Broad wavelength range single mode integrated optics device

Abstract: A broadband single mode optical circuit element such as a Mach-Zender modulator for operation over a range of optical wavelengths. An intermediate waveguide network (38) receives a beam of light from an input waveguide (40) and transmits the beam to an output waveguide (42). The intermediate waveguide network (38) includes at least one and typically two intermediate waveguides (48, 50). The index of refraction of the intermediate waveguides is sufficient to support multiple modes of light over the wavelength range of the circuit element. The input and output waveguides are narrow enough that they each can support only the fundamental mode of light over the optical wavelength range. The waveguides are configured such that no energy is coupled from the fundamental mode to higher order modes throughout the wavelength range. The intermediate waveguides can be configured as desired, for example as a strip loaded waveguide (58) or a buried waveguide (66).

Description: BACKGROUND Field of the Invention The present invention relates to elements for use in fiber optic-based systems of the type that are limited to lowest order optical mode transmission. More particularly, this invention pertains to improvements in such elements that result in operation over a broad wavelength range. Description of the Prior Art Numerous optical systems rely exclusively upon the transmission of single or lowest order mode light. For example, long distance fiber optic communication systems utilize single mode fiber to economize by increasing the distances between, and, thus, minimizing the number of, repeaters. Single mode fiber can maintain the character of transmitted signals over greater distances by offering larger bandwidths than multimode fiber. In the past, optical signals of single mode systems have been processed by integrated optical devices, such as the Mach-Zehnder amplitude modulator of Figure 1, that employ an exclusively single-mode design criterion in which all wave guides are capable of supporting only the fundamental mode. This has been believed necessary to avoid problems related to extinction (on/off) ratio, spatial uncertainty and the like. If one were to attempt to design an amplitude modulator of the Mach-Zehnder variety for operation from 1300 nm to 1550 nm, a very important wavelength band, using a conventional device optimized for 1300 nm operation, the weaker waveguide confinement at the longer wavelength would give rise to increased bend losses as well as require a higher drive voltage. Alternatively, using a 1550 nm optimized device at 1300 nm, one would expect to find a very poor extinction ratio as a consequence of multiple modes at the shorter wavelength. Analogous problems are associated with other optical waveguide devices. As a result, one is presently forced to employ circuit elements optimized for very narrow wavelength range of operation, limiting interchangeability between wavelengths of operation. SUMMARY OF THE INVENTION The present invention addresses and overcomes the shortcomings described above by providing, in a first aspect, a broadband single mode optical circuit element for use over a predetermined optical wavelength range as defined in claim 1. Such element includes an optical waveguide network. The network includes an input waveguide, an output waveguide and an intermediate waveguide network. The intermediate waveguide network is in optical communication with both the input and output waveguides, each being arranged to support only the fundamental mode throughout the predetermined range. The intermediate waveguide network includes at least one waveguide capable of supporting a plurality of light modes within the predetermined range and this network is arranged so that substantially no energy is coupled from the fundamental mode to higher order modes throughout the predetermined range. In a second aspect, the invention provides a single mode fiber optic circuit for processing light of predetermined optical wavelength range. Such circuit includes a plurality of segments of single mode optical fiber. At least one optical circuit element is provided, generally in accordance with the preceding paragraph, that is adapted to receive a first optical signal and to produce a second optical signal. Means are provided for coupling an optical signal from a first fiber segment into an input waveguide and for coupling an optical signal from the output waveguide into a second fiber segment. In a preferred embodiment, a Mach-Zehnder amplitude modulator is formed by an arrangement of titanium-doped surface diffusions on an LiNb0₃ substrate. The waveguides comprising the device are doped to an extent that would support multiple modes at the shorter wavelength of a preselected range of wavelengths. The input and output waveguides are of reduced widths to assure that only a single mode is supported at