Method of fabricating single-crystal substrates of silicon carbide

A single-crystal substrate of silicon carbide comprising a single-crystal substrate member of a material other than .alpha.-SiC, and a single-crystal layer of .alpha.-SiC formed over the substrate member with a ground layer provided between the substrate member and the single-crystal layer, the ground layer comprising a single-crystal layer of nitride of AlN, GaN or Al.sub.x Ga.sub.1-x N (0<x<1) having a hexagonal crystal structure or a crystal layer of the same structure made of a mixture of SiC and at least one of the nitrides; and a method for fabricating the same.

BACKGROUND OF THE INVENTION 
1. Field of the Invention 
The present invention relates to a method of fabricating novel 
single-crystal substrates of .alpha.-silicon carbide (.alpha.-SiC). 
2. Description of the Prior Art 
Silicon carbide is a semiconductor material having wide forbidden band gaps 
(2.2 to 3.3 eV) and exhibiting very stable properties thermally, 
chemically and mechanically and has the feature of being highly resistant 
to damage due to radiation. The material has both conductivities of the 
p-type and n-type, whereas this is seldom the case with semiconductors 
having wide forbidden band gaps. Accordingly silicon carbide appears 
useful as a semiconductor material for light-emitting or photodetector 
devices for visible lights of short wavelengths, for electronic devices 
operable at high temperatures or with high electric power, for highly 
reliable semiconductor devices and for radiation-resistant devices. 
Further silicon carbide will provide electronic devices which are usable 
in an environment where difficulties are encountered with devices made of 
conventional semiconductor materials, thus greatly enlarging the range of 
applications for semiconductor devices. Other semiconductor materials such 
as semiconductor compounds of elements from Groups II and VI or from 
Groups III and V generally contain a heavy metal as the main component and 
therefore have the problems of pollution and resources, whereas silicon 
carbide is free of these problems and accordingly appears to be a 
promising electronic material. 
There are many crystal structures of silicon carbide (called "polytype") 
which are generally divided into the .alpha.-type and .beta.-type. Silicon 
carbide of the .beta.-type has a cubic crystal structure and is the 
smallest in forbidden band gaps (2.2 eV) of all forms of silicon carbide, 
while .alpha.-silicon carbide is of hexagonal or rhombohedral crystal 
structure and has relatively large forbidden band gaps of 2.9 to 3.3 eV. 
Because of the large forbidden band gaps, .alpha.-silicon carbide is 
expected to be a promising semiconductor material for optoelectronic 
devices, such as light-emitting devices and photodectectors, for use with 
blue and other visible lights of short wavelengths and near-ultraviolet 
rays. Although zinc sulfide (ZnS), zinc selenide (ZnSe), gallium nitride 
(GaN), etc. are materials which appear useful for light-emitting devices 
for blue or other visible lights of short wavelengths, the crystals of 
these materials usually available have conductivity of only one type, i.e. 
p-type or n-type, and difficulties are encountered in obtaining crystals 
having conductivity of both types. In contrast, .alpha.-silicon carbide 
readily provides a crystal of both p-type and n-type conductivities to 
afford a p-n junction. It is therefore expected that the material will 
realize light-emitting devices and photodetectors having outstanding 
optical characteristics or electrical characteristics. Further because of 
the exceedingly high stability in its thermal, chemical and mechanical 
properties, the material will be usable for wider applications than the 
other semiconductor materials. 
Despite these many advantages and capabilities, .alpha.-silicon carbide has 
not been placed into actual use because the technique still remains to be 
established for growing .alpha.-silicon carbide crystals as controlled in 
size, shape and quality with good reproducibility, as required for the 
commercial mass production of silicon carbide substrates of large area 
with high quality and high productivity. 
Conventional processes for preparing .alpha.-silicon carbide single-crystal 
substrates on a laboratory scale include the so-called sublimation method 
[also termed the "Lely method"; "Growth Phenomena in Silicon Carbide", W. 
