CA2236970C - Wavelength multiplexer/demultiplexer with varied propagation constant - Google Patents
Wavelength multiplexer/demultiplexer with varied propagation constant Download PDFInfo
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- CA2236970C CA2236970C CA002236970A CA2236970A CA2236970C CA 2236970 C CA2236970 C CA 2236970C CA 002236970 A CA002236970 A CA 002236970A CA 2236970 A CA2236970 A CA 2236970A CA 2236970 C CA2236970 C CA 2236970C
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/12007—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind forming wavelength selective elements, e.g. multiplexer, demultiplexer
- G02B6/12009—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind forming wavelength selective elements, e.g. multiplexer, demultiplexer comprising arrayed waveguide grating [AWG] devices, i.e. with a phased array of waveguides
- G02B6/12011—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind forming wavelength selective elements, e.g. multiplexer, demultiplexer comprising arrayed waveguide grating [AWG] devices, i.e. with a phased array of waveguides characterised by the arrayed waveguides, e.g. comprising a filled groove in the array section
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/12007—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind forming wavelength selective elements, e.g. multiplexer, demultiplexer
- G02B6/12009—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind forming wavelength selective elements, e.g. multiplexer, demultiplexer comprising arrayed waveguide grating [AWG] devices, i.e. with a phased array of waveguides
- G02B6/12014—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind forming wavelength selective elements, e.g. multiplexer, demultiplexer comprising arrayed waveguide grating [AWG] devices, i.e. with a phased array of waveguides characterised by the wavefront splitting or combining section, e.g. grooves or optical elements in a slab waveguide
Abstract
Wavelength dispersion in an optical demultiplexer (10) is accomplished by varying propagation constants of a central pathway (16) traverse to the direction of wavefront propagation through the central pathway (16). The propagation constant can be varied by changing the dimensions or refractive qualities of the central pathway, which can be formed as a common waveguide (36) or as plurality of individual waveguides (16).
Description
CA 02236970 1998-0~-07 WO 97/25639 PCT~US97/00077 WAVELENGTH MULTIPLEXERJDEMULTIPLEXER WITH VARIE~
PROPAGATION CONSTANT
Technical Field The invention relates to optical communication systems including 5 multiplexers and demultiplexers that route optical signals according to their wavelength.
Bac~<ground Optical signals of dirrerei ,l wavelengths traveling in separate optical fibers can be routed into a single optical fiber by a wavelength multiplexer and later 10 rerouted into separate optical fibers by a wavelength demultiplexer. Generally, the devices used in multiplexing and demultiplexing operations must be reversible so the same devices function as multiplexers in one direction of travel and as demultiplexers in the opposite direction of travel.
Within the multiplexing and demultiplexing devices, two main functions are 15 performed, namely, dispersing and focusing. The dispersing function spatiallydistinguishes the different waveiength signals, referred to as channels; and thefocusing function routes the signals between input and output waveguides accordi.~g to their dispersion.
Often, the same optical components perform both functions~ For example, CA 02236970 1998-0~-07 W O 97/25639 PCTnUS97/00~77 some multipiexing and demultiplexing devices use reflective diffraction gratingsto both disperse and focus the signals. Diffraction is the mechanism of dispersion, and 9, ~lin 9 curvature provides the focus. Other such devices referred to as Uphasors'' interconnect input and output waveguides with a 5 plurality of central waveguides that vary progressively in length. The ~,royressive variation in waveguide length produces phase front tilt as a function of wavelength. ~n angular arrangement of the central waveguides provides the focus.
Alternatively, separate lenses or mirrors can be used to provide the focusing 10 function. Relieved of this additional requirement, the dispersing components can be simplified. For example, flat diffraction gratings can be used in place of curved diffraction gratings, or parallel central waveguides can be used in placeo~ angularly arrayed central waveguides.
As design criteria become more stringent, such as requiring more closely spaced channels with minimum loss, lower cost, and smaller size, the current designs of multiplexers and demultiplexers become increasingly difficult and expensive to manufacture. High accuracy diffraction yra~ s are particularly expensive, and the amount of etching required by phasors is particularly time consuming.
Ordinarily, care must be taken to avoid compositional variations in materials and other dimensional variations that could produce unwanted changes in the prop~g:~tional characteristics of the waveguides. For example, U.S. Patent 5,450,511 to Dragone teaches that changes in the propagation constant can cause phase errors in the optical signals conveyed by multiplexing and demultiplexing devices resulting in increased cross-talk between channels and reduced efficiency of the devices.
CA 02236970 1998-0~-07 W O 97/25639 PCTAUS97tOO077 Summary of Inv~.~lic,.l Contrary to the teaching that changes in the propagation constant are to be avoided, my invention uses a progressive change in propagation constant to provide the dispersive function in wavelength multiplexers and demultiplexers.
5 This new mechanism for accomplishing wavelength dispersion can be used to reduce the physicai size and simplify the fabrication of these devices.
An embodiment of my invention includes the usual features of input and output optical pathways interconnected by dispersing and focusing elements. As a demultiplexer, the input optical pathway conveys a plurality of channels 0 distinguished by wavelength, and the output optical pathways separately conveythe channels. The dispersing element is a central optical pathway that receives the plurality of channels from the input optical pathway as a plurality of parallel wavefronts and lr~n:jro, .I~S the plurality of parallel wavefronts into a plurality of relatively inclined waver, onls. The focusing element directs the relatively 5 inclined waver,u,-l:j along the dirrere"t output optical pathways. However, instead of relatively inclining the wa\/erl unls by diffraction or variable length waveguides, the central pathway of my invention exhibits different propagation constants for a given wavelength across the central waveguide in a direction transverse to the dil~cliGi) of wavefront prop~g~tion through the central 20 waveguide.
The propagation constants can be changed in various ways. These include changing core dimensions of the central waveguide, as well as changing the index values of the core and cladding. The index profile of the core also figures in the propagation constant of non-step index profiles. For example, the index 25 profile can be seiected to increase the rate of change of the propagation constant for a given change in core dimension or peak refractive indices.
