METHOD FOR MAKING A
SEMICONDUCTOR DEVICE HAVING A
HIGH-K GATE DIELECTRIC
This is a Divisional application of Ser. No.: 10/618,226 filed Jul. 11, 2003, which is now abandoned, and which is a Continuation application of Ser. No.: 10/082,530 tiled Feb. 22, 2002, now U.S. Pat. No. 6,617,209.
FIELD OF THE INVENTION
The present invention relates to methods for making semiconductor devices, in particular, semiconductor devices that include high-k gate dielectric layers.
BACKGROUND OF THE INVENTION
MOS field-effect transistors with very thin gate dielectrics made from silicon dioxide may experience unacceptable gate leakage currents. Forming the gate dielectric from certain high-k dielectric materials, in place of silicon dioxide, can reduce gate leakage. Such a dielectric may not, however, be compatible with polysilicon—the preferred material for making the device's gate electrode. Placing a thin layer of titanium nitride, which is compatible with many high-k gate dielectrics, between a high-k gate dielectric and a polysilicon-based gate electrode may enable such a dielectric to be used with such a gate electrode. Unfortunately, the presence of such a layer may increase the transistor's threshold voltage, which is undesirable.
Accordingly, there is a need for an improved process for making a semiconductor device that includes a high-k gate dielectric. There is a need for such a process in which a polysilicon-based gate electrode is formed on such a gate dielectric to create a functional device—without causing undesirable work function shifts. The method of the present invention provides such a process.
BRIEF DESCRIPTION OF THE DRAWINGS
FIGS. la-Id represent cross-sections of structures that may be formed when carrying out an embodiment of the method of the present invention.
DETAILED DESCRIPTION OF THE PRESENT
A method for making a semiconductor device is described. That method comprises forming on a substrate a dielectric layer that has a dielectric constant that is greater than the dielectric constant of silicon dioxide. That dielectric layer is modified so that it will be compatible with a gate electrode to be formed on it. A gate electrode is then formed on the dielectric layer. In the following description, a number of details are set forth to provide a thorough understanding of the present invention. It will be apparent to those skilled in the art, however, that the invention may be practiced in many ways other than those expressly described here. The invention is thus not limited by the specific details disclosed below.
In an embodiment of the method of the present invention, as illustrated by FIGS. la-Id, dielectric layer 101 is formed on substrate 100. Substrate 100 may include isolation regions, p-type wells and n-type wells that have been formed in a bulk silicon or silicon-on-insulator substructure. Substrate 100 may comprise other materials—which may or may not be combined with silicon—such as: germanium,
indium antimonide, lead telluride, indium arsenide, indium phosphide, gallium arsenide, or gallium antimonide. Although several examples of materials from which substrate 100 may be formed are described here, any material
5 that may serve as a foundation upon which a semiconductor device may be built falls within the spirit and scope of the present invention.
Dielectric layer 101 comprises a material that has a dielectric constant that is greater than the dielectric constant
10 of silicon dioxide. Dielectric layer 101 preferably has a dielectric constant that is at least about twice that of silicon dioxide, i.e., a dielectric constant that is greater than about 8. When serving as the gate dielectric for the semiconductor device, dielectric layer 101 is a "high-k gate dielectric."
15 Some of the materials that may be used to make high-k gate dielectrics include: hafnium oxide, lanthanum oxide, zirconium oxide, zirconium silicon oxide, titanium oxide, tantalum oxide, barium strontium titanium oxide, barium titanium oxide, strontium titanium oxide, yttrium oxide,
20 aluminum oxide, lead scandium tantalum oxide, and lead zinc niobate. Particularly preferred are hafnium oxide, zirconium oxide, titanium oxide, and aluminum oxide. Although a few examples of materials that may be used to form dielectric layer 101 are described here, that layer may
25 be made from other materials that serve to reduce gate leakage from the level present in devices that include silicon dioxide gate dielectrics.
Dielectric layer 101 may be formed on substrate 100 using a conventional deposition method, e.g., a conventional
30 chemical vapor deposition ("CVD"), low pressure CVD, or physical vapor deposition ("PVD") process. Preferably, a conventional atomic layer CVD process is used. In such a process, a metal oxide precursor (e.g., a metal chloride) and steam may be fed at selected flow rates into a CVD reactor,
35 which is then operated at a selected temperature and pressure to generate an atomically smooth interface between substrate 100 and dielectric layer 101. The CVD reactor should be operated long enough to form a layer with the desired thickness. In most applications, dielectric layer 101
40 should be less than about 100 angstroms thick, and more preferably between about 20 angstroms and about 60 angstroms thick.
As deposited, dielectric layer 101 will include undesirable impurities, e.g., hydrogen and/or unreacted metal (repre
45 sented by dots in FIG. la), which render that layer incompatible with polysilicon. In the method of the present invention, dielectric layer 101 is modified so that it will be compatible with a gate electrode to be formed on it. FIGS. la 1c illustrate steps that may be applied to modify dielec
50 trie layer 101. First, sacrificial layer 102 is formed on dielectric layer 101 to generate the structure represented by FIG. la. Sacrificial layer 102 preferably is made from a material that may getter impurities from dielectric layer 101. An example of a suitable material is titanium nitride. Such
55 a titanium nitride layer may be formed on dielectric layer 101 using a conventional CVD or PVD process. In a preferred embodiment, such a process is used to form a titanium nitride layer that is between about 10 angstroms and about 50 angstroms thick.
60 After sacrificial layer 102 is formed on dielectric layer 101, undesirable impurities are transported from dielectric layer 101 to sacrificial layer 102. When sacrificial layer 102 is made from titanium nitride and dielectric layer 101 comprises a high-k gate dielectric layer, impurities may be
65 transported from high-k gate dielectric layer 101 to titanium nitride layer 102 by annealing titanium nitride layer 102. Titanium nitride layer 102 may be annealed using a rapid