CA2153485A1 - Low-loss integrated circuits - Google Patents
Low-loss integrated circuitsInfo
- Publication number
- CA2153485A1 CA2153485A1 CA002153485A CA2153485A CA2153485A1 CA 2153485 A1 CA2153485 A1 CA 2153485A1 CA 002153485 A CA002153485 A CA 002153485A CA 2153485 A CA2153485 A CA 2153485A CA 2153485 A1 CA2153485 A1 CA 2153485A1
- Authority
- CA
- Canada
- Prior art keywords
- optical
- substrate
- integrated circuit
- forming
- waveguide
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
Classifications
-
- 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
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y20/00—Nanooptics, e.g. quantum optics or photonic crystals
-
- 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
- G02B6/12004—Combinations of two or more optical elements
-
- 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
- G02B6/1225—Basic optical elements, e.g. light-guiding paths comprising photonic band-gap structures or photonic lattices
-
- 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
- G02B6/125—Bends, branchings or intersections
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/2005—Electromagnetic photonic bandgaps [EPB], or photonic bandgaps [PBG]
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
- H01S5/11—Comprising a photonic bandgap structure
Abstract
An optical circuit and a method for substantially eliminating radiation losses associated with optical integrated circuits and, in particular, bends in optical waveguides, is disclosed. The circuit and waveguide are fabricated on a substrate having a periodic dielectric structure. The periodic dielectric structure exhibits a range of frequencies of electromagnetic radiation which cannot propagate into the structure. The range of frequencies is known as a photonic band gap or frequency band gap. Radiation at a frequency within the frequency band gap of the structure is confined within the circuit and waveguide by the periodic dielectric structure surrounding the circuit and waveguide. Radiation losses are substantially eliminated.
Description
_~9411~45 2 1 S 3 ~ 8 5 PCT~S94/00285 LOW-LOSS OPTICAL AND OPTOELECTRONIC
INTEGRATED CIRCUITS
Backqround of the Invention Optical integrated circuits and optoelectronic integrated circuits are usually fabricated on the top surface of a uniform substrate. These circuits can experience optical losses as light propagates away from the circuits and into the uniform substrate. It is desirable to produce optical and optoelectronic integrated circuits as compact as possible on a sub-strate to produce small lightweight circuits. How-ever, losses experienced by the interconnects between circuits tend to inhibit the reduction of the overall system size.
Interconnects in optical integrated circuits and optoelectronic integrated circuits are achieved by using waveguides to transport light from one optical device to another. Waveguides are also the basis of numerous optical devices including optical couplers, switches, modulators, power dividers and combiners.
Light propagating through an optical waveguide is contained within the waveguide by total internal reflection. The medium outside the waveguide has a lower index of refraction than does the interior of the waveguide. The boundary between the interior and exterior of the waveguide is characterized by a crit-ical angle determined by the ratio of the refractive indices or index contrast of the two media. The cri-tical angle of the boundary can be defined as the angle below which light inside the waveguide must strike the boundary in order to be reflected back into the waveguide rather than be transmitted through W094/1~45 ~ ~5 3 4 8 PCT~S94/00285 the boundary and out of the waveguide. Light inside the waveguide which strikes the boundary at an angle smaller than the critical angle cannot pass through the boundary and is reflected back into the wave-guide.
Since nearly all of the light traveling through a straight optical waveguide strikes the waveguide boundary at very small angles, very little loss is suffered. However, in fabricating optical and opto-electronic integrated circuits, it is necessary tomake optical waveguides with bends. Also, certain devices such as optical couplers require bends in their waveguides. Unlike straight waveguide sec-tions, waveguide bends can produce significant loss-es. As the light traveling through the waveguideenters a bend, it strikes the boundary at a larger angle than it does in a straight section. If the index contrast does not provide a large enough criti-cal angle, some of the light escapes from the wave-guide, thus introducing bend loss.
Bend losses have proven to be a substantial im-pediment to the development of optical and opto-electronic integrated circuits. To minimize losses, bends must be made with large radii of curvature, typically on the order of 10mm. Such large bend radii are not practical for compact optical and opto-electronic integrated circuits.
Numerous approaches have been suggested to mini-mize bend losses. One of these is the use of abrupt bends rather than curved bends. Abrupt bends have sharp corners joining two straight sections of wave-- guide. The drawback to abrupt bends is that the bend angle must be very small, on the order of 1 degree.
_~94/1~4~ 21 S3~8 PCT~S94/~5 So, this approach contributes little to making cir-cuits more compact.
Another approach has been to grade the index of refraction of the substrate in the area of the bend to maintain internal reflection around the bend.
Combinations of these two approaches have also been suggested. However, no present approach appears to be able to substantially reduce the radii of curva-ture of waveguide bends to facilitate the development of compact optical and optoelectronic integrated circuits.
SummarY of the Invention The present invention is an optical circuit and a method which substantially eliminates radiation losses in optical integrated circuits. The circuit is formed on a surface of a substrate made of a semi-conductor or other type material including dielectric and optical materials. The substrate comprises a region which is characterized by a frequency band gap. The frequency band gap is a band of frequencies at which electromagnetic radiation and, in particu-lar, light waves cannot propagate through the region.
The circuit is formed in the region having the fre-quency band gap such that radiation which would otherwise escape from the circuit into the substrate cannot propagate into the substrate.
The circuit of the present invention experiences reduced radiation losses at frequencies within the band gap of the substrate. In particular, losses at waveguide bends are substantially eliminated. Some of the light traveling through a waveguide bend strikes the boundary between the interior and the exterior of the waveguide at angles greater than the WO94/1~45 PCT~S94/~5 2~s3485 critical angle and would otherwise tend to escape from the waveguide into the substrate. However, in the present invention, the bend is formed in the region of the substrate with the frequency band gap.
Light at a frequency within the band gap cannot pro-pagate into the substrate. The light is confined within the optical circuit and the waveguide.
The region of the substrate with the frequency band gap has a periodic dielectric structure. A
periodic dielectric structure is a structure which exhibits a periodic spatial variation in dielectric constant. As applicable to the present invention, the variation in dielectric constant may be periodic in either two-dimensional or three-dimensional space within the structure.
There are various methods of forming such struc-tures. One of these methods involves forming a peri-odic pattern of holes in a uniform substrate ma-terial. Another is removing substrate material such that what remains is a periodic pattern of cylindri-cal or other similarly shaped rods of substrate mate-rial.
There are also various methods of forming an optical waveguide on the substrate. In one embodi-ment, an epilayer of material of high refractiveindex is formed on top of a substrate having a lower index. Next, the periodic dielectric structure is formed on opposite sites of a channel in the epilayer of uniform material. The channel is shaped as de-sired to serve as the waveguide. The periodic di-electric structure on either side of the channel prevents radiation into the substrate. Thus light is guided through the channel by the periodic dielectric structure. Light is confined vertically within the ~94/1~45 PCT~S94100285 2l~3~8s channel by internal reflection due to the index con-trast between the waveguide in the epilayer and the air on top and between the waveguide and the sub-strate on the bottom. In other embodiments, a mate-rial having a higher index of refraction than the substrate may be diffused into the substrate or etched on the substrate. Alternatively, a material of higher refractive index may be deposited by sput-tering, evaporation or other process onto the surface of the substrate. Another method involves forming a pair of trenches in a high-refractive-index layer deposited on the top surface of the substrate. The material between the trenches serves as the optical waveguide. The air in the trenches is the low-refractive-index exterior medium which provides la-teral internal reflection due to index contrast.
Periodic dielectric structure is provided on the out-side of the trenches to eliminate loss where the re-quirements for internal reflection are not met. Ver-tical losses are eliminated by internal reflectiondue to the refractive index contrast.
The present invention provides substantial ad-vantages over previous methods of reducing loss in optical circuits and in optical waveguide bends.
Unlike previous approaches, it is the substrate it-self which prevents radiation from escaping into the substrate. The present invention does not rely upon physical constraints of a waveguide such as the bend angle, as in the abrupt bend approach. In the pre-sent invention, the waveguide bend radius can bearbitrarily small because it is the substrate which - is preventing loss. Also, the index grading approach relied on the index contrast between the waveguide and the substrate to maintain internal reflection.
W094/1~45 4~ PCT~S94/~5 Even with index grading, a critical angle is present - which constrains the radius of curvature. Because the present invention does not rely solely on index contrast and internal reflection at bends, the radius of curvature at the bend is not so constrained.
Because waveguide bend radii are reduced, opti-cal and optoelectronic circuits can be made much more compact and light weight. These circuits can be to-tally integrated. Different optical devices and in-terconnects can be fabricated on a common substrate.High-speed electronics can be fabricated on the same chip as associated optoelectronic devices.
Brief Descri~tion of the Drawinqs The foregoing and other objects, features and advantages of the invention will be apparent from the following more particular description of preferred embodiments of the invention, as illustrated in the accompanying drawings in which like reference charac-ters refer to the same parts throughout the different views. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating the principles of the invention.
