1. Field of the Invention
The invention relates to structures with artificially patterned refractive indexes.
2. Discussion of the Related Art
A photonic crystal is a material with a refractive index that varies periodically. In a photonic crystal, the optical response results from a coherent superposition of optical waves propagating therein. Photonic crystals with sufficiently high refractive index contrasts, e.g., a contrast of more than 2, exhibit complete photonic bandgaps. A photonic bandgap prohibits electromagnetic waves from propagating in such a crystal for wave vectors at optical wavelengths.
Herein, a photonic crystal with a complete photonic bandgap will be referred to as a photonic bandgap structure. Photonic bandgap structures have applications in a variety of optical devices. Thus, processes for fabricating such structures are useful.
One process for fabricating a photonic bandgap structure involves producing a periodic array of voids in a base material. In such a void-filled photonic bandgap structure, the refractive index pattern has a high contrast if the base material has a high refractive index.
Fabricating a void-filled structure from a material with a high refractive index typically involves a multi-step template-based process. First, a reaction step produces a template with a periodic array of voids therein. Second, a fill step introduces a material with a high refractive index into the voids of the template. Third, a removal step eliminates the template material from the filled structure to produce a porous structure of the high refractive index material alone.
Such template-based fabrication processes need to account for the properties of both the template material and the filling material. In particular, the filling step must not damage the template material, and the removal step must not damage the filling material. Unfortunately, many photoresists do not withstand the process of being filled with a material having a high refractive index. Similarly, many high refractive index materials do not withstand the treatments for removing templates made of photoresists.
Various embodiments provide polymer templates and processes for fabricating the polymer templates. The polymer templates enable fabrication of porous structures from materials with high refractive indexes. In particular, the template material is compatible with being filled with a high refractive index material, and removal of the template material from the resulting structure is possible without damaging the high refractive index material. Both the filling and removal steps are typically performed at low temperatures to avoid damage to the various materials.
In one aspect, the invention features a process for forming a polymer template. The process includes exposing a photoresist including polymer molecules to a light pattern and baking the photoresist to chemically react polymer molecules in portions of the photoresist that were exposed to light of the light pattern. The reacted polymer molecules have a different solubility in a solvent than chemically unreacted polymer molecules. The process also includes washing the baked photoresist with the solvent to produce voids therein by selectively dissolving away either the reacted polymer molecules or the unreacted polymer molecules.
In another aspect, the invention features a process for forming a template of non-crosslinked polymer molecules. The process includes exposing a polymer photoresist to a light pattern to generate acid in illuminated regions of the photoresist and baking the photoresist to cause polymer molecules that are located in the illuminated regions to react with the acid. The baking step does not crosslink the polymer molecules. The process includes washing the baked photoresist in a nonpolar solvent to produce voids therein by selectively solvating either the reacted polymer molecules or the unreacted polymer molecules.
Herein, various processes involving exposure of a material to a light pattern with light and dark regions produce a void-filled structure. The resulting structures are referred to as positive tone structures if the voids occupy regions that were exposed to light regions of the light pattern. The resulting structures are referred to as negative tone structures if the voids occupy regions that were dark regions of the light pattern.
In the various Figures, like reference numbers indicate elements with similar functions.
The process 10 includes exposing a slab of photoresist to a light pattern to produce a corresponding pattern of acid in the photoresist (step 12). The photoresist is a homogenous mixture of polymer molecules, dye molecules, and photo-acid generator molecules. The light of the exposure causes the photo-acid generator molecules to produce acid, i.e. hydronium ions (H+). The distribution of H+ions corresponds to the light intensity pattern during the exposure.
Herein, a light pattern includes both an array of dark regions and an array of light regions. Exemplary light patterns are periodic in one, two, or three dimensions and have periods of about 0.1 microns and about 10 microns. i.e., mesoscopic scale periods suitable for photonic bandgap structures at telecommunications wavelengths. Such periodic light patterns result from interfering two, three, or four mutually coherent light beams. Processes for producing such light patterns are described in pending U.S. patent application Ser. No. 10/040,017, filed Jan. 4, 2002, ('017), which is incorporated herein by reference in its entirety.
The light exposure does not stimulate chemical reactions that significantly change the refractive index of the photoresist. In particular, the photochemical reactions do not polymerize, decompose, or crosslink molecules in the photoresist. Instead, the photochemical reactions produce acid, which does not significantly change the refractive index. The absence of refractive index changes insures that the light patterning will not lead to material changes that feedback and could otherwise interfere with the acid pattern formed in the photoresist. The final acid distribution forms a pattern that corresponds to the light pattern used to expose the photoresist.
The process 10 includes baking the exposed photoresist to cause polymer molecules, which are located in regions exposed by the light, to undergo a solubility change (step 14). In some embodiments, the solubility change results from generation of polar groups on the polymer molecules. In other embodiments, the solubility change results from generation of nonpolar groups on the polymer molecules. The new groups are generated by a heat-induced reaction of polymer molecules that are located in portions of the photoresist where acid was generated during the light patterning. The acid catalyzes the reaction.
The bake step proceeds at a temperature that is above the glass transition temperature of the organic polymer molecules of the photoresist and is lower than the decomposition temperature for the molecules. Exemplary bake temperatures for polymer resists are below about 350° C. and are preferably below about 200° C.
