IL151095A - Multilayer integrated optical device and a method of fabrication thereof - Google Patents
Multilayer integrated optical device and a method of fabrication thereofInfo
- Publication number
- IL151095A IL151095A IL151095A IL15109502A IL151095A IL 151095 A IL151095 A IL 151095A IL 151095 A IL151095 A IL 151095A IL 15109502 A IL15109502 A IL 15109502A IL 151095 A IL151095 A IL 151095A
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- Prior art keywords
- layer
- guiding
- waveguiding element
- waveguiding
- optical
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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
- G02B6/13—Integrated optical circuits characterised by the manufacturing method
- G02B6/132—Integrated optical circuits characterised by the manufacturing method by deposition of thin films
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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
- G02B6/12002—Three-dimensional structures
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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
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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
- G02B6/122—Basic optical elements, e.g. light-guiding paths
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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
- G02B2006/12083—Constructional arrangements
- G02B2006/12097—Ridge, rib or the like
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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
- G02B2006/12133—Functions
- G02B2006/12147—Coupler
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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
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29331—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by evanescent wave coupling
- G02B6/29335—Evanescent coupling to a resonator cavity, i.e. between a waveguide mode and a resonant mode of the cavity
- G02B6/29338—Loop resonators
- G02B6/29343—Cascade of loop resonators
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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
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29379—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device
- G02B6/2938—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device for multiplexing or demultiplexing, i.e. combining or separating wavelengths, e.g. 1xN, NxM
- G02B6/29386—Interleaving or deinterleaving, i.e. separating or mixing subsets of optical signals, e.g. combining even and odd channels into a single optical signal
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- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Optical Integrated Circuits (AREA)
- Semiconductor Lasers (AREA)
- Light Receiving Elements (AREA)
Abstract
A method of fabricating an integrated optical device and such a device, comprising a structure including at least one waveguiding element are presented. A basic structure is formed containing a substrate material carrying a buffer material layer coated with a core material layer of a higher refraction index as compared to that of the buffer layer. The at least one waveguiding element is defined in a guiding layer on top of the basic structure. The guiding layer is made of a material with a refractive index higher than the refractive index of the buffer layer and the core layer, and is chosen so as to minimize a height of the at least one waveguiding element and to provide effective guiding of light in the core layer. A cladding layer is formed on top of the so-obtained structure, wherein a height difference between the cladding layer region above the waveguiding element and the cladding layer region outside the waveguiding element is substantially small resulting in a desired flatness of the top cladding layer to allow direct formation of a further waveguide structure thereon and prevent significant perturbations in light propagation within the further waveguide structure.
Description
A multilayer integrated optical device and a method of fabrication thereof
Lambda Crossing Ltd. « »ip matt
C. 139706
A Multilayer Integrated Optical Device
and a Method of Fabrication Thereof
FIELD OF THE INVENTION
This invention is in the field of Planar Lightwave Circuits (PLC), and relates to a multilayer integrated optical device and a memod of fabrication thereof.
BACKGROUND OF THE INVENTION
Optical cormnunications is the enabling technology for the inforrnation age, and the essential backbone for long haul commumcations. As mis technology progresses, there is a tremendous interest in providing optical routes in the short haul, metropolitan and access networks, as well as in local area networks and cable TV networks. In all these networks, the best of breed solution for bandwidth expansion has been the adoption of wavelength division multiplexing (WDM), which entails the aggregation of many different information carrying light streams on the same optical fiber. Devices capable of accessing individual information streams are fundamentally recmired in current and future networks. These devices can also add information streams to the optical fiber, as well as impress information on an optical stream by optical modulation.
PLC technology is central in the creation of modem optical elements for communications systems. According to this technology, optical waveguides and additional functional structures are fabricated in a planar optical transparent medium in order to direct the passage of light and to implement coupling, filtering, switching, and additional processing functions as required for optical conTmunications.
Existing examples of Planar Lightwave Circuits include optical switches and modulators based on Mach Zender Interferometer (ΜΖΓ), in which interference is produced between phase coherent hght waves that have traveled over different path lengths; arrayed waveguide routers (AWG) used for combining and spreading multiple optical channels, namely, multiplexers and demultiplexers. However, to achieve a good modulation performance with the MZI, the latter is typically designed with long interference arms. As a result, this device is not size-efficient in its implementation, and limits the scaling ability of complex optical circuits. Another feature of MZI-type devices, in ti teir predominant implementation, is their frequency insemitivit over a desired f equency bandwidth. As a result, MZI-type devices cannot be used directly for wavelength routing.
An important driving force pushing PLC technology is the need for enhanced functionality in the optical domain. This need is hampered by the limitation of state of the art waveguide technology, which is two-dimensional (i.e., single-functional-layer architecture). Unlike the very large scale integrated electronic circuitry, where dimensions of the basic elements were reduced to sub-micrometer size, the optical PLC circuitry is inherently much larger, thus the exploitation of multi-layer architectures is much more crucial than in electronics.
