Field effect transistor

This application claims the priority benefit of provisional application Ser. No. 61/569,789, filed Dec. 13, 2011, the full disclosure of which is incorporated herein by reference. This application also claims the priority benefit of Taiwan application serial no. 101141319, filed Nov. 7, 2012, the full disclosure of which is incorporated herein by reference.

1. Technical Field

The disclosure relates to a semiconductor device. More particularly, the disclosure relates to a metal oxide semiconductor transistor.

2. Description of Related Art

Metal oxide semiconductor transistor is a transistor using metal oxide semiconductor layer to be its active layer. Comparing with those transistors using amorphous silicon layer as their active layers, the metal oxide semiconductor transistors have higher charge carrier mobility. While comparing with those transistors using low-temperature polysilicon layer as their active layers, the metal oxide semiconductor transistors have simpler manufacturing process and more uniform metal oxide semiconductor layers to make the metal oxide semiconductor transistors have better performance.

At the present time, increasing the mobility of the charge carriers is a method to further improve the performance of the transistors. One of the common ways is to crystallize the transistor's active layer to form a polycrystalline structure. For example, the transistors using polysilicon layer to be the active layer can have higher charge carriers mobility. However, the formation of the polysilicon increases the difficulty of the manufacturing process, and the non-uniformity of the polysilicon layer decreases the performance of the transistor. Besides, changing the material of the active layer is another way to increase the mobility of the transistors' charge carrier, but the R&D difficulty for finding new replaceable materials is also increased. Therefore, it is unfavorable to increase the improving rate of the transistors' performance.

In one aspect, the present invention is directed to a field effect transistor (FET) having improved charge carriers mobility.

The FET includes a gate, a gate insulating layer, an active layer, a source, and a drain. The gate, the gate insulating layer and the active layer are sequentially stacked on a substrate. The active layer has a first surface and a second surface opposite to the first surface. A first band gap value at the first surface and a second band gap value at the second surface are different. The source and the drain respectively connect to the active layer.

According to an embodiment, the difference between the first band gap value and the second band gap value are at least 0.5 eV.

According to another embodiment, the FET further includes a third metal oxide semiconductor layer located between the two different metal oxide semiconductor layers. A third band gap value of the third metal oxide semiconductor layer also between the first band gap value and the second band gap value.

According to yet another embodiment, the gate, the source and the drain are located on the same side of the active layer.

According to yet another embodiment, the gate is located on one side of the active layer, and the source and the drain are located on the opposite side of the active layer.

The foregoing presents a simplified summary of the disclosure in order to provide a basic understanding to the reader. This summary is not an extensive overview of the disclosure and it does not identify key/critical elements of the present invention or delineate the scope of the present invention. Its sole purpose is to present some concepts disclosed herein in a simplified form as a prelude to the more detailed description that is presented later. Many of the attendant features will be more readily appreciated as the same becomes better understood by reference to the following detailed description considered in connection with the accompanying drawings.

FIG. 1 is a cross-sectional diagram of a field effect transistor according to an embodiment of this invention.

FIG. 2 is a cross-sectional diagram of a field effect transistor according to another embodiment of this invention.

FIG. 3 is a cross-sectional diagram of a field effect transistor according to yet another embodiment of this invention.

FIG. 4 is a cross-sectional diagram of field effect transistor according to yet another embodiment of this invention.

Accordingly, a field effect transistor (FET) having improved electron mobility is provided. In the following detailed description, for purposes of explanation, numerous specific details are set forth in order to provide a thorough understanding of the disclosed embodiments. It will be apparent, however, that one or more embodiments may be practiced without these specific details. In other instances, well-known structures and devices are schematically shown in order to simplify the drawing.

The FET includes a gate, a gate insulating layer, an active layer, a source, and a drain. According to an embodiment, the gate, the gate insulating layer and the active layer are sequentially stacked on a substrate. The source and the drain respectively connect to the active layer.

According to another embodiment, the gate, the source and the drain are located on the same side of the active layer. According to yet another embodiment, the gate is located on one side of the active layer, and the source and the drain are located on the opposite side of the active layer. The material of the gate, the source and the drain can be doped semiconductor material, metal silicide, or metal, for example. The material of the gate insulating layer can be silicon oxide, silicon nitride, silicon oxynitride, or other dielectric materials having high dielectric constant, for example.

The active layer has a first surface and a second surface opposite to the first surface. A first band gap value at the first surface and a second band gap value at the second surface are different. Therefore, the active layer has at least two different amorphous metal oxide semiconductor layers stacked together to make the first band gap value at the first surface and a second band gap value at the second surface different.

According to an embodiment, the difference between the first band gap value and the second band gap value are at least 0.5 eV, such as at least 1 eV, to effectively increase the electron mobility in the active layer. The metal oxide semiconductor materials combined for the active layer can be selected from the following metal oxide semiconductor materials, such as indium gallium zinc oxide (IGZO) indium gallium oxide (IGO) indium zinc oxide (IZO) zinc oxide (ZnO) calcium oxide (CaO) magnesium oxide (MgO) aluminum oxide (Al 2 O 3 ), indium xoide (In 2 O 5 ), gallium oxide (GaO 2 ), titanium oxide (TiO 2 ), zirconium oxide (ZrO 2 ), and other suitable metal oxide semiconductor materials. At least two different metal oxide semiconductor materials are stacked to form the active layer above to make the first surface and the second surface have different band gap values.