Figure la is a schematic perspective view of a prior art optical circuit.
Figure lb is a schematic perspective view of another prior art optical circuit.
Figure 2a is a schematic perspective view of a prior art uniform substrate with a rib waveguide sec-tion having a bend.
Figure 2b is a schematic top view of the wave-guide section of Figure 2a.
~94/1~45 1 ~ 3 ~ 8 S PCT~S94/~5 Figure 3 is a graph of the loss associated with a 90 circular waveguide bend versus the radius of curvature of the bend for two propagation modes.
Figure 4 is a schematic perspective view of a periodic dielectric structure having two-dimensional periodicity.
Figure 5a is a schematic top view of the per-iodic dielectric structure of Figure 4 showing a triangular lattice pattern.
Figure 5b is a schematic top view of a periodic dielectric structure showing a square lattice pat-tern.
Figure 5c is a schematic top view of a periodic dielectric structure showing a hexagonal lattice pat-tern.
Figure 6 is a graph of the wave attenuation inthe band gap versus frequency of the wave.
Figure 7a is a schematic perspective view of an optical circuit in accordance with the present inven-tion.
Figure 7b is a schematic top view of the opticalcircuit of Figure 7a.
Figure 8a is a schematic perspective view of a waveguide section on a substrate having a two-dimen-sional periodic dielectric structure in accordancewith the present invention.
Figure 8b is a schematic top view of the device of Figure 8a.
Figure 9 is a schematic perspective view of a waveguide on a substrate having a three-dimensional periodic dielectric structure in accordance with the present invention.
Figure 10 is a schematic top view of an S-bend in accordance with the present invention.
W094/1~45 PCT~S94/0028~
21~3~85 .
Figure 11 is a schematic top view of a Y-coupler in accordance with the present invention.
Figure 12 is a schematic top view of a waveguide taper in accordance with the present invent:ion.
Detailed Description of the Invention Optical integrated circuits and optoelectronic integrated circuits can be classified as either ac-tive or passive circuits. Optical integrated cir-cuits perform a variety of passive functions, includ-ing switching and modulating, without generating ordetecting light. Optoelectronic circuits generate and detect light as well as perform certain passive functions. The present invention is applicable to both types of circuits.
It should be noted that throughout this appli-cation, the terms "optical integrated circuits", "op-toelectronic circuits", "optical circuits", and other related terms will be used to describe the various types of circuits to which the invention is appli-cable. Unless otherwise specifically stated, the use of one of these terms in this application does not limit the applicability of the description to that type of circuit. One term is selected over another for illustration purposes only. The present inven-tion is applicable to all of these circuits.
Optical circuits can be fabricated on a top sur-face of a substrate. The optical waveguides which connect the circuits can also be fabricated on the surface of the substrate. These optical waveguides consist of a channel having an index of refraction which is higher than the index of refraction of the surrounding substrate. Because of the index con-~94/1~45 PCT~S94100~5 21 S3~85 trast, light is guided along the channel by totalinternal reflection.
Optical waveguides are used to guide optical signals among the elements in optical and opto-electronic integrated circuits and are analogous tothe metallic lines used to guide electrical signals among electronic integrated circuits. They connect external optical devices such as fiber optic cables with internal optical devices such as switches, modu-lators, sources, and detectors. In addition, theyform the basic structural elements in numerous opti-cal devices including optical couplers, switches, modulators, power dividers, and combiners.
Integrated optical circuits and waveguides can be implemented by several different techniques. One prior art example is shown in Figure la. A substrate 10 is made of a material such as LiNbO3 having a low index of refraction. Optical circuits 11 and 13 are formed in the substrate 10 by techniques such as pho-tolithography, diffusion, ion i~plantation, etching and the like. The optical waveguide 12 is made of a material having a high index of refraction which may be formed by diffusing titanium into the substrate 10 .
Another type of integrated optical circuit and waveguide, commonly referred to as a rib waveguide, is shown in Figure lb. The rib waveguide 22 connects circuits 21 and 23. In this device, the optical channel 22 of high refractive index is formed on the top surface of a low-refractive-index semiconductor substrate 20. The substrate material may be GaxAl~l x~As or other similar material. The channel 22 may be formed of GaAs or other high-refractive-index ma-WO94/1~45 PCT~S94/~5 2ls3485 terial. The channel 22 is formed by depositing GaAs onto the surface of the substrate 20.
Figures la and lb illustrate straight waveguide sections 12 and 22. Light propagating through the waveguides strikes the barrier between the interior and exterior of the waveguides at small angles. Con-sequently, the light is confined within the wave-guides by total internal reflection. However, to be useful in optical integrated circuits applications, waveguides, at times, must include bends.
Figure 2a schematically depicts a section of a prior art rib waveguide 32 which includes a 90 cir-cular bend 34. The waveguide 32 is fabricated on the top surface 31 of a substrate 30 as described above in connection with Figure lb. Figure 2b is a sche-matic top view of the waveguide section 32.
For purposes of illustration, light is assumed to propagate through the waveguide 32 in the dir-ection indicated by arrows 35. It will be understood that the actual direction of propagation is im-material to the invention. The light travels through straight section 36 of the waveguide 32 and then enters bend 34. The light which remains within the waveguide after passing through the bend travels through straight section 38.
As light leaves the straight section 36 and en-ters the bend 34, it strikes the barrier 40 between the interior and the exterior of the waveguide at larger angles. Some of these angles exceed the crit-ical angle required for reflection determined by theindex contrast at the barrier 40. The light which exceeds the critical angle passes through the barrier 40, exits the waveguide 32, and propagates into the air around the waveguide and the substrate 30. This _~94/1~45 21S3~ PCT~S94/00285 lost light, represented by arrows 42 in Figure 2b, is the optical loss associated with the bend, or simply the bend loss.
As shown in Figure 2b, the bend 34 has a radius of curvature R. As R decreases, the angle at which light strikes the barrier 40 increases. More light escapes from the waveguide 32 causing increased bend loss. Experiments have shown that bend losses in-crease exponentially with decreasing bend radius of curvature. That is, L-~e~R/b, where L is the loss, R
is the radius of curvature, and a and b are con-stants.
Depending upon the application in which the waveguide is used, there is a certain maximum bend loss which can be tolerated. This maximum tolerable bend loss corresponds to a minimum allowable bend radius. Thus, bend loss imposes a restraint on the ability to reduce the size of the waveguide bend, and, consequently, on the ability to fabricate com-pact optical integrated circuits.
Figure 3 is a graph of experimental data whichdepicts a relationship between the radius of curva-ture of a 90 circular waveguide bend and the loss associated with that bend. Bend loss in decibels (dB) is plotted as a function of radius of curvature in millimeters (mm) for two modes of propagation.
Curve 44 is a quasi-transverse-electric mode, and curve 46 is a quasi-transverse-magnetic mode. The graph illustrates the exponential relationship be-tween bend radius of curvature and bend loss.
To eliminate the loss associated with opticaland optoelectronic integrated circuits as well as with waveguide bends, the present invention prevents light from propagating into the circuit substrate.
W094/1~45 PCT~S94/OOt85 2153~85 Because the light cannot propagate into the sub-strate, it is confined within circuit and the wave- -guide.
In the preferred embodiment of the present in-vention, the substrate comprises a region which has aperiodic dielectric structure. A periodic dielectric structure is a structure which exhibits a periodic spatial variation in dielectric constant. In one embodiment, the dielectric constant is periodic in two-dimensional space within the structure. In an-other embodiment, the structure exhibits three-di-mensional spatial periodicity.
The periodic dielectric structure is character-ized by a frequency or photonic band gap, or simply a band gap. The band gap of a periodic dielectric structure is a band of frequencies of electromagnetic radiation which cannot propagate through the struc-ture in the plane in which the structure exhibits periodic variation in dielectric constant.
Figure 4 is a schematic perspective view of a periodic dielectric structure 300 illustrating two-dimensional spatial periodicity. Specifically, the structure 300 is periodic in the x and z dimensions.
Therefore, electromagnetic radiation having a fre-quency within the band gap of the structure cannot propagate in a plane parallel with the x-z plane, including the plane of the top surface 326 of the structure.
The structure 300 includes a plurality of elon-gated elements 322 extending orthogonal to the sub-strate top surface 326 and bottom surface 328. The elements 322 are preferably cylindrically shaped and extend in a two-dimensional periodic arrangement relative to the x-z plane or any plane parallel ~94/1~45 21 ~3~ 85 PCT~S94/00~5 thereto. Although cylindrical elements are described - hereinafter, quasi-cylindrical elements or other shaped elongated elements may be employed. They may be formed of a non-conductive low-dielectric material disposed within a non-conductive high-dielectric sub-strate material 324. The elements 322 may simply be bores, voids, or channels which may be filled with low-dielectric fluids or solids such as air and/or other liquid or solid material.