The central pathway can be composed of either a plurality of individual -CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 waveguides (or optical fibers) or a col,lr"o,l waveguide. Both include core portions surrounded by cladding. Core portions of the individual waveguides can be varied in width, thickness, and cross-sectional shape; and the core portion of the common waveguide can be varied in thickness. The overcladding can also 5 be varied in thickness. Doping or other material variations can be used to change the index values of the core and cladding between the individual waveguides or across the common waveguide.
Preferably, a reflective optic is positioned at one end of the central pathway to provide a more compact design. The relatively inclined wavef,onts of the 10 different wavelengths are further relatively inclined within the same space of the central pathway by rell or~rlection through the central pathway. The input and output pathways are adjacent to each other. The focusing element preferably performs a collimating function for directing different portions of the waver, l, Its along parallel optical pathways. The reflective optic for retroreflecting the waverro, lls along the parallel optical pathways is flat, and the individual waveguides of the central pathway are parallel to each other. However, the parallel pathways can also extend through the common waveguide without any lateral divisions, because the light remains collimated in the direction of propagation.
The optical pathways and the dispersing and focusing elements are pre~rably formed as an integrated optical circuit in planar optics. The relatively simple design of the elements allows for the use of fabrication lech~ ues such as "redraw~, where more exact tolerances can be obtained by sll ~1~ ,i"y planar substrates to control thickness. However, the invention could also be implemented in bulk optics or in a combination of planar and bulk optics.
CA 02236970 l998-0~-07 W O 97/25639 PCT~US97/00077 Drawings FIG. 1 is a plan view of a new demultiplexing optic in planar form having a plurality of parallel waveguides for dispersing different wavelength signals.
FIG. 2 is a graph showing phase front tilt to two different wavelengths 5 measured across a central passageway of the optic.
FIG. 3 is a graph showing an index profile superimposed on a section of waveguide.
FIG. 4 is a plan view of a second demultiplexing device having a co,))",on waveguide for dispersing different wavelength signals.
FIG. 5 is a cross-sectional end view of the common waveguide showing a tapered core Isyer.
FIG. 6 is a cross-sectional end view of the common waveguide showing a tapered cladding layer.
FIG. 7 is a plan view of a third demultiplexing device having a common ~5 waveguide with varying conce"lr~lions of dopant for dispersing dirrl3,~"~
wavelength signals.
FIG. 8 is a plan view of a fourth demultiplexing device having a plurality of radial waveguides for dispersing different wavelength signals.
Detailed Descri,~,tion Illustrated by drawing FIGS. 1-3 is a first embodiment of my invention implemented in planar optics. The embodiment is described with respect to a CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 direction of light travel for a demultiplexer but could function equally well in the opposite direction of light travel as a multiplexer. In fact, the terms ~multiplexer"
and "demultiplexer" are used only for the purpose of referencing the embodiment to one of these possible functions but do not exclude the other.
Optical signals of differing wavelengths (i.e., A, through An) enter a planar demultiplexing optic 10 from an input waveguide (or optical fiber) 12 and diverge to fill the aperture of a focusing optic (collimating lens) 14. The diverging wavefronts are collimated by the focusing optic 14. Discrete portions of the wavefronts propagate through a plurality of parallel waveguides 16 to a flat reflective optic 18, which retrorerlects the wavefronts on a return path to the focusing optic 14. The input waveguide 12 is preferably located along an opticalaxis of the focusing optic 14, but similar principles also apply for off-axis arrangements.
The parallel waveguides 16, which form a central pathway through the planar optic 10, share a common length ''Iw'' in a direction "Z" of wavefront propagation but progressively vary in width from "a1" to "ann along orthogonally related direction u~,. The change in waveguide width from "a," to ~an" indirectly variesoptical path lengths UL;" of the different waveguides 16 by changing an effective refractive index "n&~F" according to the following relationship:
Li=neff-~
The change in optical path lengths "Lj" evaluated at the reflective optic 18 relatively inclines the waver, ~ Ls according to their wavelengths A, - An as shown in the graph of FIG. 2. The graph ordinate spans the waveguides 16 in the direction "~' at a position coincident with the reflective optic 18. The graph 25 abscissa is in units of phase angle "q)". The stepped line (p(A,) represents a collection of the phase angles ~ n in the waveguides 16 for the wavelength A,.
CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 The stepped line l~p(An) represents a collection of the phase angles "q)" in thewaveguides 16 for the wavelength An. The angular difference between the two stepped lines ~(A,) and (p(An) represents a difference in phase front tilt between the two wavelengths A, and An~
The phase front tilt changes the focus of the returning waverl onls from coincidence with the input waveguide 12 (the expected focus of retroreflected waver. . "ts that are not tilted) to output waveguides 20 and 22 according to the respective amounts of tilt. For example, the wavelength A, focuses on the closeroutput waveguide 20 and the wavelength An focuses on the more distant output waveguide 22. Of course, more wavelengths A between the wavelengths A, and Anl representing additionai signals (or channels), could be focused on additional output waveguides positioned between the waveguides 20 and 22. The number of waveguides 16 could be increased to more accurately image the mode field of the input waveguide 12 on each of the output waveguides 20 and 22.
The effective index Und," of the respective waveguides is a quotier~t of propagation constant ~ " and wave numberUkO~ as follows:
neff = -where the wave number ~ can be expressed in terms of wavelength as follows:
PROPAGATION CONSTANT
Technical Field The invention relates to optical communication systems including 5 multiplexers and demultiplexers that route optical signals according to their wavelength.
Bac~<ground Optical signals of dirrerei ,l wavelengths traveling in separate optical fibers can be routed into a single optical fiber by a wavelength multiplexer and later 10 rerouted into separate optical fibers by a wavelength demultiplexer. Generally, the devices used in multiplexing and demultiplexing operations must be reversible so the same devices function as multiplexers in one direction of travel and as demultiplexers in the opposite direction of travel.
Within the multiplexing and demultiplexing devices, two main functions are 15 performed, namely, dispersing and focusing. The dispersing function spatiallydistinguishes the different waveiength signals, referred to as channels; and thefocusing function routes the signals between input and output waveguides accordi.~g to their dispersion.