F. Knippenberg: Phillips Research Reports, Vol. 18, No. 3, pp. 161-274 
(1963). (Chapter 8, "The Growth of SiC by Recrystallization and 
Sublimation", pp. 244-266)] wherein silicon carbide powder is sublimed in 
a graphite crucible at 2,200.degree. C. to 2,600.degree. C. and 
recrystallized to obtain a silicon carbide substrate, the so-called 
liquid-phase method ["Growth of Silicon Carbide from Solution" R. C. 
Marshall: Material Research Bulletin, Vol. 4, pp. S73-S84 (1969)] wherein 
silicon or a mixture of silicon with iron, cobalt, platinum or like 
impurities is melted in a graphite crucible to obtain a silicon carbide 
substrate, and the Acheson method "Growth Phenomena in Silicon Carbide" W. 
F. Knippenberg: Philips Research Reports, Vol. 18, No. 3, pp. 161-274 
(1963). (Chapter 2 "Preparative Procedures", pp. 171-179)] which is 
generally used for commercially producing abrasives and by which a silicon 
carbide substrate is obtained incidentally. Blue light-emitting diodes are 
fabricated using a substrate of .alpha.-silicon carbide obtained by such a 
crystal growth method, by forming on the substrate a single-crystal layer 
of .alpha.-silicon carbide by liquid-phase epitaxial growth (LPE) or 
chemical vapor deposition (CVD) to provide a p-n junction. 
However, although the sublimation method or the liquid-phase method affords 
a large number of small single crystals, it is difficult to prepare large 
single-crystal substrates of good quality by these methods since many 
crystal nuclei occur in the initial stage of crystal growth. The silicon 
carbide substrate incidentally obtained by the Acheson method still 
remains to be improved in purity and crystal quality for use as a 
semiconductor material, while large substrates, if available, are obtained 
only incidentally. Thus, the conventional crystal growth methods for 
preparing substrates of .alpha.-silicon carbide have difficulties in 
controlling the size, shape, quality, impurities, etc. and are not suited 
to the commercial production of single-crystal substrates of silicon 
carbide in view of productivity. Although light-emitting diodes are 
produced by preparing substrates of .alpha.-silicon carbide by the 
conventional method and subjecting the substrates to liquid-phase epitaxy 
or chemical vapor deposition as already mentioned, no progress has been 
made in commercial mass production since there is no method of 
industrially preparing .alpha.-type single-crystal substrates having a 
large area and a high quality. 
On the other hand, it is possible to epitaxially grow a single-crystal film 
of silicon carbide by CVD, LPE, molecular beam epitaxy (MBE) or like 
process on a single-crystal substrate of silicon (Si), sapphire (Al.sub.2 
O.sub.3), .beta.-silicon carbide (.beta.-SiC) or the like which differs 
from .alpha.-silicon carbide in component element or crystal structure, 
whereas the silicon carbide films obtained by this method are only of the 
.beta.-type having a cubic crystal structure. 
SUMMARY OF THE INVENTION 
In view of the foregoing problems, we have carried out intensive research 
and consequently prepared a single-crystal substrate of silicon carbide by 
forming on a single-crystal substrate of a material other than 
.alpha.-silicon carbide a single-crystal layer of a specific substance 
having the same hexagonal crystal structure as .alpha.-SiC, and thereafter 
growing a single-crystal film of SiC on the layer. We have found that the 
single-crystal layer of .alpha.-SiC can be efficiently formed which takes 
over the crystal structure of the underlying substance. 
Accordingly, the present invention provides a method of fabricating a 
single-crystal substrate of silicon carbide characterized by forming on a 
single-crystal substrate member of a material other than .alpha.-SiC a 
single-crystal layer of AlN, GaN or Al.sub.x Ga.sub.1-x N (0&lt;x&lt;1) having a 
hexagonal crystal structure or a crystal layer of the same structure made 
of a mixture of SiC and at least one of the nitrides as a ground layer, 
and growing a single crystal of .alpha.-SiC on the ground layer. 
The present invention further provides a single-crystal substrate of 
silicon carbide comprising a single-crystal substrate member of a material 
other than .alpha.-SiC, and a single-crystal layer of .alpha.-SiC formed 
over the substrate member with a ground layer provided between the 
substrate member and the single-crystal layer, the ground layer comprising 
a single-crystal layer of AlN, GaN or Al.sub.x Ga.sub.1-x N (1&lt;x&lt;1) having 
a hexagonal crystal structure or a crystal layer of the same structure 
made of a mixture of SiC and at least one of the nitrides. 