In an alternative embodiment, the elements may be formed of non-conductive high-dielectric material and may be disposed in the periodic arrangement in a non-conductive low dielectric material. An example of this configuration is a high-dielectric substrate with material etched away to leave only the periodic arrangement of cylindrical rods of the high-di-electric material with air in the spaces between the rods. The space may also be filled with some other low-dielectric fluid or solid.
A longit~ axis 325 extends through the cen-ter of each element 322 in the vertical or y-direc-tion. The elements 322 are arranged periodically in two dimensions in the x-z plane which is generally orthogonal to the longitudinal axes 325 extending 25 through the elements 322.
The structure 300 can be positioned to filter incoming electromagnetic energy 329 polarized in any direction that is propagating in the x-z plane. The structure 300 reflects substantially all of the inci-dent electromagnetic energy 329 having a frequencywithin the range of the photonic or frequency band gap. More specifically, electromagnetic energy with-in the frequency range of the band gap is sub-stantially prevented from propagating through the WO94/1~45 - ~ PCT~S94/00285 2lS3485 structure 300. Thus, the structure 300 operates as a band stop filter. The structure maintains a sub-stantially constant band gap frequency range for radiation propagating along any incident angle in the x-z plane.
Figure 5a is a top view of the structure 300 of Figure 4. In this embodiment, the cylindrical ele-ments 322 are periodically arranged to provide a tri-angular lattice. The lines 327 illustrate the trian-gular lattice arrangement of the cylindrical elementsalong the top surface 326 of the substrate material 324. Other possible lattice structures are shown in Figures 5b and 5c. Figure 5b shows a square lattice structure, and Figure 5c shows a honeycomb or hex-agonal lattice structure.
A feature of the periodic dielectric structureis that the center frequency of the band gap, the bandwidth of the band gap (i.e., the stop band) and the band gap attenuation can be tailored for any frequency range in the microwave to ultraviolet bands (106 to 10l5 Hz) during the fabrication of the struc-ture. For the structure of Figures 4 and 5, the center frequency (f), the bandwidth (~f) and the band gap attenuation (A~) of the band gap are shown in Figure 6. The attenuation (AG) of the band gap is proportional to the number of rows of elements 322.
Thus, the attenuation (AG) can be increased by pro-viding additional rows. The center frequency (f) of the bandwidth (~f) can be computed in accordance with the following equation:
f = [13.8(13/~ ]/a GHz where 094/1~45 21 ~34~ PCT~Sg4/~5 ~ = dielectric constant of the substrate material, ~ = magnetic permeability of the substrate material, and a = triangular lattice constant which corres-ponds to the distance in centimeters between centers of adjacent elements.
The location of the band gap on the frequency scale is determined by the center frequency. The bandwidth (~f) is determined by the radius (r) of the cylindrical elements 322 and the triangular lattice constant (a).
A two-dimensional periodic dielectric structure as shown in Figures 4 and 5a-c may be fabricated on a portion of a homogeneous or uniform substrate by one of several methods. One method involves drilling holes in a high- dielectric uniform substrate. The holes are filled with a low-dielectric material such as air.
Another method involves the use of reactive-ion etching. The substrate is covered on one face with a mask which contains a two-dimensional array of geo-metric figures of the size, spacing, and periodicity required for the desired band gap. This two-dimen-sional array of geometric figures may be patterned by employing electron beam lithography or conventional photolithography. The geometric figures are either transparent or opaque to a reactive-ion etchant used - 30 to selectively eradicate the high dielectric sub-strate material. For example, if cylindrical air channels are to be formed in the substrate, the geo-metric figures are circles which are transparent to the etchant, and the remainder of the mask is opaque W094/1~45 ~ PCT~S94/~5 to the etchant. If square rods of high dielectric material are to be formed, the figures are squares which are opaque to the etchant, and the remainder of the mask is transparent to the etchant.
The substrate and mask are then exposed to the highly directional reactive-ion etchant. The re-- active-ion plasma is directed at the mask along the perpendicular axis, and vertical channels of the desired shape are created in the substrate. The resulting array of elements forms the two-dimensional frequency or photonic band gap.
Figure 7a is a schematic perspective view of cn integrated optical circuit 200 in accordance with the present invention. Figure 7b is a top view of the circuit 200. The circuit 200 comprises a base sub-strate 202 formed of a material having a low re-fractive index such as GaxAll~As. An epilayer 204 made of a material having a higher refractive index than the base substrate 202 such as GaAs is formed on the top surface of the base substrate 202. The com-bination of the base substrate 202 and the epilayer 204 forms the substrate 206 for the optical circuit 200.
The components of the optical circuit 200 in-clude two optical devices 208 and 210. These devicesmay be a laser and a detector or other similar de-vices. It will be understood that the invention is applicable to other such devices. Also, two devices are selected for ease of description only. Typical circuits will have more devices.
The devices 208 and 210 are connected by a wave-guide 212. The waveguide 212 includes a straight section 214, a bend 216 and a second straight section 218. For illustration purposes, light is assumed to )94/1~45 PCT~S94/~5 2 1 ~ 3 ~ 8 5 !
leave device 208 and propagate through the waveguide 212 toward device 210. The light passes through straight section 214, bend 216 and straight section - 218 and enters device 210.
The optical devices 208 and 210 are surrounded by periodic dielectric structure 222. The periodic dielectric structure 222 prevents emissions from the devices 208 and 210 at a frequency within the band gap of the structure 222 from propagating into the substrate 206. Thus, the devices 208 and 210 are isolated from each other, the waveguide 212, and any other devices on the substrate 206.
The periodic dielectric structure 222 also serves to define the lateral extents of the waveguide 212 on the epilayer 204. The periodic dielectric structure 222 prevents light at a frequency within the band gap of the structure 222 from propagating in the plane of the epilayer 204. Thus, the light is confined laterally within the waveguide 212. Light 20 is prevented from propagating out of the waveguide 212 in the vertical directions by internal re-flection. Light will not propagate up out of the waveguide into space because of the refractive index contrast between the interior of the waveguide and 25 the air above it. Light will not propagate down into the base substrate 202 because of the index contrast between the epilayer 204 and the base substrate 202.
Because the light cannot propagate outside the wave-guide 212, it is confined inside. The light entering the waveguide 212 from the device 208 travels through the straight section 214 into bend 216. It is guided around the bend 216 by the periodic dielectric struc-ture 222 and through straight section 218 into device 210.
WO94/1~45 - - PCT~S94/00285 2~534~5 The circuit 200 of Figures 7a and 7b is made by first forming the uniform high-refractive-index epi-layer 204 on top of a uniform low-refractive index base substrate 202 to form substrate 206. This is done by diffusion or similar fabrication technique.
Next, the devices 208 and 210 are formed on the epi-layer 204. Finally, the periodic dielectric struc-ture 222 is formed in the substrate 206 by one of the methods previously described.
The periodic dielectric structure 222 is de-signed to create a frequency band gap for the sub-strate 206 which includes the frequency of the radia-tion which will be carried by the waveguide 212. To create the structure 222, the periodic pattern of holes is formed in the substrate 206. The pattern of holes is made to surround devices 208 and 210 and to define the waveguide 212 connecting the devices. The holes are made by either drilling or by the reaction ion etching process previously described.
Figures 8a and 8b depict a section of waveguide 56 in accordance with another embodiment of the in-vention. A high-refractive-index epilayer 51 made of a material such as GaAs is formed on the top surface of a low-refractive-index base substrate 50 made of a -25 material such as GaxAllxAs to form a substrate 53. The substrate 53 may also be made of other materials such as di-electric or optical materials. The periodic di-electric structure 52 is periodic in two dimensions in the plane of the epilayer 51. The section of optical waveguide 56 is formed in the epilayer 51 between substantially parallel trenches 58 and 60.
The waveguide section 56 includes a 90 circular bend 62. The 90 bend angle is chosen for illustration _ 0 94/16345 1S31~5 ~/US94100285 purposes only. The bend angle need not be 90. The trenches 58 and 60 are formed by etching or other known processes. The air in the trenches provides refractive index contrast for internal reflection of the light carried by the waveguide 56. Periodic dielectric structure 52 is provided outside the tren-ches 58 and 60 to eliminate loss where the require-ments for total internal reflection are not met.
The periodic dielectric structure 52 is formed as described in connection with Figures 4-6 to have a frequency band gap at the known frequency of the light propagating in the waveguide 56. Therefore, the light cannot propagate into the substrate 53 in the plane of the epilayer 51. As a result, loss of light at the bend 62 is virtually eliminated.
To illustrate, light travels through the wave-guide 56 in the direction of arrow 64. As it enters the bend 62, it strikes the barrier 66 between the waveguide 56 and trench 58 at increasing angles as described previously. In prior devices having a uniform substrate, the light would propagate into the substrate and be lost. However, in the present in-vention as shown in Figures 8a and 8b, the light cannot propagate into the substrate 53 because of the periodic dielectric structure 52. Instead, the light is confined within the waveguide 56 and continues through the bend 62.
