Light emitting semiconductor device using gallium nitride group compound

Abstract

A semiconductor device having an n-type layer of gallium nitride that is doped with silicon and has a resistively ranging from 3×10−1 Ωcm to 8×10−3 Ωcm or a carrier concentration ranging from 6×1016/cm3 to 3×1018/cm3.

Description

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a light-emitting semiconductor device using gallium nitride group compound which emits a blue light.

2. Description of the Prior Art

It is known that GaN compound semiconductor can be made into a light-emitting semiconductor device, such as a light-emitting diode (LED), which emits a blue light. The GaN compound semiconductor attracts attention because of its high light-emitting efficiency resulting from direct transition and of its ability to emit a blue light which is one of three primary colors.

The light-emitting diode manufactured from the GaN compound semiconductor is composed of an n-layer and an i-layer grown thereon. The n-layer of the GaN compound semiconductor with n-type conduction is directly grown on a surface of a sapphire substrate or grown on a buffer layer of aluminum nitride formed on the substrate. The i-layer of insulating (i-type) GaN compound semiconductor doped with p-type impurities is grown on the n-layer. (See Japanese Patent Laid-open Nos. 119196/1987 and 188977/1988.) The light-emitting diode of this structure has room for improvement in luminous intensity. In addition, it comprises no p-n junction but it is made by joining the i-layer and n-layer.

An electric property of the GaN compound semiconductor shows inherently n-type conduction even though it is not deliberately doped with n-type impurities, and unlike silicon and similar semiconductors, when it is doped with zinc of p-type impurities, the electric property shows not p-type conduction but insulation. Moreover, the production of n-type GaN involves many difficulties in controlling conductivity.

SUMMARY OF THE INVENTION

It is the first object of the present invention to improve a luminous efficiency of a GaN group light-emitting diode.

It is the second object of the present invention to provide a new layer structure which improves a luminous efficiency of a GaN group light-emitting diode.

It is the third object of the present invention to provide a technology for production of n-type GaN group compound semiconductor in which conductivity is easily controlled.

After experience in the manufacture of the above-mentioned GaN light-emitting diode, the present inventors established a technology for a vapor phase epitaxy of the GaN group semiconductor with organometal compound. This technology enables a production of a gas-phase grown GaN layer of high purity. In other words, this technology provides n-type GaN with high resistivity without doping with impurities, unlike the conventional technology which provides n-type GaN with low resistivity when no doping is performed.

The First Feature of the Invention;

The first feature of the present invention resides in a light-emitting semiconductor device composed of an n-layer of n-type gallium nitride group compound semiconductor (Al x Ga 1−x N; inclusive of x=0) and an i-layer of insulating (i-type) gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) doped with p-type impurities, in which the n-layer is of double-layer structure including an n-layer of low carrier concentration and an n + -layer of high carrier concentration, the former being adjacent to the i-layer.

According to the present invention, the n-layer of low carrier concentration should preferably have a carrier concentration of 1×10 14 /cm 3 to 1×10 17 /cm 3 and have a thickness of 0.5 to 2 μm. In the case where the carrier concentration is higher than 1×10 17 /cm 3 , the luminous intensity of the light-emitting diode decreases. In the case where the carrier concentration is lower than 1×10 14 /cm 3 , since the series resistance of the light-emitting diode increases, an amount of heat generated in the n-layer increases when a constant current is supplied to it. In the case where the layer thickness is greater than 2 μm, since the series resistance of the light-emitting diode increases, the amount of heat generated in the n-layer increases when the constant current is supplied to it. In the case where the layer thickness is smaller than 0.5 μm, the luminous intensity of the light-emitting diode decreases.