The present invention makes it possible to commercially fabricate a 
single-crystal substrate of .alpha.-silicon carbide having a high quality 
and a large area (e.g. 1 to 2 inches in diameter) with high productivity, 
opening the way for the actual use of these substrates as an 
optoelectronic device material for light-emitting devices, photodetectors, 
etc. for use with blue and other visible lights of short wavelengths and 
near-ultraviolet rays. It is further expected that the present 
single-crystal substrate of silicon carbide will find application in a 
wide variety of fields because of its high stability in thermal, chemical 
and mechanical properties.

DESCRIPTION OF THE PREFERRED EMBODIMENTS 
The term "single-crystal substrate member of a material other than 
.alpha.-SiC" as herein used means a single-crystal substrate of Si, 
Al.sub.2 O.sub.3, .beta.-SiC or the like. The single-crystal substrate of 
.beta.-SiC is advantageous for preparing single crystals of good quality 
since it is similar to .alpha.-SiC in lattice constant and coefficient of 
thermal expansion. Usually, the single-crystal substrate of .beta.-SiC may 
be in the form of a layer formed on some other base (for example, of Si 
single crystal). It is suitable that the single-crystal substrate member 
be about 1 to about 500 .mu.m in thickness. 
The ground layer of the present invention is in the form of a 
single-crystal layer of AlN, GaN or Al.sub.x Ga.sub.1-x N ((1&lt;x&lt;1) or a 
crystal layer of a mixture of SiC and at least one of these nitrides. The 
crystal layer of the mixture suitably contains at least 0.1 mole %, e.g. 
about 1 to about 10 mole %, of AlN or the like. For example, satisfactory 
results can be achieved when a small amount, such as about 1 mole % or 
about 2 mole %, of AlN or the like is present. 
It is thought that in the case of the crystal layer of a mixture of SiC and 
AlN or the like, Al, Ga and N atoms different from SiC are present in the 
form of a compound Al--N, Ga--N or Al.sub.x Ga.sub.1-x --N, forming a 
crystal with SiC. However, such different atoms may be present in the 
crystal lattice of SiC as introduced therein locally and randomly as 
so-called dopants. Especially when the amounts of such atoms are small 
relative to SiC, these atoms will be present in the form of dopants. 
The ground layer is formed most suitably by the CVD process. Examples of 
suitable Al sources for this process are the combination of metallic 
aluminum and an etching gas (e.g. hydrogen chloride gas) therefor, 
aluminum chloride, trimethylaluminum, triethylaluminum and the like. 
Examples of suitable Ga sources are the combination of metallic gallium 
and an ethching gas therefor, gallium chloride, trimethylgallium, 
triethylgallium and the like. Examples of suitable N sources are nitrogen, 
ammonia and the like. For forming the mixture crystal layer, suitable Si 
sources are SiH.sub.4, SiCl.sub.4, SiH.sub.2 Cl.sub.2, (CH.sub.3).sub.3 
SiCl, (CH.sub.3).sub.2 SiCl.sub.2 and the like, and suitable C sources are 
CCl.sub.4, CH.sub.4, C.sub.2 H.sub.6, C.sub.3 H.sub.8. Such source gases 
are supplied to the reaction chamber for CVD usually as entrained in a 
carrier gas such as hydrogen gas. The rate of crystal growth of the ground 
layer and the ratio of constituent atoms of the crystal can be controlled 
as mentioned above by adjusting the flow rates of the source gases by mass 
flow controller or the like. The ratio of the source gases to be supplied 
in combination, e.g. Al--N source ratio, Ga--N source ratio or Al+Ga--N 
source ratio, may be such that an excess of one is used relative to the 
other. Although the supply ratio is preferably so determined that Al and 
N, for example, will be contained in the resulting crystal in the ratio of 
1:1, the ratio need not always be set accurately; an excess of one element 
may be present in the crystal. 