In the embodiment of Figures 8a and 8b, the waveguide 56 is formed by creating the trenches 58 - 30 and 60 in the epilayer 51. Other methods are also possible, including those previously described in connection with Figures la and lb. A high-re-fractive-index channel may be formed by diffusing material into a uniform substrate or etching material WO 94/1~45 2 153 48~: PCT~S94/~5 onto the substrate. After the channel is formed, the periodic dielectric structure is formed in the sub-strate by the procedure previously described.
Figure 9 illustrates a waveguide section 76 in accordance with another embodiment of the present invention. In this embodiment, the substrate 70 includes a high-refractive-index epilayer 71 and a lower-refractive-index base substrate 73. The sub-strate 70 also comprises a periodic dielectric struc-ture 72 having three-dimensional spatial periodicity.
Radiation is prevented from propagating in all three spatial dimensions of the substrate 70.
The three-dimensional periodic dielectric struc-ture 72 is fabricated in a similar manner to the two-dimensional structure. The epilayer 71 is coveredwith a mask having a two-dimensional array of geo-metric figures defining the desired pattern for the top surface of the three-dimensional periodic di-electric structure. In one embodiment, the two-di-20 mensional array has a triangular lattice pattern.The substrate and mask are exposed to the reactive-ion etchant. The etchant plasma is directed suc-cessively at three different angles with respect to the axis perpendicular to the top surface of the 25 substrate. The angles are each oriented down 35.26 from the perpendicular and are separated by 120 from each other in azimuth. The resulting channels form a three-dimensional face-centered cubic lattice. The electromagnetic dispersion relation in this lattice 30 will exhibit a photonic or frequency band gap.
With three-dimensional periodicity, the periodic dielectric structure 72 prevents propagation of light within the band gap in all three dimensions. Light cannot propagate laterally through the substrate 72 ~94/1~45 ~3~85 PCT~S941~285 as in the two-dimensional case. But also, it cannot propagate toward the bottom surface 75 of the sub-strate 70. Optical losses are further reduced.
Figures 10-12 illustrate various optical cir-cuits to which the present invention is applicable.Each figure is a top view of a portion of a substrate on which is formed a device in accordance with the invention. The periodic dielectric structure used in each device may have either two-dimensional or three-dimensional periodicity.
Figure 10 is a view of an S-bend device 93 in a waveguide section. The S-bend 93 is used in such devices as optical couplers. It includes two bend sections 90 and 91. In prior devices with uniform substrates, these bends would be sources of radiation loss. However, because the bends are surrounded by a periodic dielectric structure 92 in the substrate 87, the bend losses ae virtually eliminated.
Figure 11 is a view of a Y-coupler device 103.
An incoming signal enters the device 103 through straight section 94. The signal iB split at junction 96 into two equal outgoing signals traveling through sections 98 and 99. Radiation losses associated with the junction 96 and bends 100 and 101 are virtually eliminated by the periodic dielectric structure 102 in the substrate 97. It should be noted that where radiation propagates from right to left in Figure 11, the device 103 serves a combiner.
Figure 12 shows a waveguide taper or funnel 110 on a substrate 102 with a periodic dielectric str,uc-ture 104. Many applications require a fiber optic cable 112 to be permanently attached to a waveguide 114 on an optical integrated circuit. This con-nection can lead to insertion loss on the order of ~c\/. ~ r~ CH~ ] ~ : J ~ ; (;17~ +1 ') ~ 'J~
. . 21S3~85 lOdB. To reduce the lo~s, the cable end 116 of t~e integr~t~d wave~u~de 114 i~ ma~e th~ same width a6 t~e cable 112. The opti~u~ width of ~he circuit end 118 ~f the waveguide 114 i8 less ~h~n the ~idth of the cable end 116.
The width transition between the two ends is made o~ a taper aection 120. This ~aper section 120 is a ~ource of loss which ¢an be overcome by the periodic dielectric 6tructure 104.
The present inventi~n is no~ only applicable to op~ical Sy~te~s. The peri~dic dielectric ~tructure can be fabricated to have a frequ~ncy band g~p anyw~ere in ~he microwave t~ ultraviolet ba~ds (lQ6 to 10l5 ~
El~ctro~agnetic radiation at these frequencies can be preven~d from propagatinq through a su~str~te. Th~r-fore, the pre~ent in~ention is applicnble to ~ubst~nti~lly 20 confine radiation in waveguides, sources, detectors, l~er6, power splitter~, p~er combiner8, tapers, interferometers, and any other device in which radia~ion needs to be conflned, Losses can be substantially elimina~.d f~r electromagn~tic radiation anywhe.r~ within the above freauen~y ~an~e.
- We Cl~im:
.
AMENDED S~
INTEGRATED CIRCUITS
Backqround of the Invention Optical integrated circuits and optoelectronic integrated circuits are usually fabricated on the top surface of a uniform substrate. These circuits can experience optical losses as light propagates away from the circuits and into the uniform substrate. It is desirable to produce optical and optoelectronic integrated circuits as compact as possible on a sub-strate to produce small lightweight circuits. How-ever, losses experienced by the interconnects between circuits tend to inhibit the reduction of the overall system size.
Interconnects in optical integrated circuits and optoelectronic integrated circuits are achieved by using waveguides to transport light from one optical device to another. Waveguides are also the basis of numerous optical devices including optical couplers, switches, modulators, power dividers and combiners.
Light propagating through an optical waveguide is contained within the waveguide by total internal reflection. The medium outside the waveguide has a lower index of refraction than does the interior of the waveguide. The boundary between the interior and exterior of the waveguide is characterized by a crit-ical angle determined by the ratio of the refractive indices or index contrast of the two media. The cri-tical angle of the boundary can be defined as the angle below which light inside the waveguide must strike the boundary in order to be reflected back into the waveguide rather than be transmitted through W094/1~45 ~ ~5 3 4 8 PCT~S94/00285 the boundary and out of the waveguide. Light inside the waveguide which strikes the boundary at an angle smaller than the critical angle cannot pass through the boundary and is reflected back into the wave-guide.
Since nearly all of the light traveling through a straight optical waveguide strikes the waveguide boundary at very small angles, very little loss is suffered. However, in fabricating optical and opto-electronic integrated circuits, it is necessary tomake optical waveguides with bends. Also, certain devices such as optical couplers require bends in their waveguides. Unlike straight waveguide sec-tions, waveguide bends can produce significant loss-es. As the light traveling through the waveguideenters a bend, it strikes the boundary at a larger angle than it does in a straight section. If the index contrast does not provide a large enough criti-cal angle, some of the light escapes from the wave-guide, thus introducing bend loss.
Bend losses have proven to be a substantial im-pediment to the development of optical and opto-electronic integrated circuits. To minimize losses, bends must be made with large radii of curvature, typically on the order of 10mm. Such large bend radii are not practical for compact optical and opto-electronic integrated circuits.
Numerous approaches have been suggested to mini-mize bend losses. One of these is the use of abrupt bends rather than curved bends. Abrupt bends have sharp corners joining two straight sections of wave-- guide. The drawback to abrupt bends is that the bend angle must be very small, on the order of 1 degree.
_~94/1~4~ 21 S3~8 PCT~S94/~5 So, this approach contributes little to making cir-cuits more compact.
Another approach has been to grade the index of refraction of the substrate in the area of the bend to maintain internal reflection around the bend.
Combinations of these two approaches have also been suggested. However, no present approach appears to be able to substantially reduce the radii of curva-ture of waveguide bends to facilitate the development of compact optical and optoelectronic integrated circuits.
SummarY of the Invention The present invention is an optical circuit and a method which substantially eliminates radiation losses in optical integrated circuits. The circuit is formed on a surface of a substrate made of a semi-conductor or other type material including dielectric and optical materials. The substrate comprises a region which is characterized by a frequency band gap. The frequency band gap is a band of frequencies at which electromagnetic radiation and, in particu-lar, light waves cannot propagate through the region.
The circuit is formed in the region having the fre-quency band gap such that radiation which would otherwise escape from the circuit into the substrate cannot propagate into the substrate.
The circuit of the present invention experiences reduced radiation losses at frequencies within the band gap of the substrate. In particular, losses at waveguide bends are substantially eliminated. Some of the light traveling through a waveguide bend strikes the boundary between the interior and the exterior of the waveguide at angles greater than the WO94/1~45 PCT~S94/~5 2~s3485 critical angle and would otherwise tend to escape from the waveguide into the substrate. However, in the present invention, the bend is formed in the region of the substrate with the frequency band gap.
Light at a frequency within the band gap cannot pro-pagate into the substrate. The light is confined within the optical circuit and the waveguide.
The region of the substrate with the frequency band gap has a periodic dielectric structure. A
periodic dielectric structure is a structure which exhibits a periodic spatial variation in dielectric constant. As applicable to the present invention, the variation in dielectric constant may be periodic in either two-dimensional or three-dimensional space within the structure.
There are various methods of forming such struc-tures. One of these methods involves forming a peri-odic pattern of holes in a uniform substrate ma-terial. Another is removing substrate material such that what remains is a periodic pattern of cylindri-cal or other similarly shaped rods of substrate mate-rial.