the shorter wavelengths. An intermediate waveguide network is of adiabatic design to prevent the energization of higher order modes therein. The single mode design of the input and output waveguides avoids the possible generation of unwanted modes in the output while the wider guides of the intermediate network minimize bend losses, enhance interaction with electrical fields and reduce crosstalk between adjacent-waveguides. The preceding and other features and advantages of the present invention will become more readily appreciated from the detailed description that follows. This description is accompanied by a set of drawing figures. Numerals of the drawing figures, corresponding to those of the written description, point to the various features of the invention. Like numerals refer to like features throughout both the written description and the drawing figures. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a top plan view of a Mach-Zehnder amplitude modulator in accordance with the prior art; Figure 2 is a top plan view of a Mach-Zehnder amplitude modulator in accordance with the invention with electrodes removed for purposes of clarity; Figures 3(a) and 3(b) are cross-sectional views of surface diffusion waveguides in accordance with the invention, Figure 3(a) representing an intermediate step in the formation of the waveguide illustrated in Figure 3(b); Figure 4 is a cross-sectional view of a strip waveguide in accordance with the invention; and Figure 5 is a cross-sectional view of a buried waveguide formed in accordance with the invention. DETAILED DESCRIPTION Figure 1 is a top plan view of a portion of a fiber optic circuit in accordance with the prior art that includes a Mach-Zehnder amplitude modulator 10. Single mode optical systems and circuits often find advantageous uses due, in part, to the greater bandwidth of single mode, as opposed to multimode, optical fiber. Light is transmitted through an input single mode optical fiber 12 and, after processing by the amplitude modulator 10, the modulated optical signal is delivered to a single mode output fiber 14. The input and output fibers 12 and 14 are optically and mechanically coupled to the modulator 10 by means of an appropriate optical cement. The modulator 10 includes a substrate 20 of appropriate electro-optic material such as LiNbO₂. An electrode structure comprising metalizations 22, 24 and 26 is selectively deposited upon the top surface of the substrate 20 and situated with respect to a waveguide network 28 that includes straight input and output waveguides 30 and 32. The input and output waveguides communicate with parallel arm waveguides 34 and 36 that branch from fork or y-junctions to form a functioning device. In operation, the electrodes 22, 24 and 26 are employed to impose electric fields to the waveguides 34 and 36 that control the relative speeds of propagation of the two light beams therethrough. Accordingly, these beams (resulting from the splitting of the input beam at the input y-junction) will be in-phase or out-of-phase by a controllable amount when combined at the output y-junction that communicates with the output waveguide 32. When out-of-phase, the antisymmetric mode (first higher order mode) is excited and leaks out of the output waveguide. Since the output waveguide 32 is designed to support and transmit only the fundamental mode, the intensity of the output of the modulator 10 will be reduced (from the input signal) to the extent that the antisymmetric mode is present. Figure 2 is a top plan view of a Mach-Zehnder amplitude modulator in accordance with the invention with electrodes removed for purposes of clarity. The waveguide structure is illustrated without reference to its fabrication and the optical paths thereby existing in the device should not be considered to be limited to any particular waveguide technology. For example, the optical paths of the device 38 may comprise surface diffusions, strip-loaded or buried device structures. As before, the waveguide 38 includes straight input and output sections 40 and 42 respectively. An input y-junction 44 and an output y-junction 46 serve to split the incoming light into a pair of parallel waveguide paths 48 and 50 and to recombine the two beams, after the application of appropriate modulation voltages, to form the modulated signal as described above. In the prior art as shown in Figure 1, all waveguide structures of the modulator 10 are designed to be capable of supporting only light of the fundamental mode and are incapable of supporting any higher-order modes. As explained, this conventional approach limits the wavelength range of operation of the device essentially to its center frequency. In the present invention, the inventors have adopted a new criterion to achieve significant broadening of the wavelength range of operation. The broad operation of the device is accomplished by (1) increasing the refractive index of the