Waveguide grating optical router suitable for CWDM
View Patent ↗A planar optical device useful as a low order wavelength router is realized by using a waveguide grating comprising two curved arrays of opposite curvatures. The diffraction order is determined by the angles of rotation of the two curved arrays, and any nonzero order less than about 30 can be realized. This arrangement is smaller, and performs better than a previous grating using a combination of three curved arrays.
1. A planar router, comprising:
an input coupler;
an output coupler; and
a grating having a plurality of waveguides forming arms of the grating, wherein:
successive arms of the grating have a path length difference ΔL which has a substantially constant value from each arm to a corresponding next arm;
the grating includes an input array of radial waveguides, a first curved array of waveguides, a central array of essentially straight waveguides, a second curved array of waveguides, and an output array of radial waveguides;
each waveguide of the first curved array is characterized by a curvature radius R that varies as a function of an angle of rotation θ of the waveguide and variation of R is minimized by choosing parameters of the first curved array so that a derivative of said variation of R is essentially zero for a particular principal angle of rotation θ=θ 0 inside an aperture of the first curved array, so that a radius of a principal waveguide corresponding to said principal angle of rotation θ 0 is a smallest curvature radius in said first curved array;
each waveguide of the second curved array is characterized by a curvature radius R′ that varies as a function of an angle of rotation θ′ of the waveguide and variation of R′ is minimized by choosing parameters of the second curved array so that a derivative of said variation of R′ is essentially zero for a particular principal angle of rotation θ′=θ′ 0 inside an aperture of the second curved array, so that a radius of a principal waveguide corresponding to said principal angle of rotation θ′ 0 is a smallest curvature radius in said second curved array;
the first and second curved arrays have opposite curvatures and said principal angles of rotations θ 0 and θ′ 0 are chosen so as to produce nonzero diffraction orders.
2. The planar router as recited in claim 1 wherein:
the waveguides of the central array have substantially constant waveguide spacing.
3. The planar router as recited in claim 1 wherein:
said smallest curvature radii of the first and second principal waveguides are substantially smaller than radii produced at edges of an aperture of the grating;
said principal angles of rotations θ 0 and θ′ 0 of the first and second principal waveguides, respectively, satisfy a condition θ 0 ≧θ′ 0 ; and
a path length difference ΔL is greater than a value of an expression:
tan(θ 0 /2)·(s max +s min )−tan(θ′ 0 /2)·2s max
and ΔL is smaller than the value of:
tan(θ 0 /2)·2s max −tan(θ′ 0 /2)·(s max +s min )
where s max and s min are respectively largest and smallest waveguide separation in a central grating region that includes the first and second curved arrays and the central array.
4. The planar router as recited in claim 1 , further comprising:
only one input waveguide and wherein an angular period of the input array of radial waveguides is greater than an angular period of the output array of radial waveguides.
5. The planar router as recited in claim 1 wherein:
the output array of radial waveguides has, at a junction with the output coupler, an angular period substantially equal to one half an angular period at a junction with the second curved array.
6. The planar router as recited in claim 5 , further comprising:
one input waveguide and N output waveguides whose locations on an output circle of the router are chosen so that:
two consecutive cycles of the router provide between said input waveguide and said output waveguides substantially maximum transmission in two separate wavelength intervals λ 1 <λ<λ 2 and λ 3 <λ<λ 4 respectively produced by the two cycles; and
a spectral efficiency
(
λ
2
-
λ
1
)
(
λ
4
-
λ
3
)
(
λ
4
-
λ
1
)
is greater than 0.7.
wherein λ 1 , λ 2 , λ 3 , λ 4 denote wavelengths that define boundaries of said wavelength intervals, and
wherein the router is coupled to a plurality of fibers.
7. The planar router as recited in claim 6 wherein the router is used in a local access node to provide, in each of the fibers coupled to the router, efficient transmission of downstream and upstream signals in two separate wavelength intervals λ 1 <λ<λ 2 and λ 3 <λ<λ 4 respectively produced by the two consecutive cycles of the router.
8. An optical arrangement, comprising:
a first router as recited in claim 5 ;
a second router having one input waveguide and N output waveguides whose locations on an output circle of the second router are chosen so that two consecutive cycles of the second router provide between said input waveguide and said output waveguides substantially maximum transmission in two separate wavelength intervals λ 1 <λ<λ 2 and λ 3 <λ<λ 4 respectively produced by the two cycles and a spectral efficiency
(
λ
2
-
λ
1
)
(
λ
4
-
λ
3
)
(
λ
4
-
λ
1
)
is greater than 0.7, and a fiber is coupled between the first and second routers, wherein:
λ 1 , λ 2 , λ 3 , λ 4 denote wavelengths that define boundaries of said wavelength intervals;
the first router includes 2N input ports and one output port; and
2N wavelength channels are transmitted in one cycle of the first router.
