1. Field of the Invention
The present invention relates to electronic devices and, more specifically, to electronic devices employing thin-film graphitic layers.
2. Description of the Prior Art
Electronic devices based on interconnected graphitic structures have been proposed as an alternative to silicon based electronics. Methods have been developed to produce and to pattern graphitic material on silicon carbide in order to produce interconnected graphitic structures.
Ultra-thin graphitic layers grow on silicon carbide crystals when they are subjected to a high temperature annealing process, in which the silicon carbide crystal is heated in a vacuum or in other controlled environments to temperatures in the range of 1200° C. to about 1500° C. for about 30 seconds to about 2 hours. At these high temperatures, silicon evaporates from the silicon carbide surface so that the surface becomes carbon rich. This carbon rich surface then converts to an ultra-thin graphitic layer consisting of from one to several hundred graphene sheets. This ultra-thin graphitic layer is also known as multi-layered graphene. Ultra-thin graphitic layers grow more quickly on the carbon terminated face of hexagonal silicon carbide, while they grow more slowly on the silicon terminated face. Under similar growth conditions, the rate of growth on the carbon terminated face is about an order of magnitude greater then on the silicon terminated face.
Ultra-thin graphitic layers can be patterned using microelectronics lithography methods to produce patterned ultra-thin graphitic layers on silicon carbide. For example, an ultra-thin graphitic layer can be patterned by applying a thin coating of poly methyl methacrylate (PMMA), which inhibits growth of graphitic layers during annealing, on an ultra-thin graphitic layer that is subsequently exposed to electron irradiation supplied by an electron beam lithographer. This causes a chemical change in the PMMA so that when the PMMA is developed, the PMMA on areas that have not been exposed to the electron beam irradiation are removed and areas that have been exposed to the electron beam remain. In this way, a PMMA pattern is produced. The pattern includes selected areas on the ultra-thin graphitic layer that are covered with PMMA and other areas where the PMMA have been removed.
Subjecting the silicon carbide crystal and graphitic layer to an oxygen plasma treatment (e.g., by using the reactive ion etching method) results in ultra-thin graphitic layers that are not covered by the PMMA being consumed by the reactive ions, resulting in a patterned ultra-thin graphitic layer on a silicon carbide crystal. Such patterned ultra-thin graphitic layers have been shown to have beneficial electronic properties.
Unfortunately, it is difficult to make extremely fine ultra-thin graphitic patterns that are required for many functional electronic structures using existing methods. A graphitic ribbon with a width that is less than 20 nm is required to produce a band gap in the graphitic ribbon that is sufficiently large for certain room-temperature electronics applications. Hence, there are many applications that require ultra-thin graphitic ribbons in which the ribbon width is less than 20 nm. Such a width may be difficult to achieve using conventional microelectronics lithography methods. Also, conventional microelectronics patterning methods applied to ultra-thin graphitic layers on silicon carbide involve processes that etch the ultra-thin graphitic layer to produce desired shapes. This etching process may produce patterned ultra-thin graphitic layers with damaged edges, which may interfere with the functionality of the graphitic structures.
Therefore, there is a need for a method for growing ultra-thin graphitic layers only on selected areas of a silicon carbide crystal.
There is also a need for a method for producing graphitic patterns on sidewalls that result from etching a silicon carbide crystal.
There is also a need for a method for producing graphitic patterns on sidewalls that that result from etching a silicon carbide crystal and at the same time to inhibit the growth of an ultra-thin graphitic layer on selected areas substantially horizontal surfaces of the silicon carbide crystal by applying a growth-inhibiting layer on those selected areas.
There is also a need for a method for producing substantially freestanding ultra-thin graphitic patterns on a silicon carbide crystal substrate.
The disadvantages of the prior art are overcome by the present invention which, in one aspect, is a method of making a vertical graphitic path on a silicon carbide crystal having a horizontal surface, in which a portion of the silicon carbide crystal is removed from the horizontal surface so as to define a vertical surface that is transverse to the horizontal surface of the silicon carbide crystal. The vertical surface is annealed so as to generate a thin-film graphitic layer on the vertical surface.
In another aspect, the invention is a method of making a graphitic structure, in which a material that inhibits formation of a graphitic layer when the silicon carbide crystal is annealed is applied to a surface of a silicon carbide crystal so as to define at least one opening that exposes a portion of the surface of the silicon carbide crystal. The portion of the silicon carbide crystal is annealed so as to generate a thin-film graphitic layer in the portion of the silicon carbide crystal.
In another aspect, the invention is a method of making a graphitic structure, in which a surface of a silicon carbide crystal is annealed so as to generate a graphitic layer having a first thickness. A layer of a mask material that inhibits generation of graphitic material in silicon carbide is applied to a portion of the graphitic layer. The surface of the silicon carbide crystal is annealed so that the graphic layer becomes thicker than the first thickness except in an area subtended by the mask material.
In another aspect, the invention is a structure that includes a crystalline substrate and a first thin-film graphitic layer. The crystalline substrate includes a horizontal surface and an elongated vertical wall transverse to the horizontal surface. The first thin-film graphitic layer is disposed on the elongated vertical wall.
In yet another aspect, the invention is an active device that includes a silicon carbide crystal, an elongated thin-film graphitic layer, a source electrode, a drain electrode, a dielectric layer and a gate electrode. The silicon carbide crystal has a horizontal surface and a vertical wall transverse to the horizontal surface. The elongated thin-film graphitic layer is disposed on the vertical wall so as to have a first end and a spaced-apart second end. The source electrode is in electrical contact with the first end of the elongated thin-film graphitic layer and the drain electrode is in electrical contact with the second end of the elongated thin-film graphitic layer. The dielectric layer is disposed over a portion of the elongated thin-film graphitic layer. The gate electrode is disposed adjacent to the dielectric layer so as to be insulated from the source electrode, the drain electrode and the elongated thin-film graphitic layer.