In me implementation of PLC, there is a contradiction between the requirements of coupling to optical fibers and decreasing circuit size. Coupling to fibers is best obtained by using waveguides with modal fields similar to the fiber modes with a small refractive index difference with respect to the surrounding medium The functionality of the optical circuits depends on the amount of optical elements in the circuit By decreasing he circuit size, more optical circuits can be integrated and the attainable functionahty increases. Smaller dimensions imply tighter control of the optical mode and smaller optical modes, hence, a high index contrast between the waveguide core and surrounding medium. It is of fundamental importance to provide a means of combining both elements in one functional optical circuit
The importance of utilizing the vertical dimensions in creating complex optical circuits has been recognized and addressed in the past. This is associated with the fact that vertical fabrication tolerances are better than horizontal tolerances, and therefore such a vertical integrated optical device (filter, switch, modulator) is simpler or cheaper to manufacture. Optical devices utilizing this approach are disclosed, for example, in the article "Vertically Coupled Glass Microring Resonator Channel Dropping Filters ", B.E. Little et al., IEEE Photonics technology Letters, Vol. 11, No. 2, February 1999. This approach is critical for the fabrication of optical circuits based on structures with very different indices of refraction such that the effective coupling region between the structures is very small, e.g., coupling between waveguides and ring micro-resonators. In this case, the vertical dimension, which is easier to control in conventional processes, can mediate the structure for accurate coupling as described in the aforementioned reference.
Recently developed integrated electro-optical devices utilize resonant rings to achieve frequency selective switching. Such a device is disclosed, for example, in WO 99/17151. The device comprises a ring resonator interconnected by linear waveguides to couple light from a first linear waveguide to the second one, when die frequency of the light passing through the first waveguide fulfils that of the resonance condition of the ring. By applying an electric field to the ring, its refractive index, and consequently, its resonance condition, can be desirably adjusted, thereby preventing , the passage of t e previously coupled light the device therefore acting as a switch. Alternatively, the loss of the rhg waveguide can be changed. Adding loss to the ring diminishes its operation as a resonant cavity, and light cannot be coupled from the waveguide to waveguide.
To create two or more layers of intercorinected waveguides with the prior art techniques, a planarization step has to be performed. Figs. 1A-1D illustrate main sequential steps of the prior art technique employed for manm¾c1iiring a waveguide structure shown in Fig. IE being generally designated 10. Initially, a buffer layer 12 of S1O2 is deposited on a silicon wafer 14 (Fig. 1A). Then, a layer 16 of doped S1O2 with a higher refractive index (SiCk+Ge), as compared to that of the buffer layer 12,
is deposited onto the buffer layer (Fig. IB). This layer 16 serves for the formation of a core 16A of the optical waveguide, and its thiclaiess is typically in the range of 4-12μΐη. To form the waveguide core 16A (Fig. 1C), the waveguide, as well as other optical structures, are masked using photolithography followed by etching. A third layer of S1O2, or upper cladding layer 18, is then deposited so as to bury the etched structure (Fig. ID).
This layer 18 retains to some extent the topography of the underlying structure, and thus requires planarization to allow for an additional overiaying waveguide structure to be deposited Planarization can be implemented by Chemical Mechanical Polishing, refLow techniques, deposition of a very thick layer, selective etching or deposition techniques. As shown in Fig. IF, after achieving a planar top layer, a second waveguide structure 20 can be fabricated on top of the structure 10 in the above-described manner.
Planarization is a difficult process step, which utilizes expensive equipment and is difficult to be accurately applied for large area wafers. Therefore, it would be desirable to eliminate this step in the fabrication of multi-layered optical waveguide structures.
SUMMARY OF THE INVENTION
There is accordingly a need in the art to facilitate the manufacturing of a three-dimensional (multi-layered) integrated optical device, by providing a novel method of fabricating such a device, and a novel integrated optical device based on an optical structure embodying- different material systems. Such a device may be an optical f equency dependent switch, a modulator, an Optical Add Drop Multiplexer (OADM), a spectral analyzer, a sensor, etc.
The main idea of the present invention consists of utilizing a waveguide definition on several layers, enabling to combine low coupling loss waveguides with high com nement waveguides. The present invention opens new horizons for the functionality of optical devices using Planar Waveguide Technology. The present invention provides a fabrication method for the manufacture of three-dimensional
P T/EL01/00379
- 5 - fabrics of waveguides with three-dmiei-sm Furthermore, since it is recognized that three-dimensional interconnections are crucial for creating resonator-based, high-density optical circuits, the invention provides a fabrication method for such devices.
The invention provides for the fabrication of three-dimensional optical waveguiding structures by simple processing steps. The main innovation here relates to the elirnination or at least alleviation of the planarization step, which is difficult to implement As indicated above, planarization is required to overcome the perturbations in a given layer caused by the previously deposited layers. In the present invention, the adoption of novel waveguide structures roinirnizes the perturbation, and facilitates multi-level integration of light guiding structures.
There is thus provided according to one aspect of the present invention, a method of fabricating an integrated optical device comprising a structure including at least one waveguiding element, the method comprising the steps of:
(i) forming a basic structure containing a substrate material carrying a buffer material layer coated with a core material layer of a higher refraction index as compared to that of the buffer layer;
(ii) defining said at least one waveguiding element in a guiding layer on top of said basic structure, wherein said gmding layer is made of a material with a refractive index higher than the refractive index of said buffer layer and the core layer, and is chosen so as to minimize a height of said at least one waveguiding element and to provide effective guiding of light in the core layer;
(iii) forming a cladding layer on top of a structure obtained i step (ii), wherein a height difference between a height of the cladding layer region above said at least one waveguiding element and a height of the cladding layer region outside the waveguiding element is substantially small, thereby providing a sufficient flatness of the top cladding layer to allow formation of a further waveguide structure
P T/IL01/00379
- 6 - thereon and prevent significant perturbation in light propagation within said further waveguide structure.