Often, the same optical components perform both functions~ For example, CA 02236970 1998-0~-07 W O 97/25639 PCTnUS97/00~77 some multipiexing and demultiplexing devices use reflective diffraction gratingsto both disperse and focus the signals. Diffraction is the mechanism of dispersion, and 9, ~lin 9 curvature provides the focus. Other such devices referred to as Uphasors'' interconnect input and output waveguides with a 5 plurality of central waveguides that vary progressively in length. The ~,royressive variation in waveguide length produces phase front tilt as a function of wavelength. ~n angular arrangement of the central waveguides provides the focus.
Alternatively, separate lenses or mirrors can be used to provide the focusing 10 function. Relieved of this additional requirement, the dispersing components can be simplified. For example, flat diffraction gratings can be used in place of curved diffraction gratings, or parallel central waveguides can be used in placeo~ angularly arrayed central waveguides.
As design criteria become more stringent, such as requiring more closely spaced channels with minimum loss, lower cost, and smaller size, the current designs of multiplexers and demultiplexers become increasingly difficult and expensive to manufacture. High accuracy diffraction yra~ s are particularly expensive, and the amount of etching required by phasors is particularly time consuming.
Ordinarily, care must be taken to avoid compositional variations in materials and other dimensional variations that could produce unwanted changes in the prop~g:~tional characteristics of the waveguides. For example, U.S. Patent 5,450,511 to Dragone teaches that changes in the propagation constant can cause phase errors in the optical signals conveyed by multiplexing and demultiplexing devices resulting in increased cross-talk between channels and reduced efficiency of the devices.
CA 02236970 1998-0~-07 W O 97/25639 PCTAUS97tOO077 Summary of Inv~.~lic,.l Contrary to the teaching that changes in the propagation constant are to be avoided, my invention uses a progressive change in propagation constant to provide the dispersive function in wavelength multiplexers and demultiplexers.
5 This new mechanism for accomplishing wavelength dispersion can be used to reduce the physicai size and simplify the fabrication of these devices.
An embodiment of my invention includes the usual features of input and output optical pathways interconnected by dispersing and focusing elements. As a demultiplexer, the input optical pathway conveys a plurality of channels 0 distinguished by wavelength, and the output optical pathways separately conveythe channels. The dispersing element is a central optical pathway that receives the plurality of channels from the input optical pathway as a plurality of parallel wavefronts and lr~n:jro, .I~S the plurality of parallel wavefronts into a plurality of relatively inclined waver, onls. The focusing element directs the relatively 5 inclined waver,u,-l:j along the dirrere"t output optical pathways. However, instead of relatively inclining the wa\/erl unls by diffraction or variable length waveguides, the central pathway of my invention exhibits different propagation constants for a given wavelength across the central waveguide in a direction transverse to the dil~cliGi) of wavefront prop~g~tion through the central 20 waveguide.
The propagation constants can be changed in various ways. These include changing core dimensions of the central waveguide, as well as changing the index values of the core and cladding. The index profile of the core also figures in the propagation constant of non-step index profiles. For example, the index 25 profile can be seiected to increase the rate of change of the propagation constant for a given change in core dimension or peak refractive indices.
The central pathway can be composed of either a plurality of individual -CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 waveguides (or optical fibers) or a col,lr"o,l waveguide. Both include core portions surrounded by cladding. Core portions of the individual waveguides can be varied in width, thickness, and cross-sectional shape; and the core portion of the common waveguide can be varied in thickness. The overcladding can also 5 be varied in thickness. Doping or other material variations can be used to change the index values of the core and cladding between the individual waveguides or across the common waveguide.
Preferably, a reflective optic is positioned at one end of the central pathway to provide a more compact design. The relatively inclined wavef,onts of the 10 different wavelengths are further relatively inclined within the same space of the central pathway by rell or~rlection through the central pathway. The input and output pathways are adjacent to each other. The focusing element preferably performs a collimating function for directing different portions of the waver, l, Its along parallel optical pathways. The reflective optic for retroreflecting the waverro, lls along the parallel optical pathways is flat, and the individual waveguides of the central pathway are parallel to each other. However, the parallel pathways can also extend through the common waveguide without any lateral divisions, because the light remains collimated in the direction of propagation.
The optical pathways and the dispersing and focusing elements are pre~rably formed as an integrated optical circuit in planar optics. The relatively simple design of the elements allows for the use of fabrication lech~ ues such as "redraw~, where more exact tolerances can be obtained by sll ~1~ ,i"y planar substrates to control thickness. However, the invention could also be implemented in bulk optics or in a combination of planar and bulk optics.
CA 02236970 l998-0~-07 W O 97/25639 PCT~US97/00077 Drawings FIG. 1 is a plan view of a new demultiplexing optic in planar form having a plurality of parallel waveguides for dispersing different wavelength signals.
FIG. 2 is a graph showing phase front tilt to two different wavelengths 5 measured across a central passageway of the optic.
FIG. 3 is a graph showing an index profile superimposed on a section of waveguide.
FIG. 4 is a plan view of a second demultiplexing device having a co,))",on waveguide for dispersing different wavelength signals.
FIG. 5 is a cross-sectional end view of the common waveguide showing a tapered core Isyer.
FIG. 6 is a cross-sectional end view of the common waveguide showing a tapered cladding layer.
FIG. 7 is a plan view of a third demultiplexing device having a common ~5 waveguide with varying conce"lr~lions of dopant for dispersing dirrl3,~"~
wavelength signals.
FIG. 8 is a plan view of a fourth demultiplexing device having a plurality of radial waveguides for dispersing different wavelength signals.
Detailed Descri,~,tion Illustrated by drawing FIGS. 1-3 is a first embodiment of my invention implemented in planar optics. The embodiment is described with respect to a CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 direction of light travel for a demultiplexer but could function equally well in the opposite direction of light travel as a multiplexer. In fact, the terms ~multiplexer"
and "demultiplexer" are used only for the purpose of referencing the embodiment to one of these possible functions but do not exclude the other.
Optical signals of differing wavelengths (i.e., A, through An) enter a planar demultiplexing optic 10 from an input waveguide (or optical fiber) 12 and diverge to fill the aperture of a focusing optic (collimating lens) 14. The diverging wavefronts are collimated by the focusing optic 14. Discrete portions of the wavefronts propagate through a plurality of parallel waveguides 16 to a flat reflective optic 18, which retrorerlects the wavefronts on a return path to the focusing optic 14. The input waveguide 12 is preferably located along an opticalaxis of the focusing optic 14, but similar principles also apply for off-axis arrangements.