waveguide over that of a corresponding "conventional" waveguide designed for single mode operation at the longer wavelength (at the wider width) of a predetermined spectrum and (2) decreasing the widths of the input waveguide section 40 and the output section 42 below those of a conventional single mode device designed for operation at the shorter wavelength (at the lower index of refraction). The combination of these two principles is "fine tuned" so that the input waveguide 40 and the output waveguide 42 are capable of supporting only the fundamental mode throughout the predetermined optical wavelength range of interest. Unlike the input and output sections, the waveguides of the intermediate waveguide network comprising the y-junctions 44 and 46 and the parallel arms 48 and 50 are not of reduced widths. Rather, the widths of the waveguides of the intermediate network are adequate for containment of the fundamental mode at the larger wavelength in a waveguide having a "conventional" index of refraction (as opposed to the increased index of the present invention.) It is well known that the design of a structure such as a Mach-Zehnder amplitude modulator for operation over any appreciable wavelength range faces an inherent contradiction. A device optimized for operation at the shorter wavelength requires waveguides that are unable to guide the longer wavelength while one designed for the longer wavelength will excite higher-order modes at the shorter wavelength. As discussed above, in the present invention the input waveguide 40 and the output waveguide 42 are designed to be capable of supporting only single mode light throughout the wavelength range of interest. This is accomplished, as mentioned above, by increasing the refractive index of the waveguide to assure containment of the longer wavelengths and decreasing the widths of these sections to prevent multi-mode operation at the shorter wavelengths. The widths of the waveguides of the intermediate waveguide network 38 are not so limited. The inventors have found that, while the input and the output waveguides must be capable of supporting only the fundamental mode throughout the range of interest, conventional design techniques may be employed to assure that, although the waveguides of the intermediate network could support higher order modes at the shorter wavelengths, this does not, in fact, occur. The intermediate waveguide network of the device is carefully designed, by judicious selection of angles, symmetry, materials and the like so that the incoming optical energy does not in fact excite higher-order modes as it passes therethrough. The design of so-called "adiabatic" networks for maintaining the mode structure and for avoiding the energization of undesired (although potentially supportable) modes is well known and disclosed, for example, in D. Marcuse, Theory of Dielectric Optical Waveguides , Academic Press (1974) at pages 55 through 117. Thus, the optical energy from the input waveguide 40 essentially remains at the fundamental mode as it passes through the intermediate waveguide network 38. This feature of the design is, of course, most significant at the shorter wavelengths. The existence of a positive relationship between waveguide dopant concentration and refractive index is well recognized in the art. See, for example, R. V. Schmidt and I. P. Kaminow, "Metal-Diffused Optical Waveguides in LiNb0₃," Applied Physics Letters, Vol. 25, No. 8 (October 15, 1974). The dependence of the number of modes of light that can be supported or contained by a waveguide upon the refractive index differential, Δn, existing between the substrate and waveguide may be seen by examination of the so-called "V number" that characterizes a waveguide in integrated optics. This may be defined as follows: V = (2π/λ) (hw) ½ (2nΔn) ½ where: n = refractive index of material surrounding waveguide; Δn = refractive index differential between waveguide and surrounding material; λ= wavelength of light propagating in waveguide; h = height of waveguide; and w = width of waveguide. (Note: If the waveguide does not have a constant index of refraction and the height and width are not precisely defined ( e.g. a diffused waveguide), a suitable average Δn, h and w can be defined.) It can be shown that the number of modes N that the guide will support is: N= cV² = (4π²c)(hw/λ²)(2nΔn) where: c = a constant of order unity whose exact value is a function of details of the waveguide. In order to maintain a single mode waveguide, the quantity hwnΔn/λ² must be a constant. Accordingly, an increase in the wavelength λ must be compensated for the waveguide to remain single mode. It can be seen that either an increase in waveguide dimensions (h, w or both) or index difference (Δn) can counteract the effect of an increase in wavelength upon V, maintaining both that value and the number of modes (1 in the case of a single mode guide). Conversely, it will be appreciated