At least one Waveguide element may be defined by a ridge of the high index material (as compared to the buffer layer) on top of the basic structure. Alternatively this waveguide element may be a resonator ring (resonator cavity loop), in which case the further waveguide structure contains a further waveguiding element formed on top of the cladding layer by repeating steps (i) and (ii).
It should be understood that the term "sufficient flatness of the cladding layer" used herein signifies a flatness defined by the height difference of the different regions of the cladding layer (i.e., above the wavegmding element and outside the waveguiding element) much smaller than the optical mode zise of a further waveguiding element
For example, the height difference in the order of few hundreds of nanometers can be obtained, the optical mode size of the further waveguide formed on the cladding layer being about several micrometers. Typically, the height difference of the cladding layer does not exceed the height of the at least one wavegdding element (ie., the thickness of the guiding layer) covered by said cladding layer.
According to another aspect of the present invention, there is provided a method of fabricating a three-dimensional integrated optical device comprising at least two vertically aligned waveguide structures, each mcluding at least one waveguiding element, the method comprising the steps of:
(a) forming a basic structure containing a substrate carrying a buffer layer coated with a core material layer of a higher refractive index as compared to that of he buffer layer;
(b) defining said at least one waveguiding element of the lower waveguide structure in a guiding layer on top of said basic structure, wherein said guiding layer is made of a material with a refractive mdexMgfter than the refractive index of said buffer layer and the core layer, is chosen so as to minimize a height of said at least one waveguide element and to provide effective gmdmg oflightin the core layer; and
(c) forming an upper cladding layer on top of a structure obtained in step (b), wherein a height difference between a height ofme cladding layer region above said at least one waveguiding element and a height of the cladding layer region outside the waveguiding element is substantially small, thereby providing a sufficient flatness of said upper cladding layer to allow direct formation of the upper waveguide structure thereon;
(d) forming said upper waveguide structure on top of said upper cladding layer by depositing a further buffer layer and repeating steps (b) and (c) with respect to a further guiding layer, sigmficant perturbation in light propagation within said upper waveguide structure being thereby prevented.
According to yet another aspect of the present invention, there is provided an integrated optical device comprising at least one stmcture having at least one waveguiding element, the device comprising:
- a basic structure containing a substrate material carrying a buffer material layer coated with a core material layer of a higher refraction index as compared to that of the buffer layer;
- said at least one waveguiding element formed in a guiding layer on top of said basic structure, wherein said guiding layer is made of a material with a refractive index higher than the refractive index of said buffer layer and the core layer, and is chosen so as to minimize a height of said at least one waveguiding element and to provide effective guiding of light in the core layer;
- a cladding layer on top of a stracture with said at least one waveguiding element, wherein a height difference between a height of the cladding layer region above said at least one mveguiding element and a height of the cladding layer region outside the waveguiding element is substantially small, the top cladding layer thereby having a desired flatness.
The device may comprise additional waveguides and additional loop-resonators, foiming together several frequency selective switches, thereby providing complex optical signal switching and routing.
Since optical waveguides can be implemented in complex manners, the universal quantity characterizing the behavior of the confined light is the effective refractive index of the waveguide. In conventional devices, Ihe difference between the effective refractive index of the waveguide and the index of the surrounding medium is typically smaller than 1%. When using ring micro resonator structures, the effective refractive index of the ring- waveguide has to be large, i.e., typically greater than 20%, to accommodate tight mode confinement and small losses, m these structures, however, the effective index of the ring waveguide and the linear waveguide are similar to within few percents (e.g., about 3%). The present invention provides for using several (at least two) ring resonators (ring waveguides) in an integrated optical device, the refractive index of the ring waveguide being thereby substantially greater (e.g., 20% greater) than title refractive index of the linear waveguide that receives an input signal.
. In an optical complex filter/resonator according to the invention, waveguide sections are specifically connected to ring resonators in a configuration which enables realization of optical switehing, wavelength routing, optical filtering, etc. The device may also combine a plurality of such filters in a wavelength router module.
Modem optical communications are typically based on transmitting frequency multiplexed optical signals tkough an optical fiber. The OADM is capable of adding or dropping optical channels from an optical fiber, and is an essential element in modem optical communications. In the present invention, the OADM is based on a combination of tunable filters, which provide the add or drop multiplexing functions. Since OADMs have to meet stringent criteria in their filtering, each ring resonator is an optical filter, and, by combining them in parallel, high order filters are obtained.
- Si -
Ill general, the resonator-cavity loops (ring-resonators) can be replaced by any other implementation of a f equency-selective element that couple between the two waveguide sections. For example, optical gratings can be used.
BRIEF DESCRIPTION OF THE DRAWINGS
In order to understand the invention and to see how it may be carried out in practice, a preferred embodiment will now be described, by way of non-limiting example only, with reference to the accompanying drawings, in which:
Figs. 1 Ato IF illustrate the prior art technique of manuf acturing a waveguide structure;
Figs. 2 A and 2B compare the prior art ridge waveguide structure shown in
Fig.2A to that of the present invention shown in Fig. 2B.