Various embodiments of the process 10 use a photoresist whose polymer molecules are initially soluble in a nonpolar solvent. For polymer molecules initially soluble in a nonpolar solvent, the acid-catalyzed reaction produces polymer molecules with more polar functional groups. The reacted polymer molecules are thus, less soluble in the nonpolar solvent and more soluble in polar solvents. After the bake, the photoresist includes a pattern of polymer molecule solubility type that tracks the light pattern used during the exposure at step 12.
In some embodiments, further chemical treatments invert the solubilities of polymer molecules located in respective light and dark regions of the light pattern as described below.
The process 10 also includes washing the baked photoresist with solvent to produce voids therein by selectively dissolving away polymer molecules of one solubility type (step 16). Exemplary washes use a nonpolar liquid as the solvent. In such solvents, the unreacted and reacted polymer molecules of the baked photoresist have different solubilities. For that reason, the wash generates a pattern of voids that tracks the light pattern originally used to exposure the photoresist. The resulting void-filled photoresist is a polymer template.
To enable the wash to produce voids, the conditions of the bake are selected to not crosslink polymer molecules. Crosslinking would significantly lower solubilities of the polymer molecules and would impede a solvent from removing the polymer template after subsequent filling with high index materials.
Processes 40 and 40′ start with a layer of photoresist 42. The photoresist is supported on a substrate 44, e.g., a glass substrate. The photoresist 42 is a homogeneous mixture whose components include soluble polymer molecules, dye molecules, photoacid generator (PAG) molecules, and solvent. Exemplary components for the photoresist 42 are shown in FIGS. 5, 6A-6C, and 7A-7B.
An exemplary polymer component for the photoresist 42 includes the polymer molecule 30 shown in
An exemplary dye component for the photoresist 42 includes one of the dye molecules 33, 34, 35 shown in
An exemplary PAG component for the photoresist 42 includes one of the molecules 36, 37 as shown in
Exemplary solvents for the photoresist 42 include hydrocarbons, fluorinated hydrocarbons, and liquid and supercritical carbon dioxide.
Referring to
The photoreaction sequence 38 does not produce changes to the refractive index in the illuminated regions 45 of the photoresist 49. Thus, the light pattern does not produce feedback, which could otherwise interfere with formation of the light pattern in the photoresist 42. For this reason, the exposure cm be performed over an extended time period and produce an acid pattern that tracks a selected light pattern.
Referring again to
Referring again to
The fabrication process 40 includes raising the pressure and temperature in the cell to values corresponding to the critical point of carbon dioxide. At the critical point conditions, the carbon dioxide is allowed to diffuse out of the template 47 thereby drying the template 47. The drying does not produce internal stresses, which could otherwise cause cracks, because critical carbon dioxide is a surface tension free fluid. Drying the template 47 in critical carbon dioxide minimizes the risk of damage due to internal surface tension forces.
The fabrication process 40 includes filling voids in the template 47 with a high refractive index material (step 22). The filling step is performed at a temperature below 350° C. and preferably below about 300° C. to avoid damaging polymer molecules, cross-linking of polymer molecules, or damaging the high refractive index material. The filling step produces filled structure 48, which includes non-crosslinked polymer molecules in regions 45 and high refractive index material elsewhere.
A variety of processes are available to fill the voids of the template 47 with a high refractive index material. Exemplary fill steps include melting a high refractive index material with a low melting temperature, e.g., selenium or bismuth, and filling the melted material into the voids of the template 47 under pressure. Other exemplary fill steps include subliming a high refractive index material having a low vaporization temperature into the voids of the template 47. Other exemplary fill steps include performing a gas-phase reaction that deposits a high refractive index byproduct it, the voids of the template 47.
The fabrication process 40 also includes washing the filled structure 48 to dissolve away the polymer molecules of the original template 47 to produce a porous structure 41 of the high refractive index material and then drying the structure (steps 24 and 26). The washing step produces a porous structure of the high refractive index material alone. For the polar polymer molecules 39 shown in
The process 40′ includes performing a vapor-phase reaction to change the solubility of a portion of the polymer molecules of the photoresist 43. The vapor-phase reaction produces a photoresist 43′ in which the polymer molecules located in the regions 45 have a changed solubility. The reaction causes these previously reacted polymer molecules to become more soluble in nonpolar solvents such as liquid or supercritical carbon dioxide.
Referring again to
The process 40′ also includes producing a void-filled polymer template 47 by washing the rebaked photoresist 43″ with fluid or supercritical carbon dioxide as already described with respect to above process 40 (step 16). The wash dissolves away the nonpolar polymer molecules that located in regions 45 thereby producing a positive tone structure in polymer template 47′. Combining the vapor-phase reaction, uniform illumination, and rebake inverted the spatial distribution of molecules soluble in polar and nonpolar solvents, respectively, to produce a positive tone template 47′ rather than the negative tone template 47 of
The fabrication process 40′ also includes filling voids in the template 47′ with a high refractive index material to produce filled structure 48′ in a manner already described with respect to process 40 (step 22). The filled structure 48′ is then washed with a solvent that solvates the non-crosslinked polymer molecules of the template 47′ to produce the porous structure of the high refractive index material (step 24).
The porous structure is dried to produce the final void-filled structure 41′ of the high refractive index material (step 26). The final void-filled structure 41′ of the high refractive index material is a positive tone structure.
From the disclosure, drawings, and claims, other embodiments of the invention will be apparent to those skilled in the art.
Number | Date | Country | |
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Parent | 10321027 | Dec 2002 | US |
Child | 11316058 | Dec 2005 | US |