These and other aspects of the invention will become apparent from the following description of the preferred embodiments taken in conjunction with the following drawings. As would be obvious to one skilled in the art, many variations and modifications of the invention may be effected without departing from the spirit and scope of the novel concepts of the disclosure.
The figures are not necessarily drawn to scale and do not imply relative dimensions or angles of any of the components. Also, straight lines in the figures do not imply any degree of smoothness.
A preferred embodiment of the invention is now described in detail. Referring to the drawings, like numbers indicate like parts throughout the views. As used in the description herein and throughout the claims, the following terms take the meanings explicitly associated herein, unless the context clearly dictates otherwise: the meaning of “a,” “an,” and “the” includes plural reference, the meaning of “in” includes “in” and “on.” As used herein “vertical” refers to any first selected orientation, “horizontal” refers to any second selected orientation that is not parallel to the first selected orientation and “transverse” refers to a relationship between two objects that are at an angle relative to each other that is greater than 0° and less than 180°.
Ultra-thin graphitic layers are grown on a silicon carbide crystal by the high temperature annealing process which causes silicon to evaporate from the silicon carbide surface, which causes the surface of the crystal to become carbon-rich and form into an ultra-thin graphitic layer. Patterning is achieved either by a process in which a mask layer is applied on selected areas of the silicon carbide surface, so that silicon evaporation is inhibited; by a process where the silicon carbide is etched to produce sidewalls which are subsequently graphitized by the high temperature annealing process; or by a combination of these two processes. This may be followed by processes to remove graphitic material from selected areas on the silicon carbide substrate.
Experiments in the laboratory have demonstrated that ultra-thin graphitic layers form on the sidewalls of etched silicon carbide crystals upon being subjected to high temperature annealing. Specifically, in these experiments portions of the surface of a silicon carbide crystal was provided with an aluminum hard mask. The crystal was subsequently subjected to a reactive ion etch using CHF3 as the etching gas to etch the unprotected silicon carbide crystal to a depth of approximately 100 nm. This technique etched the silicon carbide surfaces that were not protected by the hard mask. The substantially vertical surfaces at the edges of the etched regions are referred to herein as “sidewalls.” When the etched silicon carbide crystal was subjected to the high temperature annealing process not only the horizontal surfaces, but also the sidewall surfaces acquired an ultra-thin graphitic layer. When in the high temperature annealing process, silicon evaporation from the surface of the silicon carbide under the mask was inhibited so that the surface did not become carbon rich and so that the growth rate of the ultra-thin graphitic layer was substantially reduced.
In some applications, the mask material layer includes a material that is not substantially reduced in thickness by the application of a reactive ion etch. In other applications, mask material layer includes two layers: a first layer is a material that can be coated on top of a silicon carbide surface and that substantially reduces the rate of growth of the ultra-thin graphitic layer during annealing; and a second layer on top of the first layer, which has the property that it is not removed by an ion etching procedure, used, for example to etch silicon carbide.
U.S. Pat. Nos. 7,015,142 and 7,327,000 disclose methods of generating a thin-film graphitic layer on a silicon carbide crystal (See, e.g., U.S. Pat. No. 7,015,142, col. 3, 1. 55-col. 4, 1. 65 and col. 5, 1. 62-col. 6, 1. 31). These patents are hereby incorporated by reference in support of the disclosure of methods of making thin-film graphitic layers that follows.
As shown in
At least the area of the opening 122 (and the entire surface of the crystal 110 in most practical applications) is annealed at a temperature and pressure that causes silicon to evaporate from the crystal 110, thereby leaving a horizontal thin graphitic film 130 in the region under the opening 122. The remaining mask material 120 may be removed, thereby leaving a patterned silicon carbide substrate 100.
A method of making a vertical thin film graphitic layer is shown in
The etch-resistant mask layer 220 is removed and the crystal 110 is subjected to a high temperature annealing process, thereby producing an ultra-thin graphitic layer 230 on the surfaces of the crystal 110. The ultra-thin graphitic layer 230 includes a vertical ultra-thin graphitic ribbon 232.
The ultra-thin graphitic layer 230 is subjected to a directional reactive ion etch using, for example, a inductively-coupled plasma with oxygen as the reaction gas. This process removes the portion of the graphitic layer 230 on the horizontal surfaces and leaves the graphitic material only on the vertical surfaces, leaving the ultra-thin graphitic ribbon 232 on the etched sidewall 224.
This method may be used to make two parallel vertical ultra-thin graphitic ribbons 232, as shown in
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The making of a graphitic structure of multiple depths is shown in
One example of a field effect transistor 1000 employing an ultra-thin film graphitic ribbon 1020 is shown in
The above described embodiments, while including the preferred embodiment and the best mode of the invention known to the inventor at the time of filing, are given as illustrative examples only. It will be readily appreciated that many deviations may be made from the specific embodiments disclosed in this specification without departing from the spirit and scope of the invention. Accordingly, the scope of the invention is to be determined by the claims below rather than being limited to the specifically described embodiments above.
This application claims the benefit of U.S. Provisional Patent Application Ser. No. 61/037,591, filed Mar. 18, 2008, the entirety of which is hereby incorporated herein by reference.
Number | Date | Country | |
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61037591 | Mar 2008 | US |