Figs. 3A and 3B illustrate mode profiles o£ respectively, a prior art standard waveguide and a prior art ridge waveguide;
Fig. 3C illustrates a mode profile of a ridge waveguide according to the present invention;
Fig. 4 iHustrates a stracture definition of a ridge waveguide coupled to a ring resonator, fabricated by a method according to the invention;
Figs. 5A to 5E illustrate main mmufacturing steps of the method used for fabricating the stracture of Fig. 4;
Fig. 6 illustrates a stracture definition of a two-layer ridge waveguide optical coupler fabricated by a method according to the invention;
Figs. 7A to 7E illustrate main manufacturing steps of the method used for fabricating the structure of Fig. 6;
Fig. 8 illustrates a stracture definition of a ring resonator coupled to a low index difference waveguide, fabricated by a method according to the invention;
Figs. 9A to 9E illustrate main manufacturing steps of the method used for fabricating the stracture of Fig. 8;
Figs. 10A to IOC illustrate ring resonator based filters of, respectively, one, two and three rings, that can be manufactured by the method according to the invention;
Fig. 11 illustrates the optical spectral response of the ring resonator based filters of Figs. lOA-lOC;
Figs. 12A and 12B illustrate main constructional features and main functional features, respectively, of a single channel Optical Add Drop Multiplexer (OADM) according to the invention;
Fig. 13 illustrates a four port-add drop multiplexer accord^ to the invention; Fig. 14 illustrates an example of the integration of switches and add drop filters for switch-able filters;
Figs. 15A and 15B illustrate the construction and operational principles of an interleave filter;
Figs. 16A and 16B illustrate the construction and operational principles of a single channel separation element (filter) according to the invention utilizing ring resonators optically coupled to linear waveguides;
Fig. 17 illustrates a spectral analysis filter accordmg to the invention;
Fig. 18 illustrates a tap coupler and spectral analysis system utilizing the spectral analysis filter of Fig. 17;
Fig. 19 illustrates a spectrum analyzer according to the invention utilizing several spectral analysis filters of Fig. 17; and
Figs. 20A and 20B illustrate the construction and operational principles of a sensor device utilizing an environmental sensitive filter according to the invention
DETAILED DESCRIPTION OF A PREFERRED EMBODIMENT
Figs. 1A-1D illustrate the main principles of the prior art technique applied for mmufacturing the waveguide structure 10 shown in Fig. IE. Fig. IF illustrates the fabrication of the further structure 20 on top of the structure 10, so as to obtain a three-dimensional integrated optical device. This technique will unavoidably require
a planarization procedure to be appKed to the uppermost layer, of the first structure 10 to allow the deposition of the second structure 20 thereon.
Referring to Figs. 2A and 2B, a prior art ridge waveguide structure Si (Fig. 2A) is compared to a waveguide structure WS2 of the present invention.(Fig. 2B) According to the prior art techniques, a ridge 202 was patterned from a core material - Layer 1, which is dielectric or semiconductor material with a ref active index higher than that of the underiymg buffer layer (S1O2). For example, the refractive indices of Layer 1 and the underlying buffer layer may be 1.475 and 1.46, respectively. As a result, the height of the ridge 202 has to be a substantial percent of the height of a waveguiding element (e.g., a 3-μηι ridge of the total 6-μτη wavegdding element).
As shown in Fig. 2B, according to the technique of the present invention, a thin layer of a different material (dielectric or semiconductor), is deposited on top of a layer 201 (Layer 1), and is utilized for fabricating a ridge 203 with a decreased height The resulting ridge part of the waveguide is much thinner in the vertical dimensions than the ridge part of state of the art ridge waveguide.
Figs. 3A-3C illustrate the mode profiles (optical fields) of three different light guiding structures. Fig 3A shows the optical mode of the prior art waveguide structure 10 shown in Fig. IE, Fig. 3B shows the optical mode of the prior art waveguide structure WSi shown in Fig. 2A, and Fig. 3C shows the mode of the waveguide structure WS2 of the present invention shown in Fig. 2B. The resulting mode profile in all cases is adaptable to fiber optic coupling, and hence can be used in integrated optical circuits.
Referring to Figs. 4 and 5A-5E, there is illustrated one embodiment of the present invention. Fig. 4 shows an integrated optical device 30 composed of a ridge waveguide 32 optically coupled to a ring resonator 34. Ridge waveguides are commonly used in semiconductor-based optical waveguides, while being less commonplace in silica-based waveguides. The integrated optical device 30 can be used as a filter in signal processing applications. To this end, the coupling between the ring resonator 34 and a pair of buried channel waveguides is typically provided,
only the lower buried layer being shown in Fig. 4. The buried channels serve as input/output bus guides, while the ring functions as the frequency selective element At the resonance, power can be substantially transferred from the input port to the drop port.
In the present example, the. bottom layer waveguides are realized as buried ridge waveguides, with the ridge material being chosen as high index material. Figs. 5A-5E illustrate the main manufactoing steps of a method according to the invention used for fabricating the structure definition 30. Fig. 5A shows an initial structure 35 obta: - ad by the deposition of a buffer layer 36 of a thickness about ΙΟμπι onto a substrate 38 (usually Silica over Silicon), and deposition of a layer 39 of doped S1O2, e.g., (Si02+Ge) onto the buffer layer 36. The layer 39 has a refractive index higher than that of the buffer layer 36 (e.g., 1.475 of layer 39 compared to 1.46 of buffer layer 36). The deposition can be of PECVD, LPCVD or another kind.
Then, a dielectric or a semiconductor layer 40 with a higher refractive index (e.g., in the range of 1.51-2.00), as compared to that of the buffer layer 36, is deposited on the upper surface of the layer 39 (Fig. 5B). Specific examples of such a dielectric material include, but are not limited to, Smcone-OxyNitride, doped S1O2, Ta.205, poly silicon, amorphous silicon, Y2O3 (Yitterium Oxide).
