The present invention is a novel structure for a field effect transistor having a buried channel graphene layer and a method for forming such structure.
Graphene has been shown to be an excellent material for use as the channel layer in field effect transistors (FETs). It exhibits high carrier mobility and low noise properties. However, the manufacture of FETs with graphene channel layer has met with certain problems.
One such problem is that the gate dielectric, which must be present between the graphene layer and the gate electrode, usually causes severe degradation of channel mobility in the graphene layer. Commonly used methods for depositing high-K gate dielectrics include atomic level deposition (ALD) and evaporation.
For ALD high-k gate dielectrics, the coverage of the high-k film on graphene is usually poor. To enhance coverage, surface pre-treatment or seed layer are usually used. Such surface pre-treatment or seed layer usually causes severe doping of the graphene and can cause mobility degradation as well. Evaporated high-k gate dielectrics also demonstrate the same problem of degrading mobility of electrons in the graphene layer.
To overcome these problems, the present invention provides a novel buried-channel graphene FET structure and method for manufacture. The new structure includes a two level channel layer comprised of the buried-channel graphene layer with an amorphous silicon top channel layer.
The method for making such structure includes the steps of depositing a graphene layer on a substrate, depositing an amorphous silicon layer (a-Si) on the graphene layer, converting the upper layer of the a-Si layer to gate dielectrics by nitridation or oxidation, while keeping the bottom of the a-Si layer to serve as part of the channel to form the buried-channel graphene FET.
The advantages of this new structure include: (1) high quality of gate dielectrics with low leakage and low trap density; and (2) high mobility of the underneath graphene channel, since it is protected by the thin a-Si layer during gate dielectric and metal gate electrode formation. This contributes to high speed, low power and long lifetime of the device.
Additional features and advantages are realized through the techniques of the present invention. Other embodiments and aspects of the invention are described in detail herein and are considered a part of the claimed invention. For a better understanding of the invention with the advantages and the features, refer to the description and to the drawings.
The subject matter which is regarded as the invention is particularly pointed out and distinctly claimed in the claims at the conclusion of the specification. The forgoing and other features, and advantages of the invention are apparent from the following detailed description taken in conjunction with the accompanying drawings in which:
The terminology used herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the invention. As used herein, the singular forms “a”, “an” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise. It will be further understood that the terms “comprises” and/or “comprising,” when used in this specification, specify the presence of stated features, integers, steps, operations, elements, and/or components, but do not preclude the presence or addition of one or more other features, integers, steps, operations, element components, and/or groups thereof.
The corresponding structures, materials, acts, and equivalents of all means or step plus function elements in the claims below are intended to include any structure, material, or act for performing the function in combination with other claimed elements as specifically claimed. The description of the present invention has been presented for purposes of illustration and description, but is not intended to be exhaustive or limited to the invention in the form disclosed. For example, the invention is applicable to all types of graphene devices, including logic, such as field effect transistors, and analog, such as RF amplifiers. Many other modifications and variations will be apparent to those of ordinary skill in the art without departing from the scope and spirit of the invention. The embodiment was chosen and described in order to best explain the principles of the invention and the practical application, and to enable others of ordinary skill in the art to understand the invention for various embodiments with various modifications as are suited to the particular use contemplated.
The flow diagrams depicted herein are just one example. There may be many variations to this diagram or the steps (or operations) described therein without departing from the spirit of the invention. For instance, the steps may be performed in a differing order or steps may be added, deleted or modified. All of these variations are considered a part of the claimed invention.
With reference to
The graphene layer 102 can be formed by various processes such as sublimation process on SiC wafer, CVD grown in metals substrate (such as Ni or Cu), or mechanical exfoliated from natural graphite, etc. as is well known in the art. The thickness of the graphene layer 102 is in the range of 0.35 nm to 3.5 nm,
With reference to
With reference to
To achieve a controlled conversion process to ensure that the remaining lower layer of the amorphous silicon layer 106a remains as the surface channel, the process parameters must be selected carefully. Generally, amorphous silicon layer 106 is deposited with a thickness in the range of 2 nm-15 nm. During the nitridation, oxidation or oxynitridation process, 1 nm to 8 nm of the upper layer of the amorphous silicon layer 106b is consumed, which results in a thickness of the dielectric layer of oxide, nitride or oxynitride 108 in the range of 1.1 nm to 15 nm (The thickness ratio of the formed gate dielectrics to the consumed amorphous silicon is dependent on the oxygen/nitrogen ratio in the formed gate dielectrics). This leaves the thickness of the lower layer of amorphous silicon 106a in the range of 1 nm to 7 nm.
In the preferred embodiment, amorphous silicon layer 106 is depositing with a thickness in the range of 3 nm-7 nm. The upper layer of amorphous silicon layer 106b is consumed in the oxidation/nitridation process to a depth of 1.5 nm-4 nm, which results in an oxide, nitride or oxynitride layer 108 in the range of 1.7 nm to 7.6 nm thick. This leaves a lower layer of amorphous silicon 106a in the range of approximately 1.5 nm to 3 nm thick remaining as the surface channel. As one example of the process, the amorphous silicon can be converted to oxynitride using furnace oxynitridation at temperatures in the range of 700° C. to 1000° C. in N2O for 10 to 40 mins.
The lower layer of amorphous silicon 106a serves as the surface channel while the underneath graphene layer 102 serves as the buried channel. The resulting structure is show in
With reference to
Option 2, shown in
The gate electrode 112 can be formed either before source/drain contacts 110, at the same time or after them as well known in the art. The gate electrode 112 can be polysilicon, silicide, Ti, TiN, W, TaN, Al, Pb, Re, Au, Ni, etc.
While the preferred embodiment to the invention had been described, it will be understood that those skilled in the art, both now and in the future, may make various improvements and enhancements which fall within the scope of the claims which follow. These claims should be construed to maintain the proper protection for the invention first described.
This invention was made with Government support under FA8650-08-C-7838 awarded by Defense Advanced Research Projects Agency. The Government has certain rights to this invention.