that an increase in Δn due to increased waveguide dopant concentration can be offset in the same sense by an increase in the wavelength of the single mode supported by the subject waveguide. Figures 3 through 5 are cross-sectional views of waveguides adapted for use in a Mach-Zehnder amplitude modulator in accordance with the invention. Referring first to a diffused surface waveguide structure, Figure 3(a) illustrates a substrate 52 of appropriate electro-optic material such as LiNb0₃ prior to diffusion of titanium (or equivalent) atoms from a metallic strip 54 of appropriate material which, in this case, is, of course, titanium. The strip 54 may be deposited onto the substrate 52 by any number of conventional processes such as electron beam evaporation or sputtering. The strip 54 for forming a waveguide in accordance with the invention is somewhat thicker than the strip 54′ shown in shadow outline for forming a conventional waveguide. For example, in a conventional device optimized for operation at 1300 nm, a titanium strip 54 having a thickness of about 70 nm might be employed. In the present invention, a strip 54 of about 95 nm thickness is used to attain the greater concentration of atoms required to enhance the refractive index of the diffused waveguide. As mentioned earlier, increasing the concentration of diffused atoms increases the refractive index of the waveguide and permits it to support the longer wavelength light despite narrowing of the input and output waveguides. Figure 3(b) is a cross-sectional view of an input (or output) waveguide of a Mach-Zehnder amplitude modulator in accordance to the invention. The waveguide comprises a surface diffusion 56 of titanium atoms. Such diffusion 56 is produced by the conventional processing of the strip 54 discussed with reference to Figure 3(a). Typically, the diffusion 56 is formed by baking the arrangement of Figure 3(a) at a temperature of about 1050 degrees C for about six (6) hours. The thickness of the strip 54, discussed above, enables one to produce a waveguide diffusion having an effective index of refraction about 2.17 as opposed to one of about 2.16 for a waveguide of a corresponding prior art device. (Note: The substrate 52 will have an index of refraction of about 2.15 for operation within the wavelength range discussed above.) As a result the longer wavelength can be guided in spite of reductions in widths of the input and output waveguide sections. A waveguide of the intermediate waveguide network is shown in shadow outline at 56′. The width of the waveguide 56′ is the same as that of the input and output waveguides of a conventional Mach-Zehnder amplitude modulator for operation at the longer wavelengths of the spectrum covered by the present invention. Figure 4 is a cross-sectional view of an input or output waveguide in accordance with an alternative embodiment of the invention. Such a waveguide is fabricated with strip waveguide technology. In such a waveguide, an overlying strip 58 of dielectric material such as glass or silicon nitride is located at the surface of a substrate 60 that includes an upper, light guiding layer 62. The layer 62 may comprise an epitaxially-grown layer of InGaAsP formed on a substrate of InP. The width of the waveguiding channel within the light guiding strip 62 is reduced (with respect to one for a prior art Mach-Zehnder modulator or for a waveguide of the intermediate network of the invention) at the input and output waveguides by reducing the width of the overlying dielectric strip 58. The bounds of a dielectric strip for either the intermediate waveguide network (or for any waveguide of the prior art device) is shown in shadow outline at 64. In the present invention, at the wavelength spectrum described above, a reduction in the width of the strip 58 from about 3µm to 2µm would be appropriate for preventing support of higher order modes at the shorter wavelength. The refractive index of the light guiding layer 62 is increased in accordance with the invention by adjusting the chemical composition of the components of the InGaAsP system prior to epitaxial deposition. The adjustment of elemental factors results in a corresponding adjustment of the refractive index of the layer 62 as is well known by those skilled in the art. In a representative strip-loaded waveguide for operation at 1300 nm, representative indices of refraction in accordance with the prior art might be approximately as follows: 3.4 (strip 58); 3.5 (waveguiding layer 62); and 3.2 (substrate 60). By modifying the chemical composition of the epitaxial light guiding layer 62, the index of refraction of that layer is preferably increased to about 3.6 (the indices of the other layers remaining the same) to accomplish operation over a predetermined optical wavelength range in accordance with the invention. Figure 5 is a cross-sectional view of a buried waveguide (input or output section) in accordance with the