The thickness of this guiding layer 40 in which a ridge 42 is formed depends on the difference in the refractive indices of the dielectric and buffer layers. At a further manufacturing step (Fig. 5C), the ridge 42 is created in the layer 40. According to the present invention, a high refractive index dielectric or semiconductor material is used to create the ridge. The height of the ridge is designed so that, after the deposition of the next cladding layer, the combined perturbation is typically smaller than 200nm.
To create the ridge 42, the ridge material 40 (dielectric or sem conductor) is covered by photoresist material (not shown), the waveguide surroundings are exposed, and etching is carried out to define the ridge(s) for the waveguide(s). It should, however, be noted that these steps can be replaced by a lift off procedure,
wherein, first, the photoresist is applied and the waveguide structure is exposed, and, then, the ridge material is deposited.
Thereafter, a further buffer (serving as a cladding) layer 44 is deposited (Fig. 5D), which may be of the same composition as the first buffer layer 36. A height difference Ah of the height of a region of layer 44 above the ridge 42 and a region of layer 44 outside the ridge 42 (Fig. 4) is small, typically equal to or less than the height of the ridge (e.g., less than 200nm). This step thereby results in that the top layer 44 is flattened to less man 200nm, which is suitable for the direct formation of an additional waveguiding structure, i.e., dielectric ring resonators 34 in the present example (only one such resonator being shown here). To this end, a high index dielectric or semiconductor material is deposited (such as S13N4, Ta20s, Si), and masking of the ring structure 34 is carried out by photoUthography. Then, the ring structure undergoes anisotropic etching. Finally, a further burying layer 46 is deposited, usually with the same composition as the buffer layer 36 (i.e. SiO_>). By this, significant perturbations of light propagation in the additional waveguiding structure are prevented.
Reference is now made to Figs. 6 and 7A-7E illustrating a three-dimensional optical coupler 50 formed by a combination of an overlay layer with a waveguide structure (Fig. 6), and the main manufacturing steps in a method of its fabrication (Figs. 7A-7E). To facilitate understanding, the same reference numbers are used for identifying those stractural elements, which are common in the examples of Figs. 5A-5E and 7A-7E.
Fig. 7A-7D show manufacturing steps which are similar to those of Figs. 5A-5D. Namely, me dielectric or semiconductor layer 40 is deposited on the stack-structure 35 formed of the substrate layer 38 (Si), buffer layer 36 (Si02) and doped silicon layer 39 (Si02+Ge). The guiding layer 40 has a higher refraction index (e.g., in the range of 1.51-2.00), as compared to the index of ref action of the buffer layer 36, the thickness of the layer depending on the index of refraction difference. Tnis guiding layer may be formed from Silicone - OxyNitride, doped S1O2, Ta2Os, YO (Yitterium Oxide). Then, the ridge 42 is created in the high refraction index layer
40 (Fig. 5C), and the buffer layer 44 is deposited on the outer surface of the so-obtained structure (Fig. 5D).
At further manufacturing steps, the following procedures are carried out: Further doped silicon layer 48 (Si02+Ge) and dielectric layer 49 are sequentially deposited. The dielectric layer has .either a slightly higher refraction index than the buffer layer (e.g., Silicone OxyNitride, doped S1O2, Ta205, YO), or a much higher refraction index (e.g., S13N4 with the index of refraction being 2.00). Photolifliography and etching are sequentially applied for, respectively, masking and defining a waveguide 52. Finally, a burying layer 54 (e.g., S1O2) is deposited.
An alternative embodiment of the invention relates primarily to coaling of waveguides and ring resonators. According to this technique, the ring structures are first fabricated (which are relatively thin due to their high refractive index), and then the regular waveguides are defined in the overlay structure. By utilizing relatively broad waveguides with a small refractive index difference, a higher tolerance to potential perturbations in the waveguide structure can be achieved, as a consequence of the residual perturbations of the underlying ring structure.
The above approach is exemplified in Figs. 8 and 9A-9E, wherein Fig. 8 illustrates a complete structure 60 fabricated by sequentially performing the steps shown in Figs. 9A-9E.
Initially, a buffer layer 36 is deposited on a substrate 38 (usually Silica over
Silicon), using PECVD, HPCVD or other deposition methods. Deposited on the buffer layer 38 is a dielectric layer 40 with a much higher refraction index (e.g., S13N4). The thickness of the guiding layer 40 depends on the refractive index difference, but can be a few hundred nanometers.
Photohthography is performed to mask the waveguides of the ring structures
34, and anisotropic etching is applied to define the waveguides for the ring structures (Fig. 9C).
Thereafter, a S1O2 buffer layer 62, and a dielectric 64 with a slightly higher refractive index (e.g., in the range of 1.48-1.51) than that of the S1O2 layer are sequentially deposited. This dielectric material may, for example, be Silicone
Oxy itride, or S1O2 with a Ge or other doping. Then, the deposition of a photoresist material (not shown), and subsequent exposure and development are carried out to define the waveguides 68; By performing anisotropic etching of the guiding layer, the waveguides are defined. A further S1O2 upper cladding layer 66 is deposited on the so-obtained structure (Fig. 9E) to enable the fabrication of a furmer layer arcMtedure of the entire structure 60 (Fig. 8).
The following are some possible examples of integrated optical devices that can be manvjfactured by the above-described methods. It should be noted, although not specifically shown in the figures, that all devices manufactured by the invented technique can be tuned or switched by changing the device temperature using the mermooptic effect This can be implemented by depositing microresistors (made of Cr, Ni-Cr, PolySilicone, etc.) on top of the multi-layer structures and applying electric current to the microresistors.