There are also various methods of forming an optical waveguide on the substrate. In one embodi-ment, an epilayer of material of high refractiveindex is formed on top of a substrate having a lower index. Next, the periodic dielectric structure is formed on opposite sites of a channel in the epilayer of uniform material. The channel is shaped as de-sired to serve as the waveguide. The periodic di-electric structure on either side of the channel prevents radiation into the substrate. Thus light is guided through the channel by the periodic dielectric structure. Light is confined vertically within the ~94/1~45 PCT~S94100285 2l~3~8s channel by internal reflection due to the index con-trast between the waveguide in the epilayer and the air on top and between the waveguide and the sub-strate on the bottom. In other embodiments, a mate-rial having a higher index of refraction than the substrate may be diffused into the substrate or etched on the substrate. Alternatively, a material of higher refractive index may be deposited by sput-tering, evaporation or other process onto the surface of the substrate. Another method involves forming a pair of trenches in a high-refractive-index layer deposited on the top surface of the substrate. The material between the trenches serves as the optical waveguide. The air in the trenches is the low-refractive-index exterior medium which provides la-teral internal reflection due to index contrast.
Periodic dielectric structure is provided on the out-side of the trenches to eliminate loss where the re-quirements for internal reflection are not met. Ver-tical losses are eliminated by internal reflectiondue to the refractive index contrast.
The present invention provides substantial ad-vantages over previous methods of reducing loss in optical circuits and in optical waveguide bends.
Unlike previous approaches, it is the substrate it-self which prevents radiation from escaping into the substrate. The present invention does not rely upon physical constraints of a waveguide such as the bend angle, as in the abrupt bend approach. In the pre-sent invention, the waveguide bend radius can bearbitrarily small because it is the substrate which - is preventing loss. Also, the index grading approach relied on the index contrast between the waveguide and the substrate to maintain internal reflection.
W094/1~45 4~ PCT~S94/~5 Even with index grading, a critical angle is present - which constrains the radius of curvature. Because the present invention does not rely solely on index contrast and internal reflection at bends, the radius of curvature at the bend is not so constrained.
Because waveguide bend radii are reduced, opti-cal and optoelectronic circuits can be made much more compact and light weight. These circuits can be to-tally integrated. Different optical devices and in-terconnects can be fabricated on a common substrate.High-speed electronics can be fabricated on the same chip as associated optoelectronic devices.
Brief Descri~tion of the Drawinqs The foregoing and other objects, features and advantages of the invention will be apparent from the following more particular description of preferred embodiments of the invention, as illustrated in the accompanying drawings in which like reference charac-ters refer to the same parts throughout the different views. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating the principles of the invention.
Figure la is a schematic perspective view of a prior art optical circuit.
Figure lb is a schematic perspective view of another prior art optical circuit.
Figure 2a is a schematic perspective view of a prior art uniform substrate with a rib waveguide sec-tion having a bend.
Figure 2b is a schematic top view of the wave-guide section of Figure 2a.
~94/1~45 1 ~ 3 ~ 8 S PCT~S94/~5 Figure 3 is a graph of the loss associated with a 90 circular waveguide bend versus the radius of curvature of the bend for two propagation modes.
Figure 4 is a schematic perspective view of a periodic dielectric structure having two-dimensional periodicity.
Figure 5a is a schematic top view of the per-iodic dielectric structure of Figure 4 showing a triangular lattice pattern.
Figure 5b is a schematic top view of a periodic dielectric structure showing a square lattice pat-tern.
Figure 5c is a schematic top view of a periodic dielectric structure showing a hexagonal lattice pat-tern.
Figure 6 is a graph of the wave attenuation inthe band gap versus frequency of the wave.
Figure 7a is a schematic perspective view of an optical circuit in accordance with the present inven-tion.
Figure 7b is a schematic top view of the opticalcircuit of Figure 7a.
Figure 8a is a schematic perspective view of a waveguide section on a substrate having a two-dimen-sional periodic dielectric structure in accordancewith the present invention.
Figure 8b is a schematic top view of the device of Figure 8a.
Figure 9 is a schematic perspective view of a waveguide on a substrate having a three-dimensional periodic dielectric structure in accordance with the present invention.
Figure 10 is a schematic top view of an S-bend in accordance with the present invention.
W094/1~45 PCT~S94/0028~
21~3~85 .
Figure 11 is a schematic top view of a Y-coupler in accordance with the present invention.
Figure 12 is a schematic top view of a waveguide taper in accordance with the present invent:ion.
Detailed Description of the Invention Optical integrated circuits and optoelectronic integrated circuits can be classified as either ac-tive or passive circuits. Optical integrated cir-cuits perform a variety of passive functions, includ-ing switching and modulating, without generating ordetecting light. Optoelectronic circuits generate and detect light as well as perform certain passive functions. The present invention is applicable to both types of circuits.
It should be noted that throughout this appli-cation, the terms "optical integrated circuits", "op-toelectronic circuits", "optical circuits", and other related terms will be used to describe the various types of circuits to which the invention is appli-cable. Unless otherwise specifically stated, the use of one of these terms in this application does not limit the applicability of the description to that type of circuit. One term is selected over another for illustration purposes only. The present inven-tion is applicable to all of these circuits.
Optical circuits can be fabricated on a top sur-face of a substrate. The optical waveguides which connect the circuits can also be fabricated on the surface of the substrate. These optical waveguides consist of a channel having an index of refraction which is higher than the index of refraction of the surrounding substrate. Because of the index con-~94/1~45 PCT~S94100~5 21 S3~85 trast, light is guided along the channel by totalinternal reflection.
Optical waveguides are used to guide optical signals among the elements in optical and opto-electronic integrated circuits and are analogous tothe metallic lines used to guide electrical signals among electronic integrated circuits. They connect external optical devices such as fiber optic cables with internal optical devices such as switches, modu-lators, sources, and detectors. In addition, theyform the basic structural elements in numerous opti-cal devices including optical couplers, switches, modulators, power dividers, and combiners.
Integrated optical circuits and waveguides can be implemented by several different techniques. One prior art example is shown in Figure la. A substrate 10 is made of a material such as LiNbO3 having a low index of refraction. Optical circuits 11 and 13 are formed in the substrate 10 by techniques such as pho-tolithography, diffusion, ion i~plantation, etching and the like. The optical waveguide 12 is made of a material having a high index of refraction which may be formed by diffusing titanium into the substrate 10 .
Another type of integrated optical circuit and waveguide, commonly referred to as a rib waveguide, is shown in Figure lb. The rib waveguide 22 connects circuits 21 and 23. In this device, the optical channel 22 of high refractive index is formed on the top surface of a low-refractive-index semiconductor substrate 20. The substrate material may be GaxAl~l x~As or other similar material. The channel 22 may be formed of GaAs or other high-refractive-index ma-WO94/1~45 PCT~S94/~5 2ls3485 terial. The channel 22 is formed by depositing GaAs onto the surface of the substrate 20.
Figures la and lb illustrate straight waveguide sections 12 and 22. Light propagating through the waveguides strikes the barrier between the interior and exterior of the waveguides at small angles. Con-sequently, the light is confined within the wave-guides by total internal reflection. However, to be useful in optical integrated circuits applications, waveguides, at times, must include bends.
Figure 2a schematically depicts a section of a prior art rib waveguide 32 which includes a 90 cir-cular bend 34. The waveguide 32 is fabricated on the top surface 31 of a substrate 30 as described above in connection with Figure lb. Figure 2b is a sche-matic top view of the waveguide section 32.
For purposes of illustration, light is assumed to propagate through the waveguide 32 in the dir-ection indicated by arrows 35. It will be understood that the actual direction of propagation is im-material to the invention. The light travels through straight section 36 of the waveguide 32 and then enters bend 34. The light which remains within the waveguide after passing through the bend travels through straight section 38.
As light leaves the straight section 36 and en-ters the bend 34, it strikes the barrier 40 between the interior and the exterior of the waveguide at larger angles. Some of these angles exceed the crit-ical angle required for reflection determined by theindex contrast at the barrier 40. The light which exceeds the critical angle passes through the barrier 40, exits the waveguide 32, and propagates into the air around the waveguide and the substrate 30. This _~94/1~45 21S3~ PCT~S94/00285 lost light, represented by arrows 42 in Figure 2b, is the optical loss associated with the bend, or simply the bend loss.
As shown in Figure 2b, the bend 34 has a radius of curvature R. As R decreases, the angle at which light strikes the barrier 40 increases. More light escapes from the waveguide 32 causing increased bend loss. Experiments have shown that bend losses in-crease exponentially with decreasing bend radius of curvature. That is, L-~e~R/b, where L is the loss, R
is the radius of curvature, and a and b are con-stants.
Depending upon the application in which the waveguide is used, there is a certain maximum bend loss which can be tolerated. This maximum tolerable bend loss corresponds to a minimum allowable bend radius. Thus, bend loss imposes a restraint on the ability to reduce the size of the waveguide bend, and, consequently, on the ability to fabricate com-pact optical integrated circuits.