The CVD apparatus to be used can be one already known in the art. It is 
suitable that the substrate member be maintained at a temperature usually 
of 1000.degree. to 1800.degree. C., preferably 1200.degree. to 
1600.degree. C. for CVD. The supplied gas pressure within the CVD chamber 
may be atmospheric or a low pressure of about 0.01 to about 100 torr. 
While it is suitable to form the ground layer to a thickness of at least 
0.1 .mu.m, especially about 0.1 to about 5 .mu.m, the thickness may be 
larger. 
The ground layer can be formed also by various processes for growing single 
crystals other than the CVD process, such as liquid-phase method, 
sublimation method, vacuum evaporation, MBE process, sputtering, etc. When 
the ground layer is formed, for example, by the liquid-phase method, 
metallic aluminum or metallic gallium and Si.sub.3 N.sub.4 are used in 
addition to Si material at a growth temperature of 1500.degree. to 
1900.degree. C. When the sublimation method is resorted to, metallic 
aluminum or metallic gallium and Si.sub.3 N.sub.4 are admixed with SiC 
material. 
A single crystal of SiC is grown on the ground layer thus obtained, whereby 
a single crystal of .alpha.-SiC is formed. Like the ground layer, the SiC 
single crystal is grown suitably by the CVD process, while the 
above-mentioned other processes may be used. While it is suitable to grow 
the single crystal to a thickness of about 1 to about 10 .mu.m, the 
thickness can be larger. 
The SiC single crystal grown on the ground layer is of the .alpha.-type 
presumably for the following reason. 
.alpha.-SiC has various crystal structures which slightly differ from one 
another and typical of which are 2H form, 4H form and 6H form. AlN, GaN 
and Al.sub.x Ga.sub.1-x N single crystals have exactly the same hexagonal 
crystal structure as .alpha.-SiC of 2H form. The lattice constants and 
coefficients of thermal expansion of these single crystals are 3.10 .ANG. 
and 4.15.times.10.sup.-6 K.sup.-1 for AlN, 3.19 .ANG. and 
5.59.times.10.sup.-6 K.sup.-1 for GaN, and intermediate values between 
these values of AlN and GaN for Al.sub.x Ga.sub.1-x N according to the 
ratio x. All of these values are approximate to the corresponding values 
of .alpha.-SiC, i.e. 3.08 .ANG. and 4.2.times.10.sup.-6 K.sup.-1. Further 
the crystal of a mixture of SiC with AlN, GaN or Al.sub.x Ga.sub.1-x N 
also has the same hexagonal crystal structure as .alpha.-SiC of 2H form 
and is approximate to .alpha.-SiC in lattice constant and coefficient of 
thermal expansion. Accordingly, the SiC film grown is an .alpha.-crystal 
film taking over the crystal structure of the ground substance. From this 
viewpoint, use of AlN or the mixture of SiC and AlN is especially 
advantageous in obtaining a single crystal of .alpha.-SiC having good 
crystal quality since the material is very close to .alpha.-SiC in lattice 
constant and coefficient of thermal expansion. 
The single-crystal substrate obtained is a novel one which itself has a 
specific layered structure. Moreover, the large band gaps of the ground 
layer serve to electrically separate the .alpha.-SiC single crystal from 
the substrate member. (The ground layer acts also as an insulating film 
since AlN, for example, has band gaps of 6.2 eV, or the mixture crystal of 
AlN and SiC has band gaps of at least 3.3 eV.) These features render the 
.alpha.-SiC single crystal usable for devices with a great advantage. 
The present invention will be described in greater detail with reference to 
the following examples in which crystals were grown by the CVD process on 
substrate members of .beta.-SiC single crystal. In Example 1, an AlN 
single-crystal layer was grown first on the substrate member, and an 
.alpha.-SiC single-crystal film was then grown on the layer. In Examples 2 
and 3, a crystal layer of a mixture of AlN and SiC was grown first on the 
substrate member, and an .alpha.-SiC single-crystal film was then grown on 
the layer. 