Figs. lOA-lOC iUustrate ring resonator based filters o£ respectively, one, two and three rings. As shown, one or more ring waveguides are accommodated between two linear waveguides, each ring waveguide being optically coupled to the linear waveguides. Each ring resonator is an optical filter, and, by combining them in parallel, high order filters can be obtained. The examples of Figs. 10B and IOC present a combination of two spaced-apart linear waveguides and two and three spaced-apart resonator-cavity loops, respectively. The resonator-cavity loops are accommodated between the two linear waveguides and are connected to each other through sections of the linear waveguides, such at least two spaced-apart resonator-cavity loops and the waveguide sections creating a closed loop compound resonator for storing optical energy of a predetermined f equency range. The physical characteristics of the compound resonator are control
adjust the optical storage characteristics of the compound resonator.
Fig. 11 illustrates the optical spectral response of the ring resonator based filters. Graphs Gi, <¾ and (¾ correspond, respectively, to one-, two- and three-ring filters.
Optical Add Drop Multiplexer
Figs. 12A and 12b iUust^
features, respectively, of a single channel Optical Add Drop Multiplexer (OADM), generally designated 70. The OADM 70 is composed of two compound resonators 72 and 74, each constructed as described above, namely, including two ring-resonators accornmodated between and coupled to two linear waveguides. Here, each ring resonator is an optical filter, and, by combining them in parallel, high order filters are obtained. The drop port (filter) is implemented using a double filter pass, while the add port is obtained with a- single filter.
Fig. 13 illustrates a four port add drop multiplexer. Here, multiple channel
OADMs are obtained by cascading the structures of Figs. 12A-12B. In a real system, four blocks D are followed by four blocks A.
Fig. 14 illustrates an example of the integration of switches and add drop filters for switch-able filters. Here, optical switches are added to insert and extract the ring based OADM fiom the optical path to aUowm^ess operation - not disturbing u e through channels while tuning the OADM filters.
Interleaved Filters
Interleave filters are typically employed to achieve tight channel spacing in optical cormnunication systems. As shown in Fig. 15A, such a filter accepts an incoming signal composed of optical channels with a small frequency spacing and distributes the input channels amongst output waveguides in a circular function. Spectral functionality of this interleaved filter is shown in Fig. 15B. The output frequencies have a wider frequency spacing, resulting in wider tolerances from the optical elements. Interleaved filters are critical elements in achieving very tight frequency spaced optical channels.
Ring resonators are ideal candidates for implementing an interleave filter in a planar tigihtwave circuit A particular embodiment is obtained by using a ring resonator with a free spectral range (FSR), which is equal to the desired output frequency spacing. FSR is the frequency at which the response of an optical filter repeats itself.
Fig. 16A illustrates a single channel separatio element (filter) utilizing ring resonators optically coupled to linear waveguides. As shown in Fig. 16B, by combining four single stage filters (SSF) of Fig. 16A, the interleaved filter of Fig. 15A can be obtained
Optical Spectrum Analyzer .
The real time monitoring of optical networks poses the foUowing challenges for spectral analysis systems: high resolution; short spectrum acquisition time; low cost; low loss on the optical link; and small size. In standard spectrum analyzers, where the wavelength separation element is based on gratings, high resolution implies larger size and higher cost An alternative would be to use tunable filters to scan across the optical spectrum of interest. However, existing tunable filters are limited in their ability to provide me reqjm-ed resolution.
The technique of the present invention provides for manufacturing a compound high Q optical ring resonator structure operable as a filter, which is used in the analysis of optical spectra.
Fig. 17 illustrates a spectral analysis filter 80 associated wit a detector 82. The filter 80 comprises two compound resonators 80A and 80B connected in parallel through a common linear waveguide W2, and serves as a compound high Q optical ring resonator slructure. The output linear waveguide W3 of the structure is connected to the detector 82. The Q of the filter is determined by the coupling factor describing the amount of light that is coupled into the filter at every round trip. The Q factor is also determined by the optical losses in the cavity and the ring radius.
Fig. 18 illustrates a tap coupler and spectral analysis system, generally designated 90, utilizing the combination of the spectral analysis filter 80 and detector 82. The filter 80 is connected to an optical network (hnk) 84 via a coupler 86, which taps a small amount of light, thereby minimizing the losses incurred in the optical link.
Fig. 19 illustrates a spectrum analyzer 100 utilizing several spectral analysis filters - three such filters 110A, HOB and HOC in the present example, used in parallel through a common input linear waveguide Wi. Each filter has a different
radius, as compared to the others, and therefore is capable of carrying out a spectral analysis on a different portion of the communications spectrum. This feature is associated with, two problems that may occur when using ring resonators, namely, limited timing range and limited free spectral range, resulting in that a different approach has to be adopted to scan across a wide spectrum. In addition, this parallel approach provides for reducing the scan time required to approach all frequency channels of the communications spectrum.
Sensor
A high Q optical filter can- be used as a very sensitive sensor for various applications, such as a biological, mechanical, or temperature sensor. To this end, the filter characteristics depend on the external element to be measured. Fig. 20A illustrates a sensor device 200 comprising an environmental sensitive filter 210 constructed as the above-described compound resonator, which is connected to a laser 212 and a detector 214 through its input and output waveguides Wi and W2, respectively. Such a high Q optical filter structure is used as a sensor, which is suitable for various applications, such as a biological, mechanical, or temperature sensor. This is due to the fact that the filter characteristics depend on the external element to be measured. Fig. 20B shows the results of tuning the laser 212 to the edge of the filter 210. Generally speaking, the environmental element changes the resonance frequency of the filter, which results in a change of the optical power at the detector. With proper calibration, this device can be used to measure or monitor various physical, mechanical or biological enwonmental changes.
