GaAs single crystal as well as method of producing the same,...

Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode

Reexamination Certificate

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C257S613000

Reexamination Certificate

active

06297523

ABSTRACT:

BACKGROUND OF THE INVENTION
The present invention relates to the single crystal of GaAs semiconductor as well as a method of producing the same, and a semiconductor device utilizing the GaAs single crystal. In particular, the present invention is well suited to make uniform the characteristics of semiconductor elements which are fabricated in a wafer of GaAs semiconductor.
Among factors which dominate the dispersion of semiconductor elements fabricated in a wafer, those attributed to a crystal structure such as resistivity and FET characteristics have heretofore been considered to be the distribution of etch pit densities and the ununiform distribution of an impurity substance within the wafer, but they have not been clarified yet. Reports on them having hitherto been made include the following:
(1): Yoshizumi TSUNODA, Masayoshi MATSUI and Takeshi YOKOYAMA
Collection of Drafts of Lectures in 30th Spring Symposium of Applied Physics Society (1983), 4p-D-10, p. 437
(2): Yasunobu ISHII, Shintaro MIYAZAWA, Akira ISHIDA and Hajime YAMASAKI
Collection of Drafts of Lectures in 31st Spring Symposium of Applied Physics Society (1984), 1p-D-5, p. 633
(3): Yoshiro HIRAYAMA, Shintaro MIYAZAWA and Hajime YAMASAKI
Collection of Drafts of Lectures in 31st Spring Symposium of Applied Physics Society (1984), 1p-D-6, p. 633
SUMMARY OF THE INVENTION
An object of the present invention is to provide the structure of a crystal in the shape of a wafer for making uniform the electrical characteristics of semiconductor elements to be fabricated in the wafer of a GaAs semiconductor single crystal, from a novel viewpoint, as well as a method of producing the same, and a semiconductor device utilizing the crystal.
The inventors have found out that, among factors which dominate the distribution of the characteristics of semiconductor elements fabricated in a GaAs single crystal wafer, an important one attributed to a crystal structure is the discrepancy of the lattice constants of the GaAs single crystal in the wafer. For example, in case of fabricating field effect transistors (FETs), an intense correlation has been found out between the distribution of lattice distortions in the wafer and the distribution of the threshold voltages of the FETs as will be described in detail later.
The present invention is based on such new knowledge, and achieves the uniformity of the characteristics of semiconductor elements by adjusting the discrepancy of the lattice constants of a GaAs single crystal. At present, the inventors do not know any measure in which the distribution of lattice constants in a wafer is taken into consideration.
It is important for obtaining a semiconductor device satisfactorily functioning in practical use that the range of distribution in the wafer of a GaAs single crystal is set in a predetermined range.
More specifically, the discrepancy D of lattice constants at a normal temperature in a wafer as measured with a region 1-100 mm
2
in area taken as one unit is set as follows:
D/d
o
≦4×10
−5
  (1)
(where d
o
denotes the lattice constant of a GaAs single crystal of its stoichiometric composition at the normal temperature (23±1° C.), D=&Dgr;d
max
−&Dgr;d
min
holds with &Dgr;d
max
being the maximum value of &Dgr;d in the wafer and &Dgr;d
min
being the minimum value of &Dgr;d in the wafer, and &Dgr;d=(d−d
o
) holds in which d denotes the lattice constant of the GaAs wafer at the normal temperature).
In this regard, when the discrepancy in the wafer is suppressed to be too small, the production of the GaAs single crystal becomes difficult, and the reproducibility of the production might be spoilt. It is accordingly reasonable that the discrepancy in the wafer is at least 4×10
−6
.
By the way, in case of fabricating field effect transistors or the likes with a GaAs single crystal wafer, it has been considered desirable to set the density of Si atoms of the GaAs single crystal to a value less than 1×10
15
cm
−3
. The inventors' study, however, has revealed that with GaAs single-crystals having hitherto been produced, the densities of Si atoms of which are not higher than 1×10
16
cm
−3
, none of the distributions of lattice constants in the wafers of the GaAs crystals satisfies the aforementioned equation (1) in terms of D/d
o
as shown by a lattice distortion distribution curve
1
in FIG.
1
.
That is, in the case of fabricating the FETs or the likes satisfactorily functioning in practical use by employing the GaAs single crystal, there has not been any GaAs single crystal which realizes the discrepancy of lattice constants in the wafer thereof as meets the aforementioned equation (1). The present invention achieves uniformity in the characteristics of semiconductor devices, e.g., the threshold voltages thereof using a GaAs single crystal the density of contained Si atoms of which is at most 1×10
16
cm
−3
, this value permitting the semiconductor devices such as field effect transistors to function satisfactorily in practical use, and with which the distribution of lattice constants in the wafer of the single crystal satisfies the aforementioned equation (1).
In accordance with the present invention as described above, the distribution of the characteristics of semiconductor elements in a wafer can be sharply reduced, which can bring forth the effect of enhancing the production yields of ICs or LSIs in which the semiconductor elements are integrated at high densities. Besides, the invention is effective for the high speed operations of ICs and LSIs for the same reason.


REFERENCES:
patent: 2908004 (1959-10-01), Levinson
patent: 3033660 (1962-05-01), Okkerse
patent: 3446603 (1969-05-01), Loiacono et al.
patent: 3833342 (1974-09-01), Holliday et al.
patent: 4299650 (1981-11-01), Bonner
patent: 4544417 (1985-10-01), Clarke et al.
patent: 4618396 (1986-10-01), Shimoda et al.
Ghandhi, S.VLSI Fabrication Principles, John Wiley, 1983 pp. 86-90, 98-100.*
Sze, S.Physics of Semiconductor Devices, John Wiley, 1981, p. 33.*
IEEE Transactions on Electron Devices, vo. ED-31, No. 8, Aug., 1984, p. 1057, para. 4, 5; New York, US; S. Miyazawa, et al: “Dislocations as the origin of threshold voltage scatterings for GaAs MESFET on LEC-grown semi-insulating GaAs substrate”.
Journal of Crystal Growth, vol. 63, No. 2, Oct., 1983, pp. 415-418, Amsterdam, NL; R. Fornari, et al.: “Dislocation-free silicon-doped gallium arsenide grown by LEC procedure”.
Applied Physics Letters, vol. 44, No. 1, Jan. 1984, pp. 74-76 New York, US; A.T. Hunter, et al.: “Carbon in semi-insulating, liquid encapsulated Czochralski GaAs”.
Patent Abstracts of Japan, vol. 4, No. 173 (C-32) [655], 29th, Nov., 1980; & JP-A-55 113 669 (Sumitomo) 02-09-1080.

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