Thorn EMI North America, Inc. v. Intel Corp.

928 F. Supp. 449, 1996 U.S. Dist. LEXIS 7864, 1996 WL 308863
CourtDistrict Court, D. Delaware
DecidedMay 28, 1996
DocketCivil Action 95-199-RRM
StatusPublished
Cited by4 cases

This text of 928 F. Supp. 449 (Thorn EMI North America, Inc. v. Intel Corp.) is published on Counsel Stack Legal Research, covering District Court, D. Delaware primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Thorn EMI North America, Inc. v. Intel Corp., 928 F. Supp. 449, 1996 U.S. Dist. LEXIS 7864, 1996 WL 308863 (D. Del. 1996).

Opinion

McKELVIE, District Judge.

This is a patent case. Plaintiff Thorn EMI North America, Inc. (“TENA”) is the owner of U.S. Patent No. 4,486,943 (“the ’943 patent”). The ’943 patent claims an improved method for fabricating metal oxide semiconductor (“MOS”) field effect transistors in a large scale integrated circuit. On March 29, 1995, TENA filed a complaint against defendant Intel Corporation (“Intel”) alleging infringement of the ’943 patent. On November 14,1995, Intel filed a motion for partial summary judgment that Intel processes P652 and P852 (revisions 9 and 10) do not infringe the ’943 patent. This is the court’s decision on Intel’s motion.

I. FACTUAL AND PROCEDURAL BACKGROUND

On January 31,1996, the court held an oral argument on Intel’s motion for partial summary judgment. The court draws the following facts from the ’943 patent claims and specification, the prosecution history of the ’943 patent, the briefs of the parties submitted in connection with Intel’s motion, the declarations of Dr. Fair, TENA’s expert, and Dr. Chung, Intel’s expert, and the oral argument.

A The Basic Technology Underlying This Lawsuit

MOS field effect transistors, or simply MOS transistors, are devices found on integrated circuit computer chips, such as static random access memory chips (“SRAMs”) and microprocessor chips. A typical microprocessor chip contains anywhere from several hundred thousand to several million MOS transistors. Each MOS transistor generates a signal by acting as a switch that can selectively turn on or off an electrical current. The signals generated by the MOS transistors on an integrated circuit chip control the operations of the computer.

1. The structure of an MOS transistor

An MOS transistor generally consists of the following sections. First, there is the “substrate,” which is the bottom layer of the transistor. The substrate is formed from a material, such as monocrystalline silicon, that is a poor conductor. Monocrystalline silicon is essentially a wafer of very pure glass made of a tightly packed and neatly organized single-crystal structure. Second, there is a “source” region at one end of the substrate and a “drain” region at the other end. The source and drain regions are areas of electrical conductivity that are formed by a process known as “doping.” Doping involves implanting certain types of ions into the substrate. These ions, which are sometimes referred to simply as impurities, essentially “rain” down onto the ends of the substrate where they become embedded.

Third, there is a “gate electrode” formed on top of the substrate between the source and drain regions of the substrate. The gate electrode may be formed either from a conductive material, such as a metal, or a non-conductive material, such as polysilicon. Polysilicon is made of loosely packed, minute pieces of silicon oriented differently from each other. If polysilicon is used, it also must be doped to become electrically conductive. Finally, the gate electrode is separated from the substrate by a relatively thin “die *451 lectric,” which is a material that does not conduct electricity. For example, a thin layer of oxide may separate the gate electrode and the substrate.

The following illustration demonstrates the various parts of an MOS transistor,

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The name “metal oxide semiconductor” field effect transistor derives from the use of a metal gate electrode on top of the substrate, an insulating oxide layer between the gate electrode and the substrate, and a substrate made from a semiconductive material. However, the term “MOS field effect transistor” now refers to any transistor that has a conductive gate electrode on top of a semi-conductive substrate with a layer of dielectric insulating the gate electrode from the substrate. For example, some of the MOS transistors manufactured by the processes claimed in the ’943 patent do not require the use of a metal gate electrode or an insulating oxide layer.

2. The operation of an MOS transistor

MOS transistors operate in the following manner. When a voltage is applied to the gate electrode on top of the substrate, a channel opens between the source and drain regions within the substrate. This allows a current to flow through the transistor, between the source and drain regions and underneath the gate electrode. This current generates a signal that is communicated to various portions of a computer in combination with the signals from other MOS transistors on the integrated circuit chip. When the voltage is turned off, the transistor ceases to generate the signal.

3. Manufacturing processes for MOS transistors before the ’943 patent

Conventional processes for manufacturing MOS transistors before the issuance of the ’943 patent involved starting with a substrate, forming an insulating dielectric on the substrate, forming a gate electrode on top of the insulating layer, doping the substrate to create the source and drain regions, and then heating the transistor. The heating is necessary to “activate” the source and drain regions, in other words, to give those areas the property of electrical conductivity. An incidental consequence of the heating step is that the ions, or impurities, in the substrate are driven deeper into the substrate and farther towards the center of the substrate. Those skilled in the art of making MOS transistors refer to this heating step as “heat driving” the source and drain regions. The movement of the source and drain regions toward the center of the substrate is referred to as “lateral diffusion.”

Using conventional techniques known before the issuance of the ’943 patent, each of these steps could be done in various ways. For example, the insulating dielectric could be deposited on top of the substrate, or it could be “grown” by heating the substrate in an oxygen oven. During the heating process, the top surface of the substrate is converted *452 into another material, such as oxide, in a manner similar to the way that metal rusts. In addition, the gate electrode could be deposited just in the middle on top of the substrate, or it could be deposited along the entire surface of the substrate and etched to remove the unnecessary portions. Finally, the gate electrode could be doped prior to the doping of the substrate, or it could be doped at the same time as the substrate.

A problem existed with these conventional techniques, however. When the source and drain regions were implanted, the edges of these regions were aligned vertically with the edges of the gate electrode before heat driving. Then the heat driving step would cause the source and drain regions to diffuse laterally underneath the gate electrode.

This “overlap” between the edges of the source and drain regions and the gate electrode caused something known in the field as “Miller capacitances.” Miller capacitances reduce the operating speed of the transistor, which is an undesirable result because the speed of a transistor is the key to its functionality and commercial desirability. Ideally, to prevent the occurrence of Miller capacitances, the edges of the source and drain regions should be aligned vertically with the edges of the gate electrode

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928 F. Supp. 449, 1996 U.S. Dist. LEXIS 7864, 1996 WL 308863, Counsel Stack Legal Research, https://law.counselstack.com/opinion/thorn-emi-north-america-inc-v-intel-corp-ded-1996.