Those skilled in the art will readily appreciate that various modifications and changes can be applied to the preferred embodiments of the invention as hereinbefore exemplified without departing from its scope defined in and by the appended claims.
Claims (20)
1. A method of fabricating an integrated optical device comprising a structure including at least one waveguiding element, the method comprising the steps of: (i) providing a basic structure that comprises a substrate material and a buffer material layer on surface of said substrate; (ii) providing said at least one waveguiding element on said substrate, wherein said waveguiding element is made of a guiding material with a refractive index higher than the refractive index of said buffer ayer; the method being characterized in that: (Hi) a core material layer, having a refractive index higher than that of the buffer layer and smaller than that of the guiding layer, is deposited on surface of the buffer layer for carrying said at least one waveguiding element on the surface thereof; (iv) said at least one waveguiding element is formed by patterning the guiding layer on top of said core material layer, said guiding material with the refractive index higher than the refractive indices of said buffer layer and said core layer allowing to minimize a height of said at least one waveguiding element and to provide effective guiding of light in the core layer; (v) a cladding layer is formed on surface of a structure obtained in step (iv), wherein a height difference between a height of the cladding layer region above said at least one wavegmding element and a height of the cladding layer region outside the waveguiding element is substantially small, thereby providing a sufficient flatness of the surface of the cladding layer to allow direct formation of a further waveguide structure thereon and prevent significant perturbation in light propagation within said further, waveguide structure.
2. The method according to Claim 1, wherein said height difference is in the order of several hundreds nanometers.
3. The method according to Claim 1, wherein said height difference substantially does not exceed a thickness of said guiding layer.
4. The method according to Claim 1, wherein a thickness of said guiding layer substantially does not exceed 200nm.
5. The method according to Claim 1, wherein said guiding layer is dielectric or semiconductor.
6. The method according to Claim 5, wherein said core material is doped S1O2 formed on the surface of the basic structure including S1O2 on Si, and said guiding layer is made of at least one material from the following Ust: Silicone-OxyNitride, doped S1O2, Ta2O5, poly silicon, amorphous silicon and Y2O3 (Yitterium Oxide).
7. The method according to Claim 1, wherein said at least one waveguiding element of each waveguide structure is in the form of a ridge waveguide.
8. The method according to Claim 7, wherein the formation of said at least one waveguiding element comprises the following steps: - depositing said guiding layer material with the higher refraction index onto the external surface of said core material layer, said guiding layer material being a dielectric or semiconductor; - depositing a photoresist material onto said guiding layer material with the higher refraction index; - selectively exposing the photoresist to define a site for said at least one waveguiding element; and - applying etching to define said at least one waveguiding element
9. The method according to Claim 7, wherein the formation of said at least one waveguiding element comprises the following steps: - applying a photoresist layer to the surface of said core material layer; - selectively exposing the photoresist to define a site for said at least one waveguiding element; and - depositing said guiding material with the higher refraction index, said guiding material being a dielectric or semiconductor.
10. The method according to Claim 6, wherein said layer of doped S1O2 is Germanium (Si02+Ge).
11. The method according to Claim 1, further comprising the steps of: - forming said further waveguide structure on top of a structure obtained in step (v).
12. The method according to Claim 11, wherein the formation of said further waveguide structure comprises the steps of: - depositing an additional buffer layer on the surface of the structure obtained in step (v); - depositing on the surface of said additional buffer layer, an additional core material layer of a higher refraction index as compared to mat of the additional buffer layer - forming at least one waveguiding element of said further waveguide structure by patterning an additional guiding layer deposited on the surface of said additional core material layer, wherein said additional guiding layer is made of a material with a refraction index higher than the refraction indices of said additional buffer layer and said additional core material layer, such that said additional guiding 1 layer is substantially Ihin; and - forming a further cladding layer.
13. The method according to Claim 12, wherein said at least one waveguiding element of the lower waveguide structure is a ridge waveguide, and said at least one waveguiding element of said further waveguide stractoe is a ring resonator.
1 . The method according to Claim 12, wherei said at least one waveguiding element of the lower waveguide structure is a ring resonator, and said at least one waveguiding element of said further waveguide structure is a ridge waveguide.
15. An integrated optical device comprising at least one structure having at least one waveguiding element, the device comprising: - a basic structure having a substrate material and a buffer material layer on surface of said substrate ; and - said at least one waveguiding element carried by the basic structure; the device being characterized in that: - a core material layer of a higher refraction index as compared to that of the buffer layer is located between the buffer layer and said at least one waveguiding element; 5 - said at least one waveguiding element is made of a material with a refractive index higher than the refractive indices of said buffer layer and said core layer, to thereby nunirnize a height of said at least one waveguiding element and to provide effective guiding of light in the core layer; 10 - a cladding layer is formed on the surface of a structure with said at least one waveguiding εΐεπιεηζ wherein a height difference between a height of the cladding layer region above said at least one waveguiding elei nt and a height of the cladding layer region outside the waveguiding element is substantially small, the cladding layer thereby having a desired flatness. 15
