Application of Julian Robert Anthony Beale

378 F.2d 970, 54 C.C.P.A. 1472
CourtCourt of Customs and Patent Appeals
DecidedJune 15, 1967
DocketPatent Appeal 7755
StatusPublished
Cited by4 cases

This text of 378 F.2d 970 (Application of Julian Robert Anthony Beale) is published on Counsel Stack Legal Research, covering Court of Customs and Patent Appeals primary law. Counsel Stack provides free access to over 12 million legal documents including statutes, case law, regulations, and constitutions.

Bluebook
Application of Julian Robert Anthony Beale, 378 F.2d 970, 54 C.C.P.A. 1472 (ccpa 1967).

Opinions

RICH, Judge.

This appeal is from the decision of the Patent Office Board of Appeals affirming the rejection of claims 52-54 of application serial No. 676,563, filed August 6, 1957, originally entitled “Method of Manufacturing Semi-Conductor Devices.”

Appellant Beale copied the three appealed claims from Schwartz et al. patent (hereinafter “Schwartz”) No. 3,001,895 1 to provoke an interference. They stand rejected on the sole ground of lack of support in Beale’s specification. The examiner’s language was that the claims are “unwarranted by the disclosure.”

[971]*971The single issue in this case presents a simple problem of law, which turns on a single word, against the background of a very complex technology, some understanding of which is necessary to a comprehension of the issue.

The process of the appealed claims is directed to the making of junction transistors and is, we are told, now known in the art as the alloy-diffusion process. The claims are broad enough to cover the making of either P-N-P or N-P-N junction transistors but the drawings and illustrative embodiments in both cases relate to the P-N-P type and we shall therefore use that type in explaining the invention. Reproduced below are Figs. 2, 3, and 4 of Schwartz showing stages in the production, followed by Fig. 1 which illustrates a finished transistor.

In viewing these drawings it should be borne in mind that they are in reality schematic diagrams greatly exaggerated in size and not showing the various parts in their true relative proportions.

Referring to Figs. 2, 3, and 4, a small piece or wafer of semiconductor material 11, such as germanium (Ge) of p-type conductivity, is provided by diffusion with a relatively thin surface layer 12 of opposite or n-type conductivity, the two layers providing a PN junction 5. As shown in Fig. 3, a small quantity or pellet 13 of alloy is placed on an exposed surface of layer 12, heated to a temperature above its melting point but below the melting point of the germanium crystal, held at temperature for a desired time and then cooled, producing a structure illustrated in Fig. 4.

The controversy here revolves about the composition of alloy pellet 13. According to the claims, it comprises a “carrier” and two conductivity-type directing impurities which are of opposite types. In this art, one impurity is known as an acceptor impurity which creates p-type conductivity when incorporated in a semiconductor body and the other is known as a donor impurity which creates n-type conductivity in a semiconductor body. Exemplary materials involved in this case are gallium (Ga) which is an acceptor and antimony (Sb) which is a donor. The n-type layer 12 in Figs 2 and 3 may be produced by diffusion of Sb into the surface of the Ge crystal 11. One of Schwartz’ alloy examples is 96.6% [972]*972lead 2 as carrier, 0.2% antimony and 0.2% gallium. To indicate the true size of what is shown in the drawings in an actual transistor, the Ge crystal wafer is described in one Schwartz example as .06 x .06 inch, and .006 inch thick. The other example describes the Ge crystal as .0023 inch thick with arsenic, another donor impurity, diffused into its surface to produce the n-type layer to a depth of 0.0005 inch. Pellet 13 is described as a .01 x .01 inch cylinder.

There are other qualifying factors with respect to the acceptor and donor impurities contained in the alloy pellet of importance to the practice of the claimed invention. The donor is selected so that it has a much higher diffusion constant than the acceptor, that is, it advances faster into the crystal from the melt. The impurities are also selected so that the acceptor solubility in the germanium is higher than that of the donor.

Referring to Fig. 4, when the alloying pellet 13 containing the donor and acceptor impurities is fused to the crystal surface 12 by heating the pellet in contact with the crystal until it melts, a number of things occur. A small portion of the Ge crystal dissolves in the melt, forming a small crater the depth of which represents the furthest advance of the melt (liquid-solid inter-face or alloy-front), determined by the temperature and the solubility of the Ge in the alloy. The melt quickly saturates and can accept no more Ge. Solid-state diffusion of the impurities in the melt takes place into the underlying Ge solid crystal 11. The donor, having the higher diffusion constant advances faster into the Ge. Heating is continued until the advancing donor impurity converts the underlying p-type Ge to n-type Ge, shown at 12A. It will be noted that this n-type layer joins the diffused n-type layer 12, previously formed. The n-type Ge layer, 12-12A, constitutes the active “base” layer of the transistor. Its position in the crystal and particularly its thickness are important to obtaining the desired electrical characteristics and the invention involves control of these parameters but it is not deemed necessary to decision to discuss them.

As the melt cools, further significant events take place. Diffusion terminates, fixing the location of the collector-base junction, portion 11 of p-type Ge becoming the “collector.” As the melt begins to solidify, the solubility of the Ge dissolved in it decreases and atoms of Ge precipitate out and regrow at the original solid crystal lattice, forming a recrystallized Ge region 6. The impurities having been selected so that acceptor solubility in the Ge was higher than that of the donor, more acceptor impurities exist in the recrystallized Ge region 6 than donor impurities with the result that region 6 exhibits p-type conductivity and forms an “emitter” junction with the adjacent diffused base region 12A. The cooled pellet 13, being metallic, forms an ohmic 3 conductive contact to the emitter recrystallized region. A conductor 8 may be attached thereto as shown in Fig. 1. A collector contact and conductor 10 are attached to the other side of the original Ge crystal and a base contact 9 is applied to surface 12, thus producing the finished transistor of Fig. 1.

We have used the Schwartz drawings only because they seem easier to read and are more detailed but Beale’s drawings show substantially the same thing, additionally showing an oven in which the melting can be done in a hydrogen atmosphere and in the presence of a vaporized antimony source as a donor impurity to provide the diffused n-type conductive layer 12 on the original p-type germanium crystal wafer 11. Typical heating is to 700-800° C. for from 20 minutes to an hour.

[973]*973Claim 52, which may now be at least partially intelligible to the reader, is as follows:

52. The process of making a transistor comprising, a first step of heating a semiconductor body of an original conductivity-type in contact with a material comprising a carrier,

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Application of Julian Robert Anthony Beale
378 F.2d 970 (Customs and Patent Appeals, 1967)

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Bluebook (online)
378 F.2d 970, 54 C.C.P.A. 1472, Counsel Stack Legal Research, https://law.counselstack.com/opinion/application-of-julian-robert-anthony-beale-ccpa-1967.