The parallel waveguides 16, which form a central pathway through the planar optic 10, share a common length ''Iw'' in a direction "Z" of wavefront propagation but progressively vary in width from "a1" to "ann along orthogonally related direction u~,. The change in waveguide width from "a," to ~an" indirectly variesoptical path lengths UL;" of the different waveguides 16 by changing an effective refractive index "n&~F" according to the following relationship:
Li=neff-~
The change in optical path lengths "Lj" evaluated at the reflective optic 18 relatively inclines the waver, ~ Ls according to their wavelengths A, - An as shown in the graph of FIG. 2. The graph ordinate spans the waveguides 16 in the direction "~' at a position coincident with the reflective optic 18. The graph 25 abscissa is in units of phase angle "q)". The stepped line (p(A,) represents a collection of the phase angles ~ n in the waveguides 16 for the wavelength A,.
CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 The stepped line l~p(An) represents a collection of the phase angles "q)" in thewaveguides 16 for the wavelength An. The angular difference between the two stepped lines ~(A,) and (p(An) represents a difference in phase front tilt between the two wavelengths A, and An~
The phase front tilt changes the focus of the returning waverl onls from coincidence with the input waveguide 12 (the expected focus of retroreflected waver. . "ts that are not tilted) to output waveguides 20 and 22 according to the respective amounts of tilt. For example, the wavelength A, focuses on the closeroutput waveguide 20 and the wavelength An focuses on the more distant output waveguide 22. Of course, more wavelengths A between the wavelengths A, and Anl representing additionai signals (or channels), could be focused on additional output waveguides positioned between the waveguides 20 and 22. The number of waveguides 16 could be increased to more accurately image the mode field of the input waveguide 12 on each of the output waveguides 20 and 22.
The effective index Und," of the respective waveguides is a quotier~t of propagation constant ~ " and wave numberUkO~ as follows:
neff = -where the wave number ~ can be expressed in terms of wavelength as follows:
2~
ko =--CA 02236970 1998-0~-07 The propagation constant ",13" can be calculated from a wave equation using well-known techniques. An example of a wave equation for a planar optical waveguide found in a reference by J. P. Meunier et al., Optical and Quantum Electronics 1~, (1983) 77-85, is as follows:
d +k2 n2 (x) (Pm (x) = l~m ~Pm (x) where the term "~pm(x)n is a field distribution of the mode and Un(x)" is the index profile of the core. The index profile "n(x)", which is shown in the cross-sectional view of FIG. 3, depends on the profile shape, core dimension "a", and the peak index values Un0'' of core 24 and "nC,adr of cladding 26. The latter peak 10 index values "nO" and Unclad" are often considered together as the variable u~", which is defined as follows:
~ nO--nclad nO
Any of these variables that affect the index profile Un(x)n of the respective waveguides 16 also can be used to change the propagation constant U,B", which 5 in turn changes the effective index "nOff" and the resulting optical path length ULjD
of the waveguides 16. The progressive variation in optical path length "Lj" of the waveguides 16 in the U~' direction produces the different wavefront tilts of thewavelength A, and Anl causing them to focus in the different positions occupied by the output waveguides 20 and 22.
CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 Preferably, the profile shape of non-step index waveguide profiles Is adjusted so that changes in the waveguide dimensions, e.g., "a", or changes in the peak indices, e.g., "~\", produce larger changes in the propagation constant U~ This limits the amount of required physical change between the different waveguides s 16. Also, the waveguides are preferably single mode to better control differences between their optical path lengths ~Ljn.
Two versions of a second embodiment of my invention are illustrated in FIGS.
4-6. A new planar demultiplexing optic 30 includes several of the same components as the planar optic 10 including input waveguide 32, collimating 0 optic 34, reflecting optic 38t and output waveguides 40 and 42. However, theplurality of individual waveguides 16 are replaced by a common waveguide 36.
Instead of varying respective width dimensions Ua,n through "an~ of individual waveguides, a thickness dimension utn of the common waveguide 36, which is measured in a direction "X", is varied in the same "Y" direction transverse to the direction UZn of wavefront propagation.
The common waveguide 36 is formed by a continuous layer 44 of core material located between continuous layers 46a and 46b of cladding material on a planar substrate 48. In one version of this embodiment, illustrated by FIG. 5,the core layer 44 continuously varies in thickness from ut"1n to ~t~2n across the 20 comrllon waveguide 36. In the other version, iltustrated by FIG. 6, the cladding layer 46a varies in thickness from utbln to "tb2" across the common waveguide 36.
Both thickness variations result in a continuous change of the propagation cc~)slanl U13n in the I~Yn direction across the waveguide. The collimating optic 34 limits any movement of the propagating waver, onls in the "Y" direction, so individual waveguides are not required to separate the propagating waver, un L~
into separate paths having different optical path lengths U~jD, The continuous variation of the propagation constant U~3n iS expected to more accurately project the mode field of the input waveguide 32 on each of the output waveguides 40 , CA 02236970 l998-0~-07 W O 97n5639 PCT~US97/00077 and 42.
The planar multiplexing optics 10 and 30 are particularly suitable for simpllfled manufacture by "redraw" in which layers of core 44 and cladding 46a and 46b are deposited on the substrate 48 with additional thickness and a~e 5 stretched together with the substrate to exact dimensions. The process permitsmuch wider tolerances for deposition. Alternatively, grinding or polishing couldbe used to control waveguide thickness.
A third embodiment of my invention, illustrated in FIG. 7, includes several features in common with the second embodiment. A planar demultiplexing optic 50 includes an input waveguide 52, a focusing optic (collimating lens) 54, a common waveguide 56, a flat reflective optic 58, and output waveguides 60 and 62. In contrast to the second embodiment, the propagation constant "~3" is varied by a change of rer,a~;live index across the common waveguide 56. For example, either or both of the peak refractive indices of the core 64 and cladding 66 can15 be changed, such as by adding varying concenl,aLions of dopant 68. The result, however, is similar to the second embodiment, namely, a continuous variation in the optical path length in the uy7~ direction.