9. The planar router as recited in claim 1 wherein each of the arms of the grating includes sections having different effective refractive indexes.
10. An apparatus, comprising:
input coupler means for receiving an input signal;
grating means for propagating components of the received input signal in respective ones of a plurality of arms, the grating means including an input array of radial waveguides, a first curved array of waveguides, a central array of essentially straight waveguides, a second curved array of waveguides, and an output array of radial waveguides; and
output coupler means for combining the components that have propagated in the arms into an output signal,
wherein the first and second curved arrays have opposite curvatures,
wherein each waveguide of the first curved array is characterized by a curvature radius R that varies as a function of an angle of rotation θ the waveguide and variation of R is minimized by choosing parameters of the first curved array so that a derivative of said variation of R is essentially zero for a particular principal angle of rotation θ=θ 0 inside an aperture of the first curved array, so that a radius of a principal waveguide corresponding to said principal angle of rotation θ 0
is a smallest curvature radius in said first curved array, and
wherein each waveguide of the second curved array is characterized by a curvature radius R′ that varies as a function of an angle of rotation θ′ of the waveguide and variation of R′ is minimized by choosing parameters of the second curved array so that a derivative of said variation of R′ is essentially zero for a particular principal angle of rotation θ′=θ′ 0 inside an aperture of the second curved array, so that a radius of a principal waveguide corresponding to said principal angle of rotation θ′ 0 is a smallest curvature radius in said second curved array.
11. The apparatus of claim 10 wherein said principal angles of rotations θ 0 and θ′ 0 are chosen so as to produce nonzero diffraction orders.
12. The apparatus of claim 10 wherein each of the arms of the grating means includes sections having different effective refractive indexes.
13. The apparatus of claim 10 wherein successive arms of the grating means have a path length difference ΔL which has a substantially constant value from each arm to a corresponding next arm.
14. The apparatus of claim 10 wherein the waveguides of the central array have substantially constant waveguide spacing.
15. The apparatus of claim 10 wherein the radial waveguides in the input and output arrays have constant radial separation between waveguides.
16. The apparatus of claim 10 wherein said smallest curvature radii of the first and second principal waveguides are substantially smaller than radii produced at edges of an aperture of the grating.
17. The apparatus of claim 10 wherein the apparatus comprises a router.
18. The apparatus of claim 10 wherein an angular period of the input array of radial waveguides is greater than an angular period of the output array of radial waveguides.
19. The apparatus of claim 10 wherein the output array of radial waveguides has, at a junction with the output coupler means, an angular period substantially equal to one half an angular period at a junction with the second curved array.
20. A method, comprising:
receiving an input optical signal at an input coupler;
propagating components of the received input signal in respective ones of a plurality of arms of a grating, the grating including an input array of radial waveguides, a first curved array of waveguides, a central array of essentially straight waveguides, a second curved array of waveguides, and an output array of radial waveguides,
wherein the first and second curved arrays have opposite curvatures,
wherein each waveguide of the first curved array is characterized by a curvature radius R that varies as a function of an angle of rotation θ of the waveguide and variation of R is minimized by choosing parameters of the first curved array so that a derivative of said variation of R is essentially zero for a particular principal angle of rotation θ′=θ′ 0 inside an aperture of the first curved array, so that a radius of a principal wave guide corresponding to said principal angle of rotation θ′ 0 is a smallest curvature radius in said first curved array, and
wherein each waveguide of the second curved array is characterized by a curvature radius R′ that varies as a function of an angle of rotation θ′ of the waveguide and variation of R′ is minimized by choosing parameters of the second curved array so that a derivative of said variation of R′ is essentially zero for a particular principal angle of rotation θ′=θ′ 0 inside an aperture of the second curved array, so that a radius of a principal waveguide corresponding to said principal angle of rotation θ′ 0 is a smallest curvature radius in said second curved array; and
combining the components that have propagated in the arms into an output signal at an output coupler.
21. The method of claim 20 , further comprising arranging said principal angles of rotations θ 0 and θ′ 0 so as to produce nonzero diffraction orders.
22. The method of claim 20 , further comprising providing each of the arms of the grating with sections having different effective refractive indexes.
23. The method of claim 20 , further comprising providing successive arms of the grating with a path length difference ΔL which has a substantially constant value from each arm to a corresponding next arm.
24. The method of claim 20 , further comprising providing the waveguides of the central array with substantially constant waveguide spacing.
25. The method of claim 20 , further comprising providing the radial waveguides in the input and output arrays with constant radial separation between waveguides.
26. The method of claim 20 wherein said smallest curvature radii of the first and second principal waveguides are substantially smaller than radii produced at edges of an aperture of the grating.
27. The method of claim 20 wherein an angular period of the input array of radial waveguides is greater than an angular period of the output array of radial waveguides.
28. The method of claim 20 wherein the output array of radial waveguides has, at a junction with the output coupler, an angular period substantially equal to one half an angular period at a junction with the second curved array.