Figure 3 is a graph of experimental data whichdepicts a relationship between the radius of curva-ture of a 90 circular waveguide bend and the loss associated with that bend. Bend loss in decibels (dB) is plotted as a function of radius of curvature in millimeters (mm) for two modes of propagation.
Curve 44 is a quasi-transverse-electric mode, and curve 46 is a quasi-transverse-magnetic mode. The graph illustrates the exponential relationship be-tween bend radius of curvature and bend loss.
To eliminate the loss associated with opticaland optoelectronic integrated circuits as well as with waveguide bends, the present invention prevents light from propagating into the circuit substrate.
W094/1~45 PCT~S94/OOt85 2153~85 Because the light cannot propagate into the sub-strate, it is confined within circuit and the wave- -guide.
In the preferred embodiment of the present in-vention, the substrate comprises a region which has aperiodic dielectric structure. A periodic dielectric structure is a structure which exhibits a periodic spatial variation in dielectric constant. In one embodiment, the dielectric constant is periodic in two-dimensional space within the structure. In an-other embodiment, the structure exhibits three-di-mensional spatial periodicity.
The periodic dielectric structure is character-ized by a frequency or photonic band gap, or simply a band gap. The band gap of a periodic dielectric structure is a band of frequencies of electromagnetic radiation which cannot propagate through the struc-ture in the plane in which the structure exhibits periodic variation in dielectric constant.
Figure 4 is a schematic perspective view of a periodic dielectric structure 300 illustrating two-dimensional spatial periodicity. Specifically, the structure 300 is periodic in the x and z dimensions.
Therefore, electromagnetic radiation having a fre-quency within the band gap of the structure cannot propagate in a plane parallel with the x-z plane, including the plane of the top surface 326 of the structure.
The structure 300 includes a plurality of elon-gated elements 322 extending orthogonal to the sub-strate top surface 326 and bottom surface 328. The elements 322 are preferably cylindrically shaped and extend in a two-dimensional periodic arrangement relative to the x-z plane or any plane parallel ~94/1~45 21 ~3~ 85 PCT~S94/00~5 thereto. Although cylindrical elements are described - hereinafter, quasi-cylindrical elements or other shaped elongated elements may be employed. They may be formed of a non-conductive low-dielectric material disposed within a non-conductive high-dielectric sub-strate material 324. The elements 322 may simply be bores, voids, or channels which may be filled with low-dielectric fluids or solids such as air and/or other liquid or solid material.
In an alternative embodiment, the elements may be formed of non-conductive high-dielectric material and may be disposed in the periodic arrangement in a non-conductive low dielectric material. An example of this configuration is a high-dielectric substrate with material etched away to leave only the periodic arrangement of cylindrical rods of the high-di-electric material with air in the spaces between the rods. The space may also be filled with some other low-dielectric fluid or solid.
A longit~ axis 325 extends through the cen-ter of each element 322 in the vertical or y-direc-tion. The elements 322 are arranged periodically in two dimensions in the x-z plane which is generally orthogonal to the longitudinal axes 325 extending 25 through the elements 322.
The structure 300 can be positioned to filter incoming electromagnetic energy 329 polarized in any direction that is propagating in the x-z plane. The structure 300 reflects substantially all of the inci-dent electromagnetic energy 329 having a frequencywithin the range of the photonic or frequency band gap. More specifically, electromagnetic energy with-in the frequency range of the band gap is sub-stantially prevented from propagating through the WO94/1~45 - ~ PCT~S94/00285 2lS3485 structure 300. Thus, the structure 300 operates as a band stop filter. The structure maintains a sub-stantially constant band gap frequency range for radiation propagating along any incident angle in the x-z plane.
Figure 5a is a top view of the structure 300 of Figure 4. In this embodiment, the cylindrical ele-ments 322 are periodically arranged to provide a tri-angular lattice. The lines 327 illustrate the trian-gular lattice arrangement of the cylindrical elementsalong the top surface 326 of the substrate material 324. Other possible lattice structures are shown in Figures 5b and 5c. Figure 5b shows a square lattice structure, and Figure 5c shows a honeycomb or hex-agonal lattice structure.
A feature of the periodic dielectric structureis that the center frequency of the band gap, the bandwidth of the band gap (i.e., the stop band) and the band gap attenuation can be tailored for any frequency range in the microwave to ultraviolet bands (106 to 10l5 Hz) during the fabrication of the struc-ture. For the structure of Figures 4 and 5, the center frequency (f), the bandwidth (~f) and the band gap attenuation (A~) of the band gap are shown in Figure 6. The attenuation (AG) of the band gap is proportional to the number of rows of elements 322.
Thus, the attenuation (AG) can be increased by pro-viding additional rows. The center frequency (f) of the bandwidth (~f) can be computed in accordance with the following equation:
f = [13.8(13/~ ]/a GHz where 094/1~45 21 ~34~ PCT~Sg4/~5 ~ = dielectric constant of the substrate material, ~ = magnetic permeability of the substrate material, and a = triangular lattice constant which corres-ponds to the distance in centimeters between centers of adjacent elements.
The location of the band gap on the frequency scale is determined by the center frequency. The bandwidth (~f) is determined by the radius (r) of the cylindrical elements 322 and the triangular lattice constant (a).
A two-dimensional periodic dielectric structure as shown in Figures 4 and 5a-c may be fabricated on a portion of a homogeneous or uniform substrate by one of several methods. One method involves drilling holes in a high- dielectric uniform substrate. The holes are filled with a low-dielectric material such as air.
Another method involves the use of reactive-ion etching. The substrate is covered on one face with a mask which contains a two-dimensional array of geo-metric figures of the size, spacing, and periodicity required for the desired band gap. This two-dimen-sional array of geometric figures may be patterned by employing electron beam lithography or conventional photolithography. The geometric figures are either transparent or opaque to a reactive-ion etchant used - 30 to selectively eradicate the high dielectric sub-strate material. For example, if cylindrical air channels are to be formed in the substrate, the geo-metric figures are circles which are transparent to the etchant, and the remainder of the mask is opaque W094/1~45 ~ PCT~S94/~5 to the etchant. If square rods of high dielectric material are to be formed, the figures are squares which are opaque to the etchant, and the remainder of the mask is transparent to the etchant.
The substrate and mask are then exposed to the highly directional reactive-ion etchant. The re-- active-ion plasma is directed at the mask along the perpendicular axis, and vertical channels of the desired shape are created in the substrate. The resulting array of elements forms the two-dimensional frequency or photonic band gap.
Figure 7a is a schematic perspective view of cn integrated optical circuit 200 in accordance with the present invention. Figure 7b is a top view of the circuit 200. The circuit 200 comprises a base sub-strate 202 formed of a material having a low re-fractive index such as GaxAll~As. An epilayer 204 made of a material having a higher refractive index than the base substrate 202 such as GaAs is formed on the top surface of the base substrate 202. The com-bination of the base substrate 202 and the epilayer 204 forms the substrate 206 for the optical circuit 200.
The components of the optical circuit 200 in-clude two optical devices 208 and 210. These devicesmay be a laser and a detector or other similar de-vices. It will be understood that the invention is applicable to other such devices. Also, two devices are selected for ease of description only. Typical circuits will have more devices.
The devices 208 and 210 are connected by a wave-guide 212. The waveguide 212 includes a straight section 214, a bend 216 and a second straight section 218. For illustration purposes, light is assumed to )94/1~45 PCT~S94/~5 2 1 ~ 3 ~ 8 5 !
leave device 208 and propagate through the waveguide 212 toward device 210. The light passes through straight section 214, bend 216 and straight section - 218 and enters device 210.
The optical devices 208 and 210 are surrounded by periodic dielectric structure 222. The periodic dielectric structure 222 prevents emissions from the devices 208 and 210 at a frequency within the band gap of the structure 222 from propagating into the substrate 206. Thus, the devices 208 and 210 are isolated from each other, the waveguide 212, and any other devices on the substrate 206.
The periodic dielectric structure 222 also serves to define the lateral extents of the waveguide 212 on the epilayer 204. The periodic dielectric structure 222 prevents light at a frequency within the band gap of the structure 222 from propagating in the plane of the epilayer 204. Thus, the light is confined laterally within the waveguide 212. Light 20 is prevented from propagating out of the waveguide 212 in the vertical directions by internal re-flection. Light will not propagate up out of the waveguide into space because of the refractive index contrast between the interior of the waveguide and 25 the air above it. Light will not propagate down into the base substrate 202 because of the index contrast between the epilayer 204 and the base substrate 202.
Because the light cannot propagate outside the wave-guide 212, it is confined inside. The light entering the waveguide 212 from the device 208 travels through the straight section 214 into bend 216. It is guided around the bend 216 by the periodic dielectric struc-ture 222 and through straight section 218 into device 210.
WO94/1~45 - - PCT~S94/00285 2~534~5 The circuit 200 of Figures 7a and 7b is made by first forming the uniform high-refractive-index epi-layer 204 on top of a uniform low-refractive index base substrate 202 to form substrate 206. This is done by diffusion or similar fabrication technique.