The change in rer, active index can be made in several ways including using a thin film approach such as OVD (outside vapor deposition) and PECVD (plasn~a-20 enhanced chemical vapor deposition). The varying concentrations of dopant 68could also be achieved using ion exchange techniques.
A fourth and final embodiment shown in FIG. 8 is formed as a planar demultiplexing optic 70 including an input waveguide 72 and a focusing optic 74,which has zero power but provides a free-space region for converyil ,9 or 25 diverging wavefronts. A periodic array of radial waveguides 76, which form a central pathway through the optic 70, terminate at a curved reflective optic 78.Each radial waveguide 76 conveys a separate portion of a respective cylindrical CA 02236970 1998-0~-07 W O 97/25639 PCTrUS97/00077 wavefront corresponding to one of the wavelengths "A1" through UAn". The curved reflective optic 78 retroreflects the cylindrical wavefronts on a converging path through the radial waveguides 76 to the free-space of the focusing optic 74.
J
However, similar to the first embodiment, the radial waveguides 76 5 progressively vary in width from ~alU to "an" for changing the propagation constant "~3" of different portions of the cylindrical wavefronts. Although the waver~o"ls of the different wavelengths "A,'' through ~An~ propagate cylindrically, the change in propagation constant "~" remains transverse to the instant directions of wavefront propagation along the radial waveguides 76. The 0 resulting change in the optical path lengths "~," of the radial waveguides 76 relatively inclines the cylindrical wavefronts of the different wavelengths ~A,"through UAn", causing them to converge to slightly different focus positions at output waveguides 80 and 82.
Although the above-described embodiments of my invention are implemented 5 in planar optics, bulk or hybrid implementations are also possible. For example, optical fibers could be substituted for the parallel waveguides 16 of optic 10 or the radial waveguides 76 of optic 7Q. The various means for changing propagation constants disclosed in any one of the embodiments could also be applied to other of the embodiments. For example, the individual waveguides of 2~ FIGS. 1 and 8 could also be varied in thickness or in various refractive qualities.
Combinations of the various means for chanyil ,g the propagation CGI ,:,la"l, aswell as transverse variations in the length ''Iw~, could be used for further tuning the input and output mode fields.
The waveguides in the illustrated embodiments have been depicted as buried 25 waveguides, but other known types of waveguides including rib waveguides could also be used. Similarly, the focusing optic, which has been depicted as a lens, could also be arranged together with the input or output waveguides as a mirror, such as a collimating mirror or similar reflective surface. The input and CA 02236970 l998-05-07 W O 97125639 PCT~US97/00077 output waveguides of the various embodiments could also be arrayed in various combinations including equal numbers of input and output waveguides.
ko =--CA 02236970 1998-0~-07 The propagation constant ",13" can be calculated from a wave equation using well-known techniques. An example of a wave equation for a planar optical waveguide found in a reference by J. P. Meunier et al., Optical and Quantum Electronics 1~, (1983) 77-85, is as follows:
d +k2 n2 (x) (Pm (x) = l~m ~Pm (x) where the term "~pm(x)n is a field distribution of the mode and Un(x)" is the index profile of the core. The index profile "n(x)", which is shown in the cross-sectional view of FIG. 3, depends on the profile shape, core dimension "a", and the peak index values Un0'' of core 24 and "nC,adr of cladding 26. The latter peak 10 index values "nO" and Unclad" are often considered together as the variable u~", which is defined as follows:
~ nO--nclad nO
Any of these variables that affect the index profile Un(x)n of the respective waveguides 16 also can be used to change the propagation constant U,B", which 5 in turn changes the effective index "nOff" and the resulting optical path length ULjD
of the waveguides 16. The progressive variation in optical path length "Lj" of the waveguides 16 in the U~' direction produces the different wavefront tilts of thewavelength A, and Anl causing them to focus in the different positions occupied by the output waveguides 20 and 22.
CA 02236970 1998-0~-07 W O 97/25639 PCT~US97/00077 Preferably, the profile shape of non-step index waveguide profiles Is adjusted so that changes in the waveguide dimensions, e.g., "a", or changes in the peak indices, e.g., "~\", produce larger changes in the propagation constant U~ This limits the amount of required physical change between the different waveguides s 16. Also, the waveguides are preferably single mode to better control differences between their optical path lengths ~Ljn.
Two versions of a second embodiment of my invention are illustrated in FIGS.
4-6. A new planar demultiplexing optic 30 includes several of the same components as the planar optic 10 including input waveguide 32, collimating 0 optic 34, reflecting optic 38t and output waveguides 40 and 42. However, theplurality of individual waveguides 16 are replaced by a common waveguide 36.
Instead of varying respective width dimensions Ua,n through "an~ of individual waveguides, a thickness dimension utn of the common waveguide 36, which is measured in a direction "X", is varied in the same "Y" direction transverse to the direction UZn of wavefront propagation.
The common waveguide 36 is formed by a continuous layer 44 of core material located between continuous layers 46a and 46b of cladding material on a planar substrate 48. In one version of this embodiment, illustrated by FIG. 5,the core layer 44 continuously varies in thickness from ut"1n to ~t~2n across the 20 comrllon waveguide 36. In the other version, iltustrated by FIG. 6, the cladding layer 46a varies in thickness from utbln to "tb2" across the common waveguide 36.
Both thickness variations result in a continuous change of the propagation cc~)slanl U13n in the I~Yn direction across the waveguide. The collimating optic 34 limits any movement of the propagating waver, onls in the "Y" direction, so individual waveguides are not required to separate the propagating waver, un L~
into separate paths having different optical path lengths U~jD, The continuous variation of the propagation constant U~3n iS expected to more accurately project the mode field of the input waveguide 32 on each of the output waveguides 40 , CA 02236970 l998-0~-07 W O 97n5639 PCT~US97/00077 and 42.
The planar multiplexing optics 10 and 30 are particularly suitable for simpllfled manufacture by "redraw" in which layers of core 44 and cladding 46a and 46b are deposited on the substrate 48 with additional thickness and a~e 5 stretched together with the substrate to exact dimensions. The process permitsmuch wider tolerances for deposition. Alternatively, grinding or polishing couldbe used to control waveguide thickness.