The substrate members of .beta.-SiC single crystal were prepared by the 
successive two-step CVD process already proposed by the present applicant 
for growing .beta.-SiC single crystals (Unexamined Japanese Patent 
Publication SHO No. 59-203799). Stated more specifically, the substrate 
member was prepared by uniformly forming a thin polycrystalline SiC layer, 
about 20 nm in thickness, on an Si single-crystal base at a temperature of 
about 1050.degree. C. by CVD using SiH.sub.4 and C.sub.3 H.sub.8 as source 
gases, growing an SiC single-crystal film, about 20 .mu.m in thickness, on 
the layer at a temperature of about 1350.degree. C. by CVD using SiH.sub.4 
and C.sub.3 H.sub.8 and dissolving away the Si of the base with an acid 
mixture of HF and HNO.sub.3. The substrate members of .beta.-SiC single 
crystal used were 1 cm.times.1 cm in size. 
The accompanying drawings are diagrams showing the CVD growth apparatus 
used in Examples 1 to 3. The apparatus of FIG. 1 was used for Examples 1 
and 2, and the apparatus of FIG. 2 for Example 3. With reference to FIGS. 
1 and 2, a water-cooled double-walled horizontal quartz reaction tube 1 
has in its interior a graphite susceptor 2 supported by a graphite bar 3. 
A high-frequency current is passed through a working coil 4 wound around 
the body of the reaction tube 1 to heat the graphite susceptor 2 by 
induction. The apparatus of FIG. 2 has another graphite susceptor 17 as 
supported by a pedestal 16. The susceptor 17 is heated by induction with a 
high-frequency current passed through a working coil 19. One end of the 
reaction tube 1 has a branch pipe 5 serving as a gas inlet. Cooling water 
is passed through the outer quartz tube of the reaction tube 1 via branch 
pipes 6 and 7. The other end of the reaction tube 1 is sealed off by a 
stainless steel flange 8, retaining plate 9, bolts 10, nuts 11 and an 
O-ring 12. The flange 8 has a branch pipe 13 serving as a gas outlet. The 
graphite bar 3 is fixed to a holder 14. A substrate member of .beta.-SiC 
single crystal is placed on the susceptor 2. In FIG. 2, metallic aluminum 
18 is placed on the susceptor 17. The source gases and carrier gas 
(H.sub.2) have their flow rates controlled by mass flow controllers 20. 
Indicated at A to F are gas cylinders; A for H.sub.2, B for SiH.sub.4, C 
for C.sub.3 H.sub.8, D for (CH.sub.3).sub.3 Al, E for N.sub.2, and F for 
HCl. 
EXAMPLE 1 
The apparatus of FIG. 1 was used. 
The air within the reaction tube 1 was replaced by hydrogen gas, and a 
high-frequency current was passed through the working coil 4 to heat the 
susceptor 2 and maintain the substrate member 15 of .beta.-SiC at a 
temperature of about 1300.degree. C. 
Nitrogen (N.sub.2) gas supplied at a flow rate of 0.75 liter/min and 
trimethylaluminum ((CH.sub.3).sub.3 Al) gas at 0.6 c.c./min were admixed 
with hydrogen carrier gas at a flow rate of 1.5 liters/min, and the 
mixture was fed to the reaction tube 1 through the branch pipe 5 to grow 
AlN for 2 hours, whereby an AlN single-crystal layer was formed with a 
thickness of about 0.6 .mu.m. Subsequently, with the supply of the 
hydrogen carrier gas and the heating of the substrate member continued but 
with the supply of the nitrogen gas and trimethylaluminum gas 
discontinued, propane (C.sub.3 H.sub.8) and monosilane (SiH.sub.4) were 
fed to the reaction tube 1 via the branch pipe 5 at flow rates of 0.045 
c.c./min and 0.045 c.c./min, respectively, to grow a crystal for 1 hour. 
Consequently, an SiC film of about 1 .mu.m in thickness was formed over 
the AlN layer on the .beta.-SiC substrate member. 
The crystal structure of the SiC film grown was analyzed by reflection 
high-energy electron diffraction (RHEED) using an electron beam at an 
accelerating voltage of 50 kV. The analysis indicated spots corresponding 
to the reciprocal lattice points of 2H-form crystal. Thus, the crystal 
obtained was identified as an .alpha.-SiC single crystal of 2H form. 
