US 20070253661 A1
A method in effectuating the redirection of light which is propagated within a waveguide, and which eliminates the necessity for a bending of the waveguide, or the drawbacks encountered in directional changes in propagated light involving the need for sharp curves of essentially small-sized radii, which would resultingly lead to excessive losses in light. In this connection, the method relates to the fabricating and the provision of a wire-grid polarization beam splitter within an optical waveguide, which utilizes a diblock copolymer template to formulate the wire-grid.
1. A method of fabricating an optical waveguide polarization beam splitter, wherein said beam splitter incorporates a wire-grid array in said waveguide for facilitating the transmission or reflection of light propagated within said waveguide in dependence upon incident polarization of the propagated light:
a) depositing a dielectric waveguide substrate layer onto a base layer;
b) applying a light guiding film of a dielectric material onto the exposed surface of said waveguide substrate;
c) providing a diblock copolymer template having an array of pores formed therethrough;
d) masking off pores to provide a single line of said template pores;
e) etching at least one trench downwardly through said guiding film to said waveguide substrate surface;
f) depositing metal wire material into said line of pores formed in said diblock polymer template material;
g) stripping said diblock copolymer material while permitting metal wire to remain embedded in said waveguide guiding film;
h) etching off excess metal wire material down to the exposed surface of said waveguide guiding film; and
i) depositing a cover layer of a dielectric material onto said waveguide guiding film.
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14. An optical waveguide polarization beam splitter, wherein said beam splitter comprises a wire-grid array in said waveguide so as to facilitate the transmission or reflection of light propagated within said waveguide in dependence upon incident polarization of the propagated light said wire-grid array comprising a metal dot array formed within said waveguide, said waveguide further comprising a planar, slab-shaped waveguide structure having superimposed layers of a dielectric substrate, a SiO2 layer and a guiding film layer, said metal dot array extending diagonally across and downward in said guiding film layer, whereby photons of light propagated by a photonic integrated circuit having electrical field vectors parallel to the metal dot array are reflected at an angle relative to the initial direction of light with the waveguide while photons with an electrical field vector perpendicular to the metal dot array facilitate light to continue to propagate in the initial direction of transmission thereof.
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22. A waveguide polarization beam splitter, as claimed in claims 14 or 21, wherein a cover layer of a dielectric material is deposited on the guiding film layer of said waveguide structure.
1. Field of the Invention
The present invention relates to waveguide polarization beam splitters, and particularly, pertains to a wire-grid polarization beam splitter including a planar or ridged waveguide, which is adapted to either transmit or reflect light within the waveguide in dependence upon incident polarization.
Furthermore, the present invention also relates to a novel method of fabricating a waveguide polarization beam splitter, and particularly a wire-grid polarization beam splitter with a planar or a ridge waveguide, which is adapted to be utilized in order to either transmit or reflect light within the waveguide in dependence upon incident polarization.
In essence, a waveguide polarization beam splitter comprises a key element in a photonic integrated circuit, whereby beam splitters of that type can be advantageously employed as directional couplers, as well as being useful as directional modulators and switches when utilized in conjunction with a polarization rotational waveguide element.
Nevertheless, it is conceivable that problems may be encountered in connection with the redirecting of light within a waveguide, for instance, such as at an angle of 90 degrees relative to the direction of initial propagation of the light upon use thereof with a polarization-rotating element, as may be currently known in the technology.
In view of the above-mentioned problem, which is prevalent in the present-state of the technology, various investigations have been conducted and attempts made in addressing the issue of redirecting light in different directions, the latter of which are at sharp angles relative to the original direction of propagation of the light within a waveguide. Ordinarily, this redirecting of the propagated light has been implemented through the utilization of cylindrical waveguides, for example, such as in the form of optical fibers, or through the intermediary of ridged waveguides, which, however, are subject to being burdened with large losses of light, thereby resulting in poor and consequently unsatisfactory degrees of efficiencies when the radii of curvature in redirecting the lights are reduced so as to be extremely small in size. Consequently, these light losses are generally ascribed as being due to so called a micro-bending phenomenon.
2. Discussion of the Prior Art
Heretofore, this particular aspect in the problems of encountered light losses has not been fully addressed in the technology, and any practical attempt in solving this problem in the redirection of the propagated light has ordinarily be in the employment of a directional coupler. However, directional couplers are primarily passive devices and enable only a fraction of the incident light to be redirected, whereby the redirected light is again bounded by relatively large radii of curvatures, which are necessitated due to the limitations resulting from micro-bending losses. Although attempts have been made at switching all of the light successfully into one arm of a directional coupler, such as by means of LiNb03 and other kinds of electro-optical waveguide elements, the deviation of the light from the original direction thereof is, however, again limited in scope. Furthermore, although various types of wire-grid polarization beam splitters have been developed in the technology, none are designed to be operative within a waveguide and, consequently, are of essentially limited value within the context of the subject matter of the present invention.
In order to obviate or ameliorate the drawbacks which are encountered in the technology, the present invention is directed to the provision of a novel method in effectuating the redirection of light which is propagated within a waveguide, and which eliminates the necessity for a bending of the waveguide, or the drawbacks encountered in directional changes in propagated light involving the need for sharp curves of essentially small-sized radii, which would resultingly lead to excessive losses in light. In this connection, the present invention is directed to a method of fabricating and in the provision of a wire-grid polarization beam splitter within an optical waveguide, which utilizes a diblock copolymer template.