In addition, the n + -layer of high carrier concentration should preferably contain a carrier concentration of 1×10 17 /cm 3 to 1×10 19 /cm 3 and have a thickness of 2-10 μm. In the case where the carrier concentration is higher than 1×10 19 /cm 3 , the n + -layer is poor in crystallinity. In case that the carrier concentration is lower than 1×10 17 /cm 3 , since the series resistance of the light-emitting diode increases, an amount of heat generated in the n + -layer increases when a constant current is supplied to it. In the case where the layer thickness is greater than 10 μm, the substrate of the light-emitting diode warps. In case that the layer thickness is smaller than 2 μm, since the series resistance of the light-emitting diode increases, the amount of heat generated in the n + -layer increases when the constant current is supplied to it.

In the first feature of the present invention, it is possible to increase an intensity of blue light emitted from the light-emitting diode by making the n-layer in double-layer structure including an n-layer of low carrier concentration and an n + -layer of high carrier concentration, the former being adjacent to the i-layer. In other words, the n-layer as a whole has a low electric resistance owing to the n + -layer of high carrier concentration, and hence the light-emitting diode has low series resistance and generates less heat when a constant current is supplied to it. The n-layer adjacent to the i-layer has a lower carrier concentration or higher purity so that it contains a smaller amount of impurity atoms which are deleterious to the emission of blue light from the light-emission region (i-layer and its vicinity). Due to the above-mentioned functions, the light-emitting diode of the present invention emits a blue light of higher intensity.

The Second Feature of the Invention

The second feature of the present invention resides in a light-emitting semiconductor device composed of an n-layer of n-type gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) and an i-layer of i-type gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) doped with p-type impurities, in which the i-layer is of double-layer structure including an iL-layer containing p-type impurities in comparatively low concentration and an i H -layer containing p-type impurities in comparatively high concentration, the former being adjacent to the n-layer.

According to the present invention, the i L -layer of low impurity concentration should preferably contain the impurities in concentration of 1×10 16 /cm 3 to 5×10 19 /cm 3 and have a thickness of 0.01 to 1 μm. In the case where the impurity concentration is higher than 5×10 19 /cm 3 , since the series resistance of the light-emitting diode increases, an initial voltage to start emitting light increases. In the case where the impurity concentration is lower than 1×10 16 /cm 3 , the semiconductor of the i L -layer shows n-type conduction. In the case where the layer thickness is greater than 1 μm, since the series resistance of the light-emitting diode increases, the initial voltage to start emitting light at increases. In the case where the layer thickness is smaller than 0.01 μm, the light-emitting diode has the same structure as that of the conventional one.

In addition, the iH-layer of high impurity concentration should preferably contain the impurities in concentration of 1×10 19 /cm 3 to 5×10 20 /cm 3 and have a thickness of 0.02 to 0.3 μm. In the case where the impurity concentration is higher than 5×10 2 /cm 3 , the semiconductor of the i H -layer is poor in crystallinity. In the case where the impurity concentration is lower than 1×10 19 /cm 3 , the luminous intensity of the light-emitting diode decreases. In case that the layer thickness is greater than 0.3 μm, since the series resistance of the light-emitting diode increases, an initial voltage to start emitting light at increases. In case that the layer thickness is smaller than 0.02 μm, the i-layer is subject to breakage.

In the second feature of the present invention, it is possible to increase an intensity of blue light emitted from the light-emitting diode by making the i-layer in double-layer structure including an i L -layer containing p-type impurities in comparatively low concentration and an i H -layer containing p-type impurities in comparatively high concentration, the former being adjacent to the n-layer. In other words, this structure (in which the i-layer adjacent to the n-layer is the i L -layer of low impurity concentration) enables electrons to be injected from the n-layer into the i H -layer of high impurity concentration without being trapped in the i L -layer and its vicinity. Therefore, this structure enables electrons to pass through the i L -layer of low impurity concentration, which is poor in luminous efficacy, adjacent to the n-layer, and to reach the i H -layer of high impurity concentration in which electrons emit light with a high efficiency.

The Third Feature of the Invention

The third feature of the present invention resides in a light-emitting semiconductor device composed of an n-layer of n-type gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) and an i-layer of i-type gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) doped with p-type impurities, in which the n-layer is of double-layer structure including an n-layer of low carrier concentration and an n + -layer of high carrier concentration, the former being adjacent to the i-layer, and the i-layer is of double-layer structure including an i L -layer containing p-type impurities in comparatively low concentration and an i H -layer containing p-type impurities in comparatively high concentration, the former being adjacent to the n-layer.