A third embodiment of my invention, illustrated in FIG. 7, includes several features in common with the second embodiment. A planar demultiplexing optic 50 includes an input waveguide 52, a focusing optic (collimating lens) 54, a common waveguide 56, a flat reflective optic 58, and output waveguides 60 and 62. In contrast to the second embodiment, the propagation constant "~3" is varied by a change of rer,a~;live index across the common waveguide 56. For example, either or both of the peak refractive indices of the core 64 and cladding 66 can15 be changed, such as by adding varying concenl,aLions of dopant 68. The result, however, is similar to the second embodiment, namely, a continuous variation in the optical path length in the uy7~ direction.
The change in rer, active index can be made in several ways including using a thin film approach such as OVD (outside vapor deposition) and PECVD (plasn~a-20 enhanced chemical vapor deposition). The varying concentrations of dopant 68could also be achieved using ion exchange techniques.
A fourth and final embodiment shown in FIG. 8 is formed as a planar demultiplexing optic 70 including an input waveguide 72 and a focusing optic 74,which has zero power but provides a free-space region for converyil ,9 or 25 diverging wavefronts. A periodic array of radial waveguides 76, which form a central pathway through the optic 70, terminate at a curved reflective optic 78.Each radial waveguide 76 conveys a separate portion of a respective cylindrical CA 02236970 1998-0~-07 W O 97/25639 PCTrUS97/00077 wavefront corresponding to one of the wavelengths "A1" through UAn". The curved reflective optic 78 retroreflects the cylindrical wavefronts on a converging path through the radial waveguides 76 to the free-space of the focusing optic 74.
J
However, similar to the first embodiment, the radial waveguides 76 5 progressively vary in width from ~alU to "an" for changing the propagation constant "~3" of different portions of the cylindrical wavefronts. Although the waver~o"ls of the different wavelengths "A,'' through ~An~ propagate cylindrically, the change in propagation constant "~" remains transverse to the instant directions of wavefront propagation along the radial waveguides 76. The 0 resulting change in the optical path lengths "~," of the radial waveguides 76 relatively inclines the cylindrical wavefronts of the different wavelengths ~A,"through UAn", causing them to converge to slightly different focus positions at output waveguides 80 and 82.
Although the above-described embodiments of my invention are implemented 5 in planar optics, bulk or hybrid implementations are also possible. For example, optical fibers could be substituted for the parallel waveguides 16 of optic 10 or the radial waveguides 76 of optic 7Q. The various means for changing propagation constants disclosed in any one of the embodiments could also be applied to other of the embodiments. For example, the individual waveguides of 2~ FIGS. 1 and 8 could also be varied in thickness or in various refractive qualities.
Combinations of the various means for chanyil ,g the propagation CGI ,:,la"l, aswell as transverse variations in the length ''Iw~, could be used for further tuning the input and output mode fields.
The waveguides in the illustrated embodiments have been depicted as buried 25 waveguides, but other known types of waveguides including rib waveguides could also be used. Similarly, the focusing optic, which has been depicted as a lens, could also be arranged together with the input or output waveguides as a mirror, such as a collimating mirror or similar reflective surface. The input and CA 02236970 l998-05-07 W O 97125639 PCT~US97/00077 output waveguides of the various embodiments could also be arrayed in various combinations including equal numbers of input and output waveguides.
Claims (60)
1. A waveguide device for multiplexing or demultiplexing optical signals, as referenced in a direction for performing demultiplexing operations, comprising:
a first optical pathway that conveys a plurality of channels distinguished by wavelength;
a central optical pathway that is optically coupled to said first optical pathway and that receives the plurality of channels as a plurality of parallel wavefronts and transforms the plurality of parallel wavefronts into a plurality of relatively inclined wavefronts; and a focusing optic that is optically coupled to said central optical pathway and that conveys the relatively inclined wavefronts to respective second optical pathways, wherein said central pathway exhibits different propagation constants for a given wavelength across said central optical pathway in a direction transverse to a direction of propagation of the plurality of wavefronts through said central waveguide for relatively inclining the wavefronts of different wavelength.
a first optical pathway that conveys a plurality of channels distinguished by wavelength;
a central optical pathway that is optically coupled to said first optical pathway and that receives the plurality of channels as a plurality of parallel wavefronts and transforms the plurality of parallel wavefronts into a plurality of relatively inclined wavefronts; and a focusing optic that is optically coupled to said central optical pathway and that conveys the relatively inclined wavefronts to respective second optical pathways, wherein said central pathway exhibits different propagation constants for a given wavelength across said central optical pathway in a direction transverse to a direction of propagation of the plurality of wavefronts through said central waveguide for relatively inclining the wavefronts of different wavelength.
2. The device of claim 1 further comprising a reflective optic that reflects therelatively inclined wavefronts back through said central pathway to said focusing optic.
3. The device of claim 2 in which said reflective optic is oriented for retroreflecting the relatively inclined wavefronts.
4. The device of claim 2 in which said focusing optic directs different portionsof the wavefronts from said first optical pathway along parallel optical pathways.
5. The device of claim 1 in which said central pathway includes a plurality of waveguides having respective lengths that extend in the direction of wavefront propagation and respective widths that extend in a direction transverse to the direction of wavefront propagation.
6. The device of claim 5 in which said plurality of waveguides progressively vary in width one from another in a direction transverse to the direction of wavefront propagation.
7. The device of claim 6 in which said focusing optic directs different portionsof the wavefronts along parallel optical pathways and said plurality of waveguides extend parallel to each other for conveying the different portions ofthe wavefronts.
8. The device of claim 6 in which said plurality of waveguides are angularly related for conveying different portions of cylindrical wavefronts.
9. The device of claim 8 in which said reflective optic returns relatively inclined cylindrical wavefronts through said central pathway on route to said focusing optic, which has zero optical power.
10. The device of claim 6 in which said plurality of waveguides are equal in length.
11. The device of claim 1 in which said central pathway includes a common waveguide formed by continuous layers of core and cladding on a substrate surface and having a length that extends parallel to both the direction of wavefront propagation and the substrate surface, a width that extends perpendicular to the direction of propagation but parallel to the substrate surface, and a thickness that extends perpendicular to both the direction of wavefront propagation and the substrate surface.
12. The device of claim 11 in which one of said layers of core and cladding varies in thickness across the width of the common waveguide.
