier transform of said desired FBG phase function;

multiplying each spatial frequency component of said Fourier transform by a predetermined transfer function to obtain a spectrum of phase mask phase function for said pre-compensated phase mask; and

performing an inverse Fourier transform of said phase mask phase function spectrum to obtain said pre-compensated phase mask phase function design.

51. The method of claim 50 wherein said step of multiplying by said predetermined transfer function increases high spatial frequency components of said Fourier transform relative to low spatial frequency components of said Fourier transform.

52. The method of claim 51 wherein said predetermined transfer function has an inverse cosine spatial frequency dependence.

53. The method of claim 52 wherein said spatial frequency components are limited to frequencies appreciably below those at which said predetermined transfer function has a singularity.

54. The method of claim 52 wherein said spatial frequency components include frequencies appreciably above and below those at which said predetermined transfer function has a singularity and are limited to exclude only frequencies closely adjacent those frequencies at which said predetermined transfer function has a singularity.

55. The method of claim 44 wherein said desired phase function is generated in the form of a truncated Fourier series expansion having a preselected number of terms.

56. The method of claim 55 wherein each term of said truncated Fourier series expansion contains at least one free parameter.

57. The method of claim 56 wherein each said term of said truncated Fourier series expansion contains two free parameters.

58. The method of claim 56 further comprising the steps of:

performing a Fourier transform of said truncated Fourier series expansion to generate a channel spectrum, said channel spectrum containing a plurality of free parameters;

applying an optimization algorithm to said channel spectrum to evaluate said plurality of free parameters, such that said channel spectrum is optimized;

evaluating said truncated Fourier series expansion for values of said plurality of free parameters that result from applying said optimization algorithm; and

multiplying each term of said evaluated Fourier series expansion by a predetermined transfer function to obtain an optimized phase function for said pre-compensated phase mask.

59. The method of claim 58 wherein said step of multiplying by said predetermined transfer function increases high spatial frequency components of said truncated Fourier series expansion relative to low spatial frequency components of said evaluated Fourier series expansion.

60. The method of claim 59 wherein said predetermined transfer function has an inverse cosine spatial frequency dependence.

61. The method of claim 58 further comprising the step of varying said preselected number of terms of said truncated Fourier series expansion.

62. The method of claim 58 wherein said optimization algorithm is a nonlinear optimization procedure.

63. The method of claim 62 wherein said nonlinear optimization procedure is selected from the group consisting of simulated thermal annealing nonlinear optimization procedures, simplex method, Powell'"'"'s method, conjugate gradient method, variable metric method, linear programming methods, and Dammann optimization procedures.

64. The method of claim 45 wherein said desired FBG phase function is calculated from a preliminary phase mask design that includes at least one discontinuous π

/2 phase shift.

65. The method of claim 64 further comprising the steps of:

replacing each of said at least one discontinuous π

/2 phase shift in said preliminary phase mask design with two π

/2 phase shifts in said FBG design, with said two π

/2 phase shifts having a longitudinal separation equal to said longitudinal shift;

replacing consecutive +π

/2 phase shift pairs in said FBG design with alternating +π

/2 and −

π

/2 phase shift pairs in said FBG design;

generating a channel spectrum of said desired FBG phase function incorporating said replacement phase shift pairs; and

applying an optimization algorithm to said channel spectrum to determine the longitudinal positioning of said replacement phase shift pairs, such that said longitudinal separation between said phase shifts within said phase shift pair is maintained and such that said channel spectrum is optimized.

66. The method of claim 65 further comprising the step of calculating said designed mask phase function from the location of said ±

π

/2 phase shift pairs of said optimized FBG phase function, such that each said ±

π

/2 FBG phase shift pair having said longitudinal separation between said phase shifts within said pair is incorporated in said designed mask phase function as a single ±

π

/2 phase shift, said single ±

n/2 phase shift being located symmetrically half-way between said paired ±

π

/2 FBG phase shifts.

67. The method of claim 65 wherein said optimization algorithm is a nonlinear optimization procedure.

68. The method of claim 67 wherein said nonlinear optimization procedure is selected from the group consisting of simulated thermal annealing nonlinear optimization procedures, simplex method, Powell'"'"'s method, conjugate gradient method, variable metric method, linear programming methods, and Dammann optimization procedures.

69. The method of claim 44 wherein said pre-compensating of said phase mask comprises the steps of:

generating an initial mask phase function in the form of a truncated Fourier series expansion having a preselected number of terms containing at least one free parameter and representing at least one spatial frequency component;

calculating an initial FBG index variation from the diffracted intensity of said phase mask;

performing a transform of said FBG index variation to obtain a spectral reflectivity envelope; and

applying an optimization algorithm to said transformed FBG index variation to evaluate said at least one free parameter, such that said FBG spectral reflectivity envelope is optimized.

70. The method of claim 69 wherein said step of calculating is performed using a procedure selected from the group consisting of angular plane wave spectrum, scalar diffraction, and finite difference in time domain vector diffraction.

71. The method of claim 69 wherein said step of performing a transform is performed using a procedure selected from the group consisting of Fourier transforms and transfer matrices.

72. The method of claim 69 wherein said optimization algorithm is a nonlinear optimization procedure.

73. The method of claim 72 wherein said nonlinear optimization procedure is selected from the group consisting of simulated thermal annealing nonlinear optimization procedures, simplex method, Powell'"'"'s method, conjugate gradient method, variable metric method, linear programming methods, and Dammann optimization procedures.