IP Library Granted Patent US 7,149,384
Granted Patent B2
US 7,149,384 · App. 10/472,027 · Granted Dec 12, 2006

Grating design

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Quick Facts
Patent No.
US 7,149,384
App. No.
10/472,027
Granted
Dec 12, 2006
Kind
B2
Abstract

A method of designing a multi-channel grating structure in a waveguide material, the method comprising the step of utilizing a multi-channel grating design function describing an envelope of a refractive index variation defining the multi-channel grating structure in the waveguide material, wherein the multi-channel grating design function deviates from a periodic sampling function multiplied by a single channel grating design function.

Claims (97)

1. A method of designing a multi-channel grating structure with multi-channel spectral response characteristics in a waveguide material, the method comprising:

utilising an aperiodic multi-channel grating design function describing an envelope of a refractive index variation defining the multi-channel grating structure in the waveguide material, the design function being a solution to an inverse scattering problem for the multi-channel spectral response characteristics as described by more than one partial single channel response function, each partial single channel response function describing one channel of the multi-channel spectral response characteristics and at least one of the partial single channel response functions being phase shifted relative to the other partial single channel response functions.

2. A method as claimed in claim 1 , wherein the method further comprises providing the multi-channel grating design function by solving an inverse scattering problem for multi-channel spectral response characteristics as described by more than one partial single channel response function, each partial single channel response function describing one channel of the multi-channel spectral response characteristics and at least one partial single channel response function being phase shifted relative to the other partial single channel response functions.

3. A method as claimed in claim 2 , wherein each of the partial single channel response functions are phased shifted relative to the other partial single channel response functions.

4. A method as claimed in claim 1 , wherein the method further comprises the step of determining phase shifts of the partial single channel response functions for which an optimisation criterion is met.

5. A method as claimed in claim 4 , wherein the method further comprises determining phase shifts for which a maximum amplitude of the multi-channel grating design function is minimised.

6. A method as claimed in claim 4 , wherein the method further comprises determining phase shifts for which a maximum difference between a minimum amplitude and a maximum amplitude of the multi-channel grating design function is minimised.

7. A method as claimed in claim 4 , wherein the method further comprises determining phase shifts for which a mean-square-deviation of the amplitude of the multi-channel grating design function is minimised.

8. A method as claimed in claim 4 , wherein the determining the phase shifts comprises at least one of:

direct scanning through all combinations;

conducting a variational analysis;

using extremum search numerical techniques; and

a simulated annealing—Monte Carlo approach.

9. A method as claimed in claim 1 , wherein the method further comprises determining approximate values for the phase shifts.

10. A method as claimed in claim 9 , wherein the determining of the approximate values comprises:

forming a periodic sampling function by summation of periodic functions each describing a refractive index variation along the waveguide, wherein at least one periodic function includes an associated periodic function phase shift relative to the other periodic functions;

determining associated periodic function phase shifts for which an optimisation criteria is met; and

using the associated periodic function phase shifts as the approximate phase shifts.

11. A method as claimed in claim 10 , wherein the summation of the periodic functions comprises a Fourier analysis.

12. A method as claimed in claim 11 , wherein the result of the Fourier analysis represents a form of the expression:

l

=

1

N

κ

[

K

0

z

+

θ

+

(

2

l

-

N

-

1

)

Δ

κ

z

/

2

+

ϕ

l

]

=

κ

Q

(

K

0

z

+

θ

+

ψ

)

.

13. A method as claimed in claim 10 , wherein the determining of the associated periodic function phase shifts further comprises determining associated periodic function phase shift values for which a maximum amplitude of the periodic sampling function is minimised.

14. A method as claimed in claim 10 , wherein the determining of the associated periodic function phase shifts further comprises determining associated periodic function phase shifts for which a difference between a maximum amplitude and a minimum amplitude of the periodic sampling function is minimised.

15. A method as claimed in claim 10 , wherein the determining of the set of associated phase shifts further comprises determining a set of associated phase shifts for which a mean-square-deviation of the amplitude of the periodic sampling function is minimised.

16. A method as claimed in claim 13 , wherein the determining of the associated periodic function phase shifts comprises at least one of:

direct scanning through all combinations;

conducting a variational analysis;

using extremum search numerical techniques; and

a simulated annealing—Monte Carlo approach.

17. A method as claimed in claim 10 , wherein the periodic function phase shifts are used as the phase shifts to calculate the multi-channel grating design function.

18. A method as claimed in claim 10 , wherein the method comprises conducting a further optimisation process using the periodic function phase shifts as seeding values for the phase shifts and using the results of the optimisation process for calculating the multi-channel grating design function.

19. A method as claimed in claim 1 , wherein the grating is multi-dimensional, and wherein the multi-channel grating design function is multi-dimensional.

20. A multi-channel grating structure created utilising the design method as claimed in claim 1 .

Assignments (5)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 12, 2018
From: TE CONNECTIVITY AUSTRALIA PTY LTD
To: SUBSEA COMMUNICATIONS AUSTRALIA PTY LTD
Reel/Frame 047148/0151 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jul 27, 2018
From: TYCO ELECTRONICS PTY LIMITED
To: TE CONNECTIVITY AUSTRALIA PTY LTD
Reel/Frame 046481/0086 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 3, 2012
From: REDFERN OPTICAL COMPONENTS PTY LTD., AN AUSTRALIAN CORPORATION
To: TYCO ELECTRONICS PTY LTD., AN AUSTRALIAN CORPORATION
Reel/Frame 029072/0522 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 17, 2012
From: REDFERN OPTICAL COMPONENTS PTY LTD.
To: TYCO ELECTRONICS PTY LTD.
Reel/Frame 028972/0038 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 12, 2004
From: STEPANOV, DIMITRII YU; BURYAK, ALEXANDER
To: REDFERN OPTICAL COMPONENTS PTY LTD.
Reel/Frame 015336/0499 →