13. The device of claim 12 in which said core layer progressively varies in thickness across the width of the common waveguide.
14. The device of claim 12 in which said cladding layer progressively varies in thickness across the width of the common waveguide.
15. The device of claim 12 in which said layers of core and cladding remain of constant thickness along the length of the common waveguide.
16. The device of claim 11 in which one of said layers of core and cladding has a refractive index that varies across the width of the common waveguide.
17. The device of claim 16 in which said core layer has a refractive index that progressively varies across the width of the common waveguide.
18. The device of claim 16 in which said cladding layer has a refractive index that progressively varies across the width of the common waveguide.
19. The device of claim 16 in which the refractive indices of said core and cladding remain constant along the length of the common waveguide.
20. Apparatus for routing optical signals according to their wavelength comprising:
a single optical pathway that conveys a plurality of optical signals distinguished by their wavelength;
a plurality of optical pathways that separately convey the different wavelength signals; and a central optical pathway that relatively disperses the different wavelength signals for transmitting the different wavelength signals between the single optical pathway and the plurality of optical pathways, wherein the central optical pathway exhibits different propagation constants in a direction transverse to a direction of propagation through the central pathway for relatively dispersing the different wavelength signals.
a single optical pathway that conveys a plurality of optical signals distinguished by their wavelength;
a plurality of optical pathways that separately convey the different wavelength signals; and a central optical pathway that relatively disperses the different wavelength signals for transmitting the different wavelength signals between the single optical pathway and the plurality of optical pathways, wherein the central optical pathway exhibits different propagation constants in a direction transverse to a direction of propagation through the central pathway for relatively dispersing the different wavelength signals.
21. The apparatus of claim 20 further comprising a focusing element that directs different portions of the wavelength signals along parallel optical pathways.
22. The apparatus of claim 21 in which the parallel optical pathways differ from each other in dimension for exhibiting the different propagation constants.
23. The apparatus of claim 21 in which the parallel optical pathways differ from each other in refractive qualities for exhibiting the different propagationconstants.
24. The apparatus of claim 20 in which the central optical pathway is formed as a planar optic having a thickness that varies in the transverse direction.
25. The apparatus of claim 24 in which the central optical pathway is formed by layers of core and cladding material deposited on a substrate and the layer of core material varies in thickness in the transverse direction.
26. The apparatus of claim 24 in which the central optical pathway is formed by layers of core and cladding material deposited on a substrate and the layer of cladding material varies in thickness in the transverse direction.
27. The apparatus of claim 20 in which the central optical pathway has refractive qualities that vary in the transverse direction.
28. The apparatus of claim 27 in which the central optical pathway is formed by layers of core and cladding material and a refractive index of the layer of core material varies in the transverse direction.
29. The apparatus of claim 27 in which the central optical pathway is formed by layers of core and cladding material and a refractive index of the layer of cladding material varies in the transverse direction.
30. The apparatus of claim 27 in which the central optical pathway is formed by layers of core and cladding material and the layer of core material exhibits a non-step index profile that increases differences between the propagation constants with respect to a step index profile.
31. The apparatus of claim 20 in which the central optical pathway is formed by a plurality of waveguides exhibiting the different propagation constants.
32. The apparatus of claim 31 in which the plurality of waveguides vary from each other in a dimension measured transverse to the direction of propagation through the central pathway.
33. The apparatus of claim 31 in which the plurality of waveguides vary from each other in refractive qualities.
34. A method of dispersing different wavelength signals in a wavelength multiplexer/demultiplexer comprising the steps of:
receiving a plurality of different wavelength signals as a plurality of wavefronts;
directing different portions of the wavefronts along separate optical pathways exhibiting respective propagation constants; and varying the propagation constants between the separate optical pathways for relatively inclining the wavefronts according to their wavelength.
receiving a plurality of different wavelength signals as a plurality of wavefronts;
directing different portions of the wavefronts along separate optical pathways exhibiting respective propagation constants; and varying the propagation constants between the separate optical pathways for relatively inclining the wavefronts according to their wavelength.
35. The method of claim 34 in which said step of directing includes conveying the different portions of the wavefronts along a plurality of waveguides.
36. The method of claim 35 in which said step of directing includes conveying the different portions of the wavefronts along a plurality of parallelwaveguides.
37. The method of claim 35 in which said step of directing includes conveying the different portions of the wavefronts along a plurality of radial waveguides.
38. The method of claim 35 in which said step of varying includes varying individual dimensions of the waveguides measured transverse to a direction of propagation through the waveguides
39. The method of claim 34 in which said step of directing includes conveying the different portions of the wavefronts along a common waveguide.
40. The method of claim 39 in which said step of directing includes directing the different portions of the wavefronts along parallel pathways.
41. The method of claim 40 in which said step of varying includes varying a dimension of the common waveguide in a direction transverse to a direction of propagation through the common waveguide.
42. The method of claim 40 in which said step of varying includes varying a refractive quality of the common waveguide in a direction transverse to a direction of propagation through the common waveguide.
43. The method of claim 34 including the further step of forming the separate optical pathways with core and cladding materials exhibiting a non-step index profile that with respect to a step index profile increases differences between the propagation constants of the separate optical pathways.
44. A waveguide device for multiplexing or demultiplexing optical signals, as referenced in a direction for performing demultiplexing operations, comprising:
a first optical pathway that conveys a plurality of channels distinguished by wavelength;
a central optical pathway that is optically coupled to said first optical pathway and that receives the plurality of channels as a plurality of parallel wavefronts and transforms the plurality of parallel wavefronts into a plurality of relatively inclined wavefronts;
in which said central pathway includes a common waveguide formed by continuous layers of core and cladding on a substrate surface and having a length that extends parallel to both the direction of wavefront propagation and the substrate surface, a width that extends perpendicular to the direction of propagation but parallel to the substrate surface, and a thickness that extends perpendicular to both the direction of wavefront propagation and the substrate surface.