Next, the devices 208 and 210 are formed on the epi-layer 204. Finally, the periodic dielectric struc-ture 222 is formed in the substrate 206 by one of the methods previously described.
The periodic dielectric structure 222 is de-signed to create a frequency band gap for the sub-strate 206 which includes the frequency of the radia-tion which will be carried by the waveguide 212. To create the structure 222, the periodic pattern of holes is formed in the substrate 206. The pattern of holes is made to surround devices 208 and 210 and to define the waveguide 212 connecting the devices. The holes are made by either drilling or by the reaction ion etching process previously described.
Figures 8a and 8b depict a section of waveguide 56 in accordance with another embodiment of the in-vention. A high-refractive-index epilayer 51 made of a material such as GaAs is formed on the top surface of a low-refractive-index base substrate 50 made of a -25 material such as GaxAllxAs to form a substrate 53. The substrate 53 may also be made of other materials such as di-electric or optical materials. The periodic di-electric structure 52 is periodic in two dimensions in the plane of the epilayer 51. The section of optical waveguide 56 is formed in the epilayer 51 between substantially parallel trenches 58 and 60.
The waveguide section 56 includes a 90 circular bend 62. The 90 bend angle is chosen for illustration _ 0 94/16345 1S31~5 ~/US94100285 purposes only. The bend angle need not be 90. The trenches 58 and 60 are formed by etching or other known processes. The air in the trenches provides refractive index contrast for internal reflection of the light carried by the waveguide 56. Periodic dielectric structure 52 is provided outside the tren-ches 58 and 60 to eliminate loss where the require-ments for total internal reflection are not met.
The periodic dielectric structure 52 is formed as described in connection with Figures 4-6 to have a frequency band gap at the known frequency of the light propagating in the waveguide 56. Therefore, the light cannot propagate into the substrate 53 in the plane of the epilayer 51. As a result, loss of light at the bend 62 is virtually eliminated.
To illustrate, light travels through the wave-guide 56 in the direction of arrow 64. As it enters the bend 62, it strikes the barrier 66 between the waveguide 56 and trench 58 at increasing angles as described previously. In prior devices having a uniform substrate, the light would propagate into the substrate and be lost. However, in the present in-vention as shown in Figures 8a and 8b, the light cannot propagate into the substrate 53 because of the periodic dielectric structure 52. Instead, the light is confined within the waveguide 56 and continues through the bend 62.
In the embodiment of Figures 8a and 8b, the waveguide 56 is formed by creating the trenches 58 - 30 and 60 in the epilayer 51. Other methods are also possible, including those previously described in connection with Figures la and lb. A high-re-fractive-index channel may be formed by diffusing material into a uniform substrate or etching material WO 94/1~45 2 153 48~: PCT~S94/~5 onto the substrate. After the channel is formed, the periodic dielectric structure is formed in the sub-strate by the procedure previously described.
Figure 9 illustrates a waveguide section 76 in accordance with another embodiment of the present invention. In this embodiment, the substrate 70 includes a high-refractive-index epilayer 71 and a lower-refractive-index base substrate 73. The sub-strate 70 also comprises a periodic dielectric struc-ture 72 having three-dimensional spatial periodicity.
Radiation is prevented from propagating in all three spatial dimensions of the substrate 70.
The three-dimensional periodic dielectric struc-ture 72 is fabricated in a similar manner to the two-dimensional structure. The epilayer 71 is coveredwith a mask having a two-dimensional array of geo-metric figures defining the desired pattern for the top surface of the three-dimensional periodic di-electric structure. In one embodiment, the two-di-20 mensional array has a triangular lattice pattern.The substrate and mask are exposed to the reactive-ion etchant. The etchant plasma is directed suc-cessively at three different angles with respect to the axis perpendicular to the top surface of the 25 substrate. The angles are each oriented down 35.26 from the perpendicular and are separated by 120 from each other in azimuth. The resulting channels form a three-dimensional face-centered cubic lattice. The electromagnetic dispersion relation in this lattice 30 will exhibit a photonic or frequency band gap.
With three-dimensional periodicity, the periodic dielectric structure 72 prevents propagation of light within the band gap in all three dimensions. Light cannot propagate laterally through the substrate 72 ~94/1~45 ~3~85 PCT~S941~285 as in the two-dimensional case. But also, it cannot propagate toward the bottom surface 75 of the sub-strate 70. Optical losses are further reduced.
Figures 10-12 illustrate various optical cir-cuits to which the present invention is applicable.Each figure is a top view of a portion of a substrate on which is formed a device in accordance with the invention. The periodic dielectric structure used in each device may have either two-dimensional or three-dimensional periodicity.
Figure 10 is a view of an S-bend device 93 in a waveguide section. The S-bend 93 is used in such devices as optical couplers. It includes two bend sections 90 and 91. In prior devices with uniform substrates, these bends would be sources of radiation loss. However, because the bends are surrounded by a periodic dielectric structure 92 in the substrate 87, the bend losses ae virtually eliminated.
Figure 11 is a view of a Y-coupler device 103.
An incoming signal enters the device 103 through straight section 94. The signal iB split at junction 96 into two equal outgoing signals traveling through sections 98 and 99. Radiation losses associated with the junction 96 and bends 100 and 101 are virtually eliminated by the periodic dielectric structure 102 in the substrate 97. It should be noted that where radiation propagates from right to left in Figure 11, the device 103 serves a combiner.
Figure 12 shows a waveguide taper or funnel 110 on a substrate 102 with a periodic dielectric str,uc-ture 104. Many applications require a fiber optic cable 112 to be permanently attached to a waveguide 114 on an optical integrated circuit. This con-nection can lead to insertion loss on the order of ~c\/. ~ r~ CH~ ] ~ : J ~ ; (;17~ +1 ') ~ 'J~
. . 21S3~85 lOdB. To reduce the lo~s, the cable end 116 of t~e integr~t~d wave~u~de 114 i~ ma~e th~ same width a6 t~e cable 112. The opti~u~ width of ~he circuit end 118 ~f the waveguide 114 i8 less ~h~n the ~idth of the cable end 116.
The width transition between the two ends is made o~ a taper aection 120. This ~aper section 120 is a ~ource of loss which ¢an be overcome by the periodic dielectric 6tructure 104.
The present inventi~n is no~ only applicable to op~ical Sy~te~s. The peri~dic dielectric ~tructure can be fabricated to have a frequ~ncy band g~p anyw~ere in ~he microwave t~ ultraviolet ba~ds (lQ6 to 10l5 ~
El~ctro~agnetic radiation at these frequencies can be preven~d from propagatinq through a su~str~te. Th~r-fore, the pre~ent in~ention is applicnble to ~ubst~nti~lly 20 confine radiation in waveguides, sources, detectors, l~er6, power splitter~, p~er combiner8, tapers, interferometers, and any other device in which radia~ion needs to be conflned, Losses can be substantially elimina~.d f~r electromagn~tic radiation anywhe.r~ within the above freauen~y ~an~e.
- We Cl~im:
.
AMENDED S~
Claims (42)
1. A method of reducing radiation losses in optical integrated circuits, comprising:
providing a substrate (202); and forming an optical integrated circuit (208, 210, 212) on or in the substrate; characterized in that the method further comprising the step of forming a region of said substrate with a periodic dielectric lattice structure (222) having a spatially periodic variation in dielectric constant in at least two dimensions, the lattice dimensions being proportioned to produce a frequency band gap defining a band of frequencies of electromagnetic radiation at which the optical integrated circuit is operable such that, in a plane of the periodic variation, radiation at such frequencies is substantially prevented from propagating in at least one dimension within the region.
providing a substrate (202); and forming an optical integrated circuit (208, 210, 212) on or in the substrate; characterized in that the method further comprising the step of forming a region of said substrate with a periodic dielectric lattice structure (222) having a spatially periodic variation in dielectric constant in at least two dimensions, the lattice dimensions being proportioned to produce a frequency band gap defining a band of frequencies of electromagnetic radiation at which the optical integrated circuit is operable such that, in a plane of the periodic variation, radiation at such frequencies is substantially prevented from propagating in at least one dimension within the region.
2. The method of Claim 1 wherein the region is formed as part of the optical integrated circuit.
3. The method of Claim 1 wherein the region is formed adjacent to the optical integrated circuit.
4. The method of claim 1 wherein the step of forming the optical integrated circuit comprises forming a laser.
5. The method of Claim 1 wherein the step of forming the optical integrated circuit comprises forming a detector.
6. The method of Claim 1 wherein the step of forming the optical integrated circuit comprises forming a filter.
7. The method of Claim 1 wherein the step of forming the optical integrated circuit comprises forming a modulator.
8. The method of Claim 1 wherein the step of forming the optical integrated circuit comprises forming a power divider.
9. The method of Claim 1 wherein the step of forming the optical integrated circuit comprises forming a power combiner.
10. The method of Claim 1 wherein the step of forming the optical integrated circuit comprises forming a switch.
11. The method of Claim 1 wherein the periodic dielectric lattice structure is a two-dimensional periodic dielectric lattice structure (222).