The third feature of the present invention is a combination of the first feature (the n-layer of double layer structure) and the second feature (the i-layer of double layer structure). Therefore, the n-layer of low carrier concentration, the n + -layer of high carrier concentration, the i L -layer of low impurity concentration, and the i H -layer of high impurity concentration should correspond to the respective layers as the first and second features. The carrier concentration and layer thickness are defined in the same manner as in the first and second features.

In the third feature of the present invention, it is possible to increase an intensity of blue light from the light-emitting diode by making the n-layer in double-layer structure including an n-layer of low carrier concentration and an n + -layer of high carrier concentration, the former being adjacent to the i-layer, and also by making the i-layer in double-layer structure including an i L -layer containing p-type impurities in comparatively low concentration and an i H -layer containing p-type impurities in comparatively high concentration, the former being adjacent to the n-layer.

In other words, the n-layer as a whole has a low electric resistance owing to the n + -layer of high carrier concentration, which makes it possible to apply an effective voltage to the junction between the i L -layer and n-layer of low carrier concentration. Having a low carrier concentration. the n-layer adjacent to the i L -layer does not permit non-light-emitting impurity atoms to diffuse into the i L -layer. In addition, this structure (in which the i-layer adjacent to the n-layer is the i L -layer of low impurity concentration) permits electrons to be injected from the n-layer into the i H -layer of high impurity concentration without being trapped in the i L -layer. Therefore, this structure permits electrons to pass through the i L -layer of low impurity concentration, which is poor in luminous efficacy, adjacent to the n-layer, and to reach the i H -layer of high impurity concentration in which electrons emit light with a high efficiency.

For this reason, the light-emitting diode of the present invention has a much higher luminous efficacy than the one having the conventional simple i-n junction.

The Fourth Feature of the Invention

The fourth feature of the present invention resides in a method of producing an n-type gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) an organometallic compound by vapor phase epitaxy. This method comprises a step of feeding a silicon-containing gas and other raw material gases together at a proper mixing ratio so that the conductivity of the compound semiconductor is desirably controlled. The mixing ratio is adjusted such that silicon enters the layer of gallium nitride compound semiconductor grown by vapor phase epitaxy and functions as the donor therein. Thus it is possible to vary the conductivity of the n-type layer by adjusting the mixing ratio.

The Fifth Feature of the Invention

The fifth feature of the present invention resides in a method for producing a light-emitting semiconductor device. The method comprises two steps. The first step involves growing an n + -layer of high carrier concentration (which is an n-type gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) having a comparatively high conductivity) by vapor phase epitaxy an organometallic compound. The vapor phase epitaxy is accomplished on a sapphire substrate having a buffer layer of aluminum nitride by feeding a silicon-containing gas and other raw material gases together at a proper mixing ratio. The second step involves growing an n-layer of low carrier concentration (which is an n-type gallium nitride compound semiconductor (Al x Ga 1−x N; inclusive of x=0) having a comparatively low conductivity) by vapor phase epitaxy from an organometallic compound. The vapor phase epitaxy is accomplished on the n + -layer formed by the first step by feeding raw material gases excluding the silicon-containing gas. The n-layer of double-layer structure can be produced by properly controlling the mixing ratio of a silicon-containing gas and other raw material gases.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a diagram showing a structure of a light-emitting diode shown as Example 1 of the present invention.

FIGS. 2 to 7 are sectional views illustrating processes for producing a light-emitting diode shown as to Example 1 of the present invention.

FIG. 8 is a diagram showing relationship between a carrier concentration of an n-layer of low carrier concentration and intensity or wavelength of emitted light with respect to a light-emitting diode shown as Example 1 of the present invention.

FIG. 9 is a diagram showing a structure of a light-emitting diode shown as Example 2 of the present invention.