In essence, the use of diblock copolymers in connection with the forming of templates are known in the technology, having specific reference, for example, to C. T. Black and K. W. Guarini, “Structural Evolution of Cylindrical Phase Diblock Copolymer Thin Films”, J. Poly Sci. Part A 42, 1970 (2004); C. T. Black, K. W. Guarini, R. L. Sandstrom, S. Yeung and Y. Zhang, “Formation of Nanometer-Scale Dot Arrays from Diblock Copolymer Templates, Mat. Res. Soc. Symp. Proc. 728, S491 (2002); and K. W. Guarini, C. T. Black, K. R. Milkove and R. L. Sandstrom, “Sub-Lithographic Patterning Using Self-Assembled Polymers for Semiconductor Applications”, J. Vac. Sci. Tech. B, 19 2784 (2001).
All of these structures, as disclosed in the above-mentioned literature, are directed to the provision of various templates utilizing diblock copolymer template pore formations in a nanometer scale, preferably, but not limited to such as 50 to 100 nm diameter thin-film template pore formations, and wherein the basic concept thereof is generally known in the technology. However, none of the disclosures, as set forth hereinabove, or in any other prior art publications, are directed to the utilization of such diblock copolymer thin films in conjunction with a method of fabricating a waveguide wire-grid polarization beam splitter.
In connection with the foregoing, diblock copolymers provide a highly desirable variety in the formation of possible nanostructures, such as in being able to implement their size tunability and in their manufacturing process compatibility. In particular, highly acceptable diblock copolymer thin-films employable for the inventive purposes are generally constituted of suitable materials, preferably such as polystyrene (PS) or polymethylmethacrylate (PMMA), although numerous other copolymer materials would also be applicable thereto. The structures and concepts of forming such diblock copolymer thin films are readily and clearly discussed in the above-mentioned literature, which are publications of the International Business Machines Corporation, the assignee of the present application, and the disclosures of which are incorporated herein by reference in their entireties.
In particular, as set forth hereinabove, pursuant to the invention, by means of the novel waveguide wire-grid polarization beam splitter, light can be conducted at an angle of 90 degrees relative to the original direction of propagation thereof to a grid (such as in a TM mode). Thus, when an electrical field vector is perpendicular to the grid (TE mode) the direction of propagation of the light through the waveguide is undisturbed and light continues traveling in its original direction. However, when utilized with a polarization-rotating element, this device would then enable the directional switching of the light as a function of polarization.
Accordingly, it is an object of the invention to provide a novel waveguide wire-grid polarization beam splitter for the transmission or reflection of light and redirection thereof within a waveguide.
Another object of the present invention resides in the provision of an optical waveguide wire-grid polarization beam splitter, wherein the optical waveguide utilizes a diblock copolymer template for the function of the wire-grid.
A further object of the invention resides in the provision of a method of forming a waveguide wire-grid polarization splitter in a waveguide, which utilizes a diblock copolymer template for the fabrication of the wire-grid.
Reference may now be made to the following detailed description of the invention, illustrative of various embodiments and aspects in connection with the fabrication of a wire-grid polarization beam splitter within an optical waveguide through the use of a diblock copolymer template; and wherein:
Referring in specific detail to the invention, it is noted that, in essence, the structure of the waveguide polarization beam splitter is predicated on the concept that a grid of parallel metallic wires reflect radiation of one polarization while transmitting the other polarization, providing that the wavelength of the light is approximately 10 times larger than the period of the grid, or in the present instance, the metal dot array wire or wires. Through an application of this principle, it is possible to construct such a wire-grid within a waveguide structure by the inventive techniques, as disclosed and elucidated hereinbelow.
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A waveguide structure 14 of an embodiment, which is of a planar or slab-like shape, as shown in
In the case of a ridged waveguide 30, as shown in
In the case of the planar or slab-like waveguide 14, as represented in
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In essence, a method setting forth a unique and advantageous technique for fabricating the waveguide grid (such as a metal dot array wire or wires) light polarization beam splitter entails the following method steps:
Alternatively, subsequent to the dielectric substrate having been deposited, a layer of diblock copolymer of a thickness corresponding to that of the guiding film dimension, for example, 2 microns in the case of SiON, can be deposited and developed into 2 micron deep pores. This process entails use of an electric field to vertically align the diblock copolymer cylindrical pores (see, e.g.—T. Thurn-Albrecht, J. Schotter, G. A. Kastle, N. Emley, M. T. Tuominen, T. P. Russell, T. Shibauchi, L. Krusin-Elbaum, K. Guarini, and C. T. Black, “Ultrahigh Density Nanowire Arrays Grown in Self-Assembled Diblock Copolymer Templates”, Science 290, 2126 (2000)). The excess pores can be masked off, as described hereinabove in step 5), and the pores at 50 degrees relative to the direction of propagation can be filled with a metal, in accordance with step 7).
The diblock copolymer is then removed in accordance with steps 8) and 9) and a deposition of the guiding layer of the waveguide (2 microns thickness of SiON, in this instance) is followed by the deposition thereon of the dielectric cover layer.
Other alternative methods in creating the wire-grid arrays may also utilize applying porous anodic alumna to create the template of 50-100 diameter pores. This technique may also incorporate deep trench etching in a manner similar to that described above used in combination with diblock copolymer templates, wherein the anodized aluminum provides a further novel aspect, which may be utilized in conjunction with the present invention.
While the present invention has been particularly shown and described with respect to preferred embodiments thereof, it will be understood by those skilled in the art that the foregoing and other changes in forms and details may be made without departing from the scope and spirit of the present invention. It is therefore intended that the present invention not be limited to the exact forms and details described and illustrated, but fall within the scope of the appended claims.