present invention. A waveguide 66 is embedded in a substrate 68 of appropriate material such as LiNbO₃. The buried waveguide 66 is formed within the substrate 68 by means of a conventional titanium (Ti) diffusion process followed by a second diffusion of a different material such as magnesium dioxide (MgO₂). The waveguide is formed initially at the surface by means of the standard Ti diffusion process, which raises the index of refraction in the region of the Ti diffusion. A second diffusion of MgO₂ just at the surface lowers the index of refraction slightly to offset the effect of the first diffusion. If the second diffusion is shallower than the first, the deeper part of the Ti diffused guide is unaffected, resulting in a buried waveguide, as desired. As before, the dimensions of a buried waveguide 66 of a prior art device for operation at the longer wavelength or one for use in the intermediate waveguide network of the present invention is shown in shadow outline at 70. The index of refraction of a substrate 68 for use within the wavelength range of interest is approximately 2.15, while that of the buried waveguide 70 of a prior art device is about 2.16. In the present invention, the index of refraction of the buried waveguide 66 is increased to about 2.17. As in a surface waveguide, this can be accomplished by increasing the amount of titanium deposited on the surface of the substrate prior to the first diffusion. Thus it can be seen that the present invention provides optical circuit elements for use in single mode fiber optic systems. By employing the teachings of this invention, one may enhance systems that have been limited in optical wavelength range as a result of formerly-inherent device design limitations. Accordingly, such systems are greatly enhanced in terms of cost and versatility. Furthermore, conventional design and fabrication methods may be employed to produce the enhanced devices. While this invention has been described with reference to its presently preferred embodiment, it is not limited thereto. Rather, this invention is limited only insofar as defined by the following set of patent claims.

Claims: A broadband single mode optical circuit element for use over a predetermined optical wavelength range, the circuit element comprising: an input waveguide (40), an output waveguide (42), and an intermediate waveguide network (38) in optical communication with the input waveguide (40) and the output waveguide (42), the intermediate waveguide network (38) including at least one intermediate waveguide (48 or 50) capable of supporting a plurality of modes of light within said predetermined range, the input and output waveguides (40 and 42) being configured so that each can support only the fundamental mode of light over said predetermined range, and the input and output waveguides are coupled adiabatically to the intermediate waveguide network so that the fundamental made structure is maintained in the intermediate waveguide network and the energization of higher order modes is avoided. A circuit element as in claim 1 wherein the optical circuit element is configured as a Mach-Zender modulator in which: the intermediate waveguide network (38) comprises a pair of oppositely-directed fork junctions (44, 46) joined by a parallel pair of intermediate waveguides (48, 50); each of the input and output waveguides (40, 42) intersects the apex of one of the fork junctions; the input waveguide (40) is of substantially the same width as the output waveguide (42); each of the intermediate waveguides (48, 50) is of substantially the same width as the other; and the width of the input and output waveguides is less than the width of the intermediate waveguides. A circuit element as in claim 1 or 2 and further comprising a substrate (52), the intermediate waveguides (48, 50) being integral with the substrate. A circuit element as in claim 3 wherein the optical circuit element comprises a diffused region (56) adjacent the surface of the substrate (52). A circuit element as in any of claims 1 through 4 wherein the index of refraction of the intermediate waveguides (48, 50) is sufficient to support multiple modes within the intermediate waveguide network (38) over said predetermined range. A circuit element as in any of claims 1 through 5 wherein the widths of the input and output waveguides (40, 42) are chosen so that said waveguides can support only the fundamental mode within said predetermined range. A circuit element as in any of claims 1 through 6 wherein the intermediate waveguides (48, 50) comprise a strip loaded waveguide (58). A circuit element as in any of claims 1 through 6 wherein the intermediate waveguides (48, 50) comprise a buried waveguide (66).

Inventors: DOLFI DAVID W, RANGANATH TIRUMALA R, DOLFI, DAVID W., RANGANATH, TIRUMALA R.
Applicants: HEWLETT PACKARD CO, HEWLETT-PACKARD COMPANY
Application year: 1992
Main classification: G02F1
IPC codes: G02B6, G02F1