FIGS. 10 to 15 are sectional views illustrating processes for producing a light-emitting diode shown as Example 2 of the present invention.

FIG. 16 is a diagram showing relationship between an impurity concentration of an i H -layer of high impurity concentration and intensity or wavelength of emitted light with respect to a light-emitting diode shown as Example 2 of the present invention.

FIG. 17 is a diagram showing a structure of a light emitting diode shown as Example 3 of the present invention.

FIGS. 18 to 23 are sectional views illustrating processes for producing a light-emitting diode shown as Example 3 of the present invention.

FIG. 24 is a diagram showing relationship between a carrier concentration of an n-layer of low carrier concentration and intensity or wavelength of emitted light with respect to a light-emitting diode shown as Example 3 of the present invention.

FIG. 25 is a diagram showing relationship between an impurity concentration of an i H -layer of high impurity concentration and intensity or wavelength of emitted light with respect to a light-emitting diode shown as Example 3 of the present invention.

FIG. 26 is a diagram showing the relationship between a flow rate of silane gas and electrical properties of an n-layer formed by vapor phase epitaxy in a process shown as Example 4 of the present invention.

DETAILED DESCRIPTION OF THE INVENTION

The invention will be described in more detail with reference to the following examples.

Example 1

In FIG. 1 there is shown a light-emitting diode 10 which has a sapphire substrate 1 on which is formed a buffer layer of 500 Å thick AlN. As is know in the art, the AlN assumes a wurtzite-type structure. On the buffer layer 2 are consecutively formed an n + -layer 3 of high carrier concentration of 2.2 μm thick GaN and an n-layer 4 of low carrier concentration of 1.5 μm thick GaN. An i-(insulating) layer 6 of 0.2 μm thick GaN is formed on the n-layer 4 . Aluminum electrodes 7 and 8 are connected to the i-layer 6 and n + -layer 3 , respectively.

This light-emitting diode 10 was produced by metal organic vapor phase epitaxy in the following manner. (This process is referred to as MOVPE hereinafter.)

The gases employed in this process are NH 3 , H 2 (as carrier gas), trimethyl gallium (Ga(CH 3 ) 3 ) (TMG hereinafter), trimethyl aluminum (Al(CH 3 ) 3 ) (TMA hereinafter), silane (SiH 4 ), and diethyl zinc (DEZ hereinafter).

The sapphire substrate 1 of single crystal, with its principal crystal plane (a-surface {11{overscore (2)}0}) cleaned by solvent washing and heat treatment, was set on the susceptor placed in a reaction chamber of an MOVPE apparatus.

The sapphire substrate 1 underwent vapor phase etching at 1100° C. with H 2 flowing through the reaction chamber at a flow rate of 2 l/min under normal pressure.

On the sapphire substrate 1 was formed the AlN buffer layer 2 (about 500 Å thick) at 400° C. by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, and TMA at a flow rate of 1.8×10 −5 mol/min.

On the buffer layer 2 was formed the n + -layer 3 of high carrier concentration (1.5×10 18 /cm 3 ) of 2.2 μm thick GaN by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG at a flow rate of 1.7×10 −4 mol/min, and silane (diluted to 0.86 ppm with H 2 ) at a flow rate of 200 ml/min, with the sapphire substrate 1 kept at 1150° C.

On the n + -layer 3 was formed the n-layer 4 of low carrier concentration (1×10 15 /cm 3 ) of 1.5 μm thick GaN by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, and TMG at a flow rate of 1.7×10 −4 mol/min, with the sapphire substrate 1 kept at 1150° C.

On the n-layer 4 was formed the i-layer 6 of 0.2 μm thick GaN by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG at a flow rate of 1.7×10 −4 mol/min, and DEZ at a flow rate of 1.5×10 −4 mol/min, with the sapphire substrate 1 kept at 900° C.

Thus there was obtained the multi-layer structure as shown in FIG. 2 .

On the i-layer 6 was formed a 2000 Å thick SiO 2 layer 11 by sputtering as shown in FIG. 3 . On the SiO 2 layer 11 was formed a photoresist layer 12 which subsequently underwent a photolithographic processing to make a pattern corresponding to a figure of the electrode connected to the n + -layer 3 .