After stacking two different metal oxide semiconductor layers, a heterojunction structure is usually formed to accumulate high density electrons, and thus effectively increase electron mobility. This phenomenon is very common in III-V semiconductor material with single crystal structure, and is used by high electron mobility transistor (HEMT) to greatly increase the electron mobility thereof. In polycrystalline system, Huai-An Chin (Journal of Applied Physics 108, 054503 (2010)) observed a similar phenomenon occurred in MgZnO/ZnO system. However, in amorphous system, no one ever predict or observe the similar phenomenon. The reason may be that electrons can easily move within one single crystal, but jump over the interface between different crystal grains is a very difficult thing. Therefore, the crystallinity of a material is poorer, the electron mobility is poorer.

Accordingly, the active layer of the FET are composed by at least two different amorphous metal oxide semiconductor layers, the electron mobility still can be increased. This is an unexpected result for persons skilled in the art. Some embodiments are described below to detail illustrate the FET structure.

FIG. 1 is a cross-sectional diagram of a field effect transistor according to an embodiment of this invention. In FIG. 1 , the field effect transistor 100 includes a gate 120 , a gate insulating layer 130 , a source 140 a , a drain 140 b and an active layer 150 . The active layer 150 has a first surface 150 a and a second surface 150 b opposite to the first surface 150 a . The gate 120 , the gate insulating layer 130 , and the active layer 150 are sequentially stacked on the substrate 110 . The source 140 a and the drain 140 b are located between the gate insulating layer 130 and the active layer 150 and separated by a distance. That is, the gate 120 , the source 140 a and the drain 140 b are all disposed below the active layer 150 .

According to an embodiment, the active layer 150 has at least two different metal oxide semiconductor layers stacked together (not shown in FIG. 1A ) and positioned respectively at the sides of the first surface 150 a and the second surface 150 b . According to another embodiment, the above two different metal oxide semiconductor layers can be gradually mixed together, so that the first band gap value at the side of the first surface 150 a can gradually change to the second band gap value at the side of the second surface 150 b. According to yet another embodiment, at least a third metal oxide semiconductor layer can be sandwiched between the above at least two different metal oxide semiconductor layers. The third band gap value of the third metal oxide semiconductor layer is between the first band gap value at the first surface 150 a and the second band gap value at the second surface 150 b of the active layer 150 .

For example, an amorphous indium gallium zinc oxide (a-IGZO) layer was located at the first surface 150 a of the active layer 150 . A calcium metal layer was then stacked on the a-IGZO layer. The calcium diffused into the a-IGZO layer and then oxidized by the a-IGZO layer to form an amorphous indium gallium zinc calcium oxide (a-IGZCaO) layer at the second surface 150 b. Therefore, a heterojunction structure of a-IGZO/a-IGZCaO was formed. The result above was affirmed by X-ray photoelectron spectroscopy (XPS). The electron mobility of a-IGZO was 12 cm 2 V −1 s −1 , and the electron mobility of a-IGZO/a-IGZCaO was increased to 160 cm 2 V −1 s −1 . This surprising result is completely unexpected.

FIG. 2 is a cross-sectional diagram of a field effect transistor according to another embodiment of this invention. In FIG. 2 , the field effect transistor 200 includes a gate 220 , a gate insulating layer 230 , a source 240 a , a drain 240 b and an active layer 250 . The active layer 250 has a first surface 250 a and a second surface 250 b opposite to the first surface 250 a . The gate 220 , the gate insulating layer 230 , and the active layer 250 are sequentially stacked on the substrate 210 . The source 240 a and the drain 240 b are located on the active layer 250 and separated by a distance. That is, the gate 220 is disposed below the active layer 150 , and the source 140 a and the drain 140 b are located on the active layer 250 . Since the details of the active layer 250 is the same as the active layer 150 in FIG. 1 above, and hence omitted here.

FIG. 3 is a cross-sectional diagram of a field effect transistor according to yet another embodiment of this invention. In FIG. 3 , the field effect transistor 300 includes a gate 320 , a gate insulating layer 330 , a source 340 a , a drain 340 b and an active layer 350 . The active layer 350 has a first surface 350 a and a second surface 350 b opposite to the first surface 350 a . The active layer 350 , the gate insulating layer 330 , and the gate 320 are sequentially stacked on the substrate 310 . The source 340 a and the drain 340 b are located on the active layer 350 and separated by a distance. That is, the gate 320 , the source 340 a , and the drain 340 b are all disposed on the active layer 350 . Since the details of the active layer 350 is the same as the active layer 150 in FIG. 1 above, and hence omitted here.

FIG. 4 is a cross-sectional diagram of a field effect transistor according to yet another embodiment of this invention. In FIG. 4 , the field effect transistor 400 includes a gate 420 , a gate insulating layer 430 , a source 440 a , a drain 440 b and an active layer 450 . The active layer 450 has a first surface 450 a and a second surface 450 b opposite to the first surface 450 a . The active layer 450 , the gate insulating layer 430 , and the gate 420 are sequentially stacked on the substrate 410 . The source 440 a and the drain 440 b are located between the active layer 450 and the substrate 410 , and separated by a distance. That is, the gate 420 is located on the active layer, and the source 440 a and the drain 440 b are disposed below the active layer 450 . Since the details of the active layer 450 is the same as the active layer 150 in FIG. 1 above, and hence omitted here.

According to the embodiments above, it can be known that if the active layer of a FET comprises at least two amorphous metal oxide semiconductor layers stacked together, a heterojunction structure can be also formed to greatly increase the electron mobility of the active layer, and the performance of the FET is thus greatly improved.

All the features disclosed in this specification (including any accompanying claims, abstract, and drawings) may be replaced by alternative features serving the same, equivalent or similar purpose, unless expressly stated otherwise. Thus, each feature disclosed is one example only of a generic series of equivalent or similar features.