19a
a first optical pathway that conveys a plurality of channels distinguished by wavelength;
a central optical pathway that is optically coupled to said first optical pathway and that receives the plurality of channels as a plurality of parallel wavefronts and transforms the plurality of parallel wavefronts into a plurality of relatively inclined wavefronts;
in which said central pathway includes a common waveguide formed by continuous layers of core and cladding on a substrate surface and having a length that extends parallel to both the direction of wavefront propagation and the substrate surface, a width that extends perpendicular to the direction of propagation but parallel to the substrate surface, and a thickness that extends perpendicular to both the direction of wavefront propagation and the substrate surface.
19a
45. The device of claim 44 in which one of said layers of core and cladding varies in thickness across the width of the common waveguide.
46. The device of claim 45 in which said core layer progressively varies in thickness across the width of the common waveguide.
47. The device of claim 45 in which said cladding layer progressively varies in thickness across the width of the common waveguide.
48. The device of claim 45 in which said layers of core and cladding remain of constant thickness along the length of the common waveguide.
49. The device of claim 44 in which one of said layers of core and cladding has a refractive index that varies across the width of the common waveguide.
50. The device of claim 49 in which said core layer has a refractive index that progressively varies across the width of the common waveguide.
51. The device of claim 49 in which said cladding layer has a refractive index that progressively varies across the width of the common waveguide.
52. The device of claim 49 in which the refractive indices of said core and cladding remain constant along the length of the common waveguide.
19b
19b
53. Apparatus for routing optical signals according to their wavelength comprising:
at least one first optical pathway that conveys a plurality of optical signals distinguished by their wavelength;
a plurality of second optical pathways that separately convey the different wavelength signals; and a plurality of individual waveguides of equal length that relatively disperse the different wavelength signals for transmitting the different wavelength signals between the at least one first optical pathway and the plurality of second optical pathways.
at least one first optical pathway that conveys a plurality of optical signals distinguished by their wavelength;
a plurality of second optical pathways that separately convey the different wavelength signals; and a plurality of individual waveguides of equal length that relatively disperse the different wavelength signals for transmitting the different wavelength signals between the at least one first optical pathway and the plurality of second optical pathways.
54. The apparatus of claim 53, where in a direction traverse to the length of said individual waveguides said individual waveguides have a different propagation constant.
55. The apparatus of claim 53, wherein said apparatus comprises a reflective multiplexer/demultiplexer.
56. Apparatus for routing optical signals according to their wavelength comprising:
at least one first optical pathway that conveys a plurality of optical signals distinguished by their wavelength;
a plurality of second optical pathways that separately convey the different wavelength signals; and a common waveguide that relatively disperses the different wavelength signals for transmitting the different wavelength signals between the at least one first optical pathway and the plurality of second optical pathways.
19c
at least one first optical pathway that conveys a plurality of optical signals distinguished by their wavelength;
a plurality of second optical pathways that separately convey the different wavelength signals; and a common waveguide that relatively disperses the different wavelength signals for transmitting the different wavelength signals between the at least one first optical pathway and the plurality of second optical pathways.
19c
57. An optical wavelength multiplexer/demultiplexer for routing a plurality of different. wavelength channels into a plurality of particular individual wavelength channels as referenced in a direction for demultiplexing operations comprised of a first optical pathway that inputs the plurality of different. wavelength channels, a plurality of second optical pathways that each individually output. one of the particular individual wavelength channels, and a plurality of waveguides of equal length that disperse the plurality of different wavelength channels into the particular individual wavelength channels.
58. The optical wavelength multiplexer/demultiplexer of claim 57, further comprising a reflective optic.
59. An optical wavelength multiplexer/demultiplexer for routing a plurality of different wavelength channels into a plurality of particular individual wavelength channels as referenced in a direction for demultiplexing operations comprised a first optical pathway that inputs the plurality of different wavelength channels, a plurality of second optical pathways that each individually output one of the particular individual wavelength channels, and a common waveguide that disperses the plurality of different wavelength channels into the particular individual wavelength channels.
60. The optical wavelength multiplexer/demultiplexer of claim 59, further comprising a reflective optic.
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US08/586,134 US5768450A (en) | 1996-01-11 | 1996-01-11 | Wavelength multiplexer/demultiplexer with varied propagation constant |
| US08/586,134 | 1996-01-11 | ||
| PCT/US1997/000077 WO1997025639A1 (en) | 1996-01-11 | 1997-01-06 | Wavelength multiplexer/demultiplexer with varied propagation constant |
Publications (2)
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| CA2236970A1 CA2236970A1 (en) | 1997-07-17 |
| CA2236970C true CA2236970C (en) | 2002-12-03 |
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| CA002236970A Expired - Fee Related CA2236970C (en) | 1996-01-11 | 1997-01-06 | Wavelength multiplexer/demultiplexer with varied propagation constant |
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| DE (1) | DE69715149T2 (en) |
| TW (1) | TW317053B (en) |
| WO (1) | WO1997025639A1 (en) |
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-
1996
- 1996-01-11 US US08/586,134 patent/US5768450A/en not_active Expired - Lifetime
-
1997
- 1997-01-06 DE DE69715149T patent/DE69715149T2/en not_active Expired - Fee Related
- 1997-01-06 JP JP9525296A patent/JP2000503140A/en not_active Ceased
- 1997-01-06 WO PCT/US1997/000077 patent/WO1997025639A1/en active IP Right Grant
- 1997-01-06 AU AU16909/97A patent/AU1690997A/en not_active Abandoned
- 1997-01-06 CA CA002236970A patent/CA2236970C/en not_active Expired - Fee Related
- 1997-01-06 EP EP97902828A patent/EP0873533B1/en not_active Expired - Lifetime
- 1997-01-08 TW TW086100260A patent/TW317053B/zh active
Also Published As
| Publication number | Publication date |
|---|---|
| DE69715149D1 (en) | 2002-10-10 |
| EP0873533B1 (en) | 2002-09-04 |
| DE69715149T2 (en) | 2003-05-22 |
| WO1997025639A1 (en) | 1997-07-17 |
| EP0873533A1 (en) | 1998-10-28 |
| EP0873533A4 (en) | 1999-04-21 |
| AU1690997A (en) | 1997-08-01 |
| TW317053B (en) | 1997-10-01 |
| JP2000503140A (en) | 2000-03-14 |
| US5768450A (en) | 1998-06-16 |
| CA2236970A1 (en) | 1997-07-17 |
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| EEER | Examination request | ||
| MKLA | Lapsed |