EXAMPLE 2 
The apparatus of FIG. 1 was used. 
The air within the reaction tube 1 was replaced by hydrogen gas, and a 
high-frequency current was passed through the working coil 4 to heat the 
susceptor 2 and maintain the substrate member 15 of .beta.-SiC at a 
temperature of about 1400.degree. C. 
Propane, monosilane, nitrogen and trimethylaluminum supplied as source 
gases at flow rates of 0.25 c.c./min, 0.75 c.c./min, 0.35 c.c./min and 
0.60 c.c./min, respectively, were admixed with hydrogen carrier gas at a 
flow rate of 3 liters/min, and the gas mixture was fed to the reaction 
tube 1 via the branch pipe 5 to grow a crystal for 30 minutes, whereby a 
crystal layer of mixture of AlN and SiC was obtained with a thickness of 
about 3 .mu.m. 
Reflection high-energy electron diffraction (RHEED) analysis revealed that 
the layer had the crystal structure of 2H form. The layer was further 
subjected to Auger electron spectroscopy analysis in a high vacuum of 
1.times.10.sup.-9 torr using electron beam at an accelerating voltage of 5 
kV after removing an oxide film or the like from the surface of the Ar ion 
sputtering. The relative intensity ratio between the peaks (Si.sub.LVV, 
Si.sub.KLL, C.sub.KLL, N.sub.KLL, Al.sub.KLL) indicated that the layer was 
a mixture crystal of about 1% AlN and about 99% of SiC. 
Subsequently, SiC was grown on the layer by continuing the supply of 
hydrogen carrier gas, propane gas and monosilane gas and heating of the 
substrate member, with the supply of nitrogen gas and trimethylaluminum 
gas discontinued. In 30 minutes, a film of about 3 .mu.m in thickness was 
obtained on the crystal layer of mixture of AlN and SiC on the .beta.-SiC 
substrate member. Reflection high-energy diffraction analysis revealed 
that the layer was an .beta.-SiC single crystal of 2H form. 
EXAMPLE 3 
The apparatus of FIG. 2 was used. 
The air within the reaction tube 1 was replaced by hydrogen gas, and a 
high-frequency current was passed through the working coil 4 to heat the 
susceptor 2 and maintain the substrate member 15 of .beta.-SiC at a 
temperature of about 1500.degree. C. A high-frequency current was then 
passed through the working coil 15 to heat the susceptor 17 to a 
temperature of about 800.degree. C. and melt aluminum 18. 
Propane (C.sub.3 H.sub.8), monosilane (SiH.sub.4) and nitrogen supplied as 
source gases at flow rates of 0.25 c.c./min, 0.75 c.c./min and 0.2 
liter/min, respectively, and hydrogen chloride (HCl) supplied as an 
etching gas for the molten aluminum at a flow rate of 5 c.c./min were 
admixed with hydrogen carrier gas at a flow rate of 1 liter/min, and the 
mixture was supplied to the reaction tube 1 through the branch pipe 5. The 
molten aluminum was etched by the hydrogen chloride gas, released into the 
carrier gas and transported onto the .beta.-SiC substrate member. 
Consequently, a crystal layer of mixture of AlN and SiC was formed in 30 
minutes with a thickness of about 2 .mu.m. Reflection high-energy electron 
diffraction analysis revealed that the layer had the crystal structure of 
2H form. Auger analysis showed that the crystal was composed of about 1% 
of AlN and about 99% of SiC. 
Subsequently, a crystal was grown by continuing the supply of hydrogen 
carrier gas, propane gas and monosilane gas and the heating of the 
substrate member, with the supply of nitrogen gas and hydrogen chloride 
gas discontinued. Consequently, an SiC film of about 2 .mu.m in thickness 
was formed in 30 minutes on the crystal layer of AlN-SiC mixture over the 
.beta.-SiC substrate member. Reflection high-energy electron diffraction 
analysis revealed that the SiC film grown was an .alpha.-SiC single 
crystal of 2H form.