16. The device according to Claim 15, operabk as an optical frequency dependent switch.
17. The device according to Claim 15, operable as an optical tunable filter.
18. The device according to Claim 15, operable as an Optical Add Drop Multiplexer (OADM). 20
19. The device according to Claim 15, operable as a spectral analyzer.
20. The device according to Claim 15, operable as a sensor. For the Applicants REINHOLD COHN AND PARTNERS By 5
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IL151095A IL151095A (en) | 2000-04-24 | 2002-08-06 | Multilayer integrated optical device and a method of fabrication thereof |
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IL13580600A IL135806A0 (en) | 2000-04-24 | 2000-04-24 | A multi layer integrated optical device and a method of fabrication thereof |
US23206100P | 2000-09-12 | 2000-09-12 | |
PCT/IL2001/000379 WO2001081962A2 (en) | 2000-04-24 | 2001-04-24 | A multilayer integrated optical device and a method of fabrication thereof |
IL151095A IL151095A (en) | 2000-04-24 | 2002-08-06 | Multilayer integrated optical device and a method of fabrication thereof |
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EP (1) | EP1248960B1 (en) |
AT (1) | ATE251761T1 (en) |
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AU2002343192A1 (en) | 2001-10-25 | 2003-05-06 | Lambda Crossing Ltd. | Polarization insensitive tunable optical filters |
US6888973B2 (en) | 2001-11-14 | 2005-05-03 | Massachusetts Institute Of Technology | Tunable optical add/drop multiplexer with multi-function optical amplifiers |
US6888854B2 (en) | 2002-07-03 | 2005-05-03 | Lambda Crossing Ltd. | Integrated monitor device |
US20040081386A1 (en) * | 2002-10-25 | 2004-04-29 | Morse Michael T. | Method and apparatus for modulating an optical beam with a ring resonator having a charge modulated region |
US7356219B2 (en) * | 2002-12-31 | 2008-04-08 | Pirelli & C. S.P.A. | Integrated optical add/drop device having switching function |
US7030991B1 (en) | 2003-08-01 | 2006-04-18 | Ball Aerospace & Technologies Corp. | Field condensing imaging system for remote sensing of atmospheric trace gases |
US7050215B1 (en) | 2003-08-01 | 2006-05-23 | Ball Aerospace & Technologies Corp. | Method and apparatus for providing a gas correlation filter for remote sensing of atmospheric trace gases |
US7145660B2 (en) * | 2003-08-13 | 2006-12-05 | Lambda Crossing, Ltd. | Micro-resonator based optical sensor |
JP4779886B2 (en) * | 2006-08-31 | 2011-09-28 | 日本電気株式会社 | Tunable laser |
US9582726B2 (en) * | 2015-06-24 | 2017-02-28 | Qualcomm Incorporated | Systems and methods for image processing in a deep convolution network |
JP7211017B2 (en) | 2018-11-02 | 2023-01-24 | 株式会社デンソー | Optical filter, laser light source and optical transmitter/receiver using the same |
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US4720160A (en) | 1981-12-16 | 1988-01-19 | Polaroid Corporation | Optical resonant cavity filters |
BR8208023A (en) | 1981-12-16 | 1983-11-22 | Polaroid Corp | DEVICE FOR TRANSFERING LIGHT ENERGY AND FILTER FOR LIGHT ENERGY |
DE197943T1 (en) | 1984-10-01 | 1987-02-05 | Polaroid Corp., Cambridge, Mass. | VERST (GAMMA) RKER FRR OPTICAL WAVE GUIDE AND LASER. |
FR2596529B1 (en) | 1986-03-28 | 1988-05-13 | Thomson Csf | OPTICAL WAVEGUIDE IN SEMICONDUCTOR MATERIAL, LASER APPLYING THE SAME AND WAVEGUIDE |
FR2658307A1 (en) | 1990-02-13 | 1991-08-16 | Thomson Csf | INTEGRATED OPTICAL WAVEGUIDE AND METHOD FOR MAKING THE SAME. |
GB9202463D0 (en) | 1992-02-05 | 1992-03-18 | British Telecomm | Silica waveguide structure |
US5586206A (en) * | 1994-09-09 | 1996-12-17 | Deacon Research | Optical power splitter with electrically-controlled switching structures |
US5544268A (en) * | 1994-09-09 | 1996-08-06 | Deacon Research | Display panel with electrically-controlled waveguide-routing |
US5581642A (en) * | 1994-09-09 | 1996-12-03 | Deacon Research | Optical frequency channel selection filter with electronically-controlled grating structures |
US5647036A (en) * | 1994-09-09 | 1997-07-08 | Deacon Research | Projection display with electrically-controlled waveguide routing |
US5911018A (en) * | 1994-09-09 | 1999-06-08 | Gemfire Corporation | Low loss optical switch with inducible refractive index boundary and spaced output target |
GB2306694A (en) | 1995-10-17 | 1997-05-07 | Northern Telecom Ltd | Strip-loaded planar optical waveguide |
US6052495A (en) | 1997-10-01 | 2000-04-18 | Massachusetts Institute Of Technology | Resonator modulators and wavelength routing switches |
WO2001022141A1 (en) | 1999-09-21 | 2001-03-29 | Nanovation Technologies, Inc. | Wavelength-slicing architecture for wavelength demultiplexing using micro-ring resonators |
EP1221069A1 (en) | 1999-10-14 | 2002-07-10 | Lambda Crossing Ltd | An integrated optical device for data communication |
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WO2001081962A3 (en) | 2002-02-07 |
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