12. The method of Claim 1 wherein the periodic dielectric lattice structure is a three-dimensional periodic dielectric lattice structure (72).
13. The method of Claim 1 wherein the substrate comprises a semiconductor material.
14. The method of Claim 1 wherein the step of forming a region comprises forming a periodic pattern of void regions in the substrate.
15. The method of Claim 1 wherein the step of forming the optical integrated circuit comprises forming an optical waveguide (212) on or in the substrate.
16. The method of Claim 15 wherein the region with the periodic dielectric lattice structure is formed adjacent to a bend (216) in the waveguide such that radiation losses associated with the bend are reduced.
17. The method of Claim 15 wherein the region with the periodic dielectric lattice structure is formed adjacent to a taper (120) in the waveguide such that radiation losses associated with the taper are reduced.
18. The method of Claim 15 wherein the step of forming an optical waveguide comprises preventing the region with the frequency band gap from being formed in a specific portion of the substrate, said specific portion of the substrate being the optical waveguide.
19. The method of Claim 15 wherein the step of forming an optical waveguide comprises diffusing a material into the substrate, said material having an index of refraction higher than the index of refraction of the substrate.
20. The method of Claim 15 wherein the step of forming an optical waveguide comprises depositing a material onto a surface of the substrate, said material having a higher index of refraction than the index of refraction of the substrate.
21. The method of Claim 15 wherein the step of forming an optical waveguide comprises forming two substantially parallel trenches (58,60) in a surface of the substrate, said trenches defining a channel of material (56) between them, said channel of material being the optical waveguide.
22. An optical device with reduced radiation losses, comprising:
a substrate (202); and an optical integrated circuit (208, 210 212) formed on or in the substrate; characterized in that the optical device further comprises a region formed on or in the substrate and having a periodic dielectric lattice structure (222) having a spatially periodic variation in dielectric constant in at least two dimensions, the lattice dimensions being proportioned to produce a frequency band gap defining a band of frequencies of electromagnetic radiation at which the optical integrated circuit is operable such that, in a plane of the periodic variation, radiation at such frequencies is substantially prevented from propagating in at least one dimension within the region.
a substrate (202); and an optical integrated circuit (208, 210 212) formed on or in the substrate; characterized in that the optical device further comprises a region formed on or in the substrate and having a periodic dielectric lattice structure (222) having a spatially periodic variation in dielectric constant in at least two dimensions, the lattice dimensions being proportioned to produce a frequency band gap defining a band of frequencies of electromagnetic radiation at which the optical integrated circuit is operable such that, in a plane of the periodic variation, radiation at such frequencies is substantially prevented from propagating in at least one dimension within the region.
23. The optical device of Claim 22 wherein the region is part of the optical integrated circuit.
24. The optical device of Claim 22 wherein the region is adjacent to the optical integrated circuit.
25. The optical device of claim 22 wherein the optical integrated circuit comprises a laser.
26. The optical device of claim 22 wherein the optical integrated circuit comprises a detector.
27. The optical device of claim 22 wherein the optical integrated circuit comprises a filter.
28. The optical device of Claim 22 wherein the optical integrated circuit comprises a modulator.
29. The optical device of Claim 22 wherein the optical integrated circuit comprises a power divider.
30. The optical device of Claim 22 wherein the optical integrated circuit comprises a power combiner.
31. The optical device of Claim 22 wherein the optical integrated circuit comprises a switch.
32. The optical device of Claim 22 wherein the periodic dielectric lattice structure is a two-dimensional periodic dielectric lattice structure (222).
33. The optical device of Claim 22 wherein the periodic dielectric lattice structure is a three-dimensional periodic dielectric lattice structure (72).
34. The optical device of Claim 22 wherein the substrate comprises a semiconductor material.
35. The optical device of Claim 22 wherein the region comprises a periodic pattern of void regions in the substrate.
36. The optical device of Claim 22 wherein the optical integrated circuit comprises an optical waveguide (212).
37. The optical device of Claim 36 wherein the region is formed adjacent to a bend (216) in the optical waveguide such that radiation losses associated with the bend are reduced.
38. The optical device of Claim 36 wherein the region is formed adjacent to a taper (120) in the optical waveguide such that radiation losses associated with the taper are reduced.
39. The optical circuit of Claim 36 wherein the optical waveguide is a channel in the substrate surrounded by the region having the periodic dielectric lattice structure.
40. The optical circuit of Claim 36 wherein the optical waveguide is a channel of material diffused into the substrate, said material having an index of refraction which is higher than the index of refraction of the substrate.
41. The optical circuit of Claim 36 wherein the optical waveguide is a channel of material deposited on a surface of the substrate, said material having an index of refraction which is higher than the index of refraction of the substrate.
42. The optical circuit of Claim 36 wherein the optical waveguide is a channel of material (56) between two substantially parallel trenches (58,60) in a surface of the substrate.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US243093A | 1993-01-08 | 1993-01-08 | |
| US08/002,430 | 1993-01-08 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2153485A1 true CA2153485A1 (en) | 1994-07-21 |
Family
ID=21700730
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002153485A Abandoned CA2153485A1 (en) | 1993-01-08 | 1994-01-07 | Low-loss integrated circuits |
Country Status (6)
| Country | Link |
|---|---|
| US (1) | US5526449A (en) |
| EP (1) | EP0678196B1 (en) |
| JP (1) | JPH08505707A (en) |
| CA (1) | CA2153485A1 (en) |
| DE (1) | DE69430361D1 (en) |
| WO (1) | WO1994016345A1 (en) |
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| DE102010004442B4 (en) * | 2010-01-13 | 2015-08-20 | Leoni Kabel Holding Gmbh | Optical component for optical waveguide, optical connector system with such a device and method for producing such a device |
| CN103917915B (en) * | 2011-11-07 | 2016-09-21 | 西铁城控股株式会社 | Laser light source |
| US9581762B2 (en) | 2012-09-16 | 2017-02-28 | Shalom Wertsberger | Pixel structure using a tapered core waveguide, image sensors and camera using same |
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| CN104360439B (en) * | 2014-11-28 | 2019-01-01 | 南京信息工程大学 | A kind of photonic crystal bending waveguiding structure based on conversion medium |
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| US10908431B2 (en) | 2016-06-06 | 2021-02-02 | Shalom Wertsberger | Nano-scale conical traps based splitter, combiner, and reflector, and applications utilizing same |
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|---|---|---|---|---|
| FR2633401B1 (en) * | 1988-06-24 | 1990-10-05 | Labo Electronique Physique | SEMICONDUCTOR DEVICE COMPRISING AN INTEGRATED LIGHT GUIDE WHICH HAS AT LEAST ONE RECLINED AND ONE CURVED PART |
| US5195071A (en) * | 1989-02-14 | 1993-03-16 | Ricoh Company, Ltd. | Focus detecting optical head |
| US5054872A (en) * | 1990-03-16 | 1991-10-08 | Ibm Corporation | Polymeric optical waveguides and methods of forming the same |
| FI84869C (en) * | 1990-06-11 | 1992-01-27 | Planar Int Oy | MATRISFILMSTRUKTUR I SYNNERHET FOER ELEKTROLUMINECENS DISPLAYENHET. |
| US5172267A (en) * | 1990-12-21 | 1992-12-15 | Bell Communications Research, Inc. | Optical reflector structure, device, method of fabrication, and communications method |
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| IT1245423B (en) * | 1991-02-27 | 1994-09-20 | Alenia Aeritalia & Selenia | DICHROIC STRUCTURE DISCRIMINATING IN FREQUENCY WITH VARIABLE BANDWIDTH, AND ITS APPLICATIONS |
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| US5335240A (en) * | 1992-12-22 | 1994-08-02 | Iowa State University Research Foundation, Inc. | Periodic dielectric structure for production of photonic band gap and devices incorporating the same |
-
1994
- 1994-01-07 DE DE69430361T patent/DE69430361D1/en not_active Expired - Lifetime
- 1994-01-07 JP JP6516248A patent/JPH08505707A/en active Pending
- 1994-01-07 CA CA002153485A patent/CA2153485A1/en not_active Abandoned
- 1994-01-07 EP EP94906565A patent/EP0678196B1/en not_active Expired - Lifetime
- 1994-01-07 WO PCT/US1994/000285 patent/WO1994016345A1/en active IP Right Grant
- 1994-07-14 US US08/280,105 patent/US5526449A/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| EP0678196B1 (en) | 2002-04-10 |
| EP0678196A1 (en) | 1995-10-25 |
| DE69430361D1 (en) | 2002-05-16 |
| US5526449A (en) | 1996-06-11 |
| JPH08505707A (en) | 1996-06-18 |
| WO1994016345A1 (en) | 1994-07-21 |
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| Date | Code | Title | Description |
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| EEER | Examination request | ||
| FZDE | Discontinued |