The exposed part (not covered by the photoresist layer 12 ) of the SiO 2 layer 11 underwent etching with hydrofluoric acid for its removal, as shown in FIG. 4 .

The exposed part (not covered by the photoresist layer 12 and the SiO 2 layer 11 ) of the i-layer 6 underwent dry etching with CCl 2 F 2 gas at a flow rate of 10 cc/min and a high-frequency electric power of 0.44 W/cm 2 in a vacuum of 0.04 Torr and subsequently underwent dry etching with argon. The dry etching removed not only the exposed part of the i-layer 6 but also the n-layer 4 and the upper part of the n + -layer 3 which are underneath the exposed part of the i-layer 6 , as shown in FIG. 5 .

The SiO 2 layer 11 remaining on the i-layer 6 was removed with hydrofluoric acid as shown in FIG. 6 .

On the entire surface of the sample was formed an Al layer 13 by vapor deposition as shown in FIG. 7 . On the Al layer 13 was formed a photoresist layer 14 which subsequently underwent the photolithographic processing to make a pattern corresponding to a figure of the electrodes connected to the n + -layer 3 and the i-layer 6 , respectively.

The exposed part (not covered by the photoresist layer 14 ) of the Al layer 13 underwent etching with nitric acid as shown in FIG. 7 . The photoresist 14 was removed with acetone. Thus there were formed the electrode 8 for the n + -layer 3 and the electrode 7 for the i-layer 6 .

Such an above-mentioned process could make a gallium nitride light-emitting element of MIS (metal-insulator-semiconductor) structure as shown in FIG. 1 .

The thus obtained light-emitting diode 10 was found to have a luminous intensity of 0.2 mcd. This value is 4 times higher than that of the conventional light-emitting diode which is composed simply of an i-layer with impurity concentration of 2×10 20 /cm 3 and a 4 μm thick n-layer with carrier concentration of 5×10 17 /cm 3 .

In addition, the inspection of the luminescent surface revealed that the number of luminescent points is much greater than that of the conventional light-emitting diode.

Several samples were prepared in the same manner as mentioned above except that the carrier concentration in the n-layer of low carrier concentration was varied, and they were tested for luminous intensity and emission spectrum. The results are shown in FIG. 8 . It is noted that the luminous intensity decreases and the emission spectrum shifts to the red side according as the carrier concentration increases. This effect is estimated to be caused by atoms of silicon as doping atoms that diffuse or mix into the i-layer 6 as impurity atoms.

Example 2

In FIG. 9 there is shown a light-emitting diode 10 which has a sapphire substrate 1 on which is formed a 500 Å thick AlN buffer layer 2 . On the buffer layer 2 are consecutively formed a 4 μm thick GaN n-layer 3 with carrier concentration of 5×10 17 /cm 3 , an i L -layer 5 of low impurity concentration of 5×10 19 /cm 3 of Zn, and an i H -layer 6 of high impurity concentration (2×10 20 /cm 3 of Zn). To the i H -layer 6 and n-layer 3 are connected aluminum electrodes 7 and 8 , respectively.

This light-emitting diode 10 was produced by the MOVPE.

The gases employed in this process are NH 3 , H 2 (as carrier gas), trimethyl gallium TMG, trimethyl aluminum TMA, and diethyl zinc DEZ.

The sapphire substrate 1 of single crystal, with its principal crystal plane (c-surface {0001}) cleaned by solvent washing and heat treatment, was set on the susceptor placed in the reaction chamber of the MOVPE apparatus.

The sapphire substrate 1 underwent vapor phase etching at 1100° C. with H 2 flowing through the reaction chamber at a flow rate of 2 l/min under normal pressure.

On the sapphire substrate 1 was formed the AlN buffer layer 2 (about 500 Å thick) at 400° C. by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, and TMA at a flow rate of 1.8×10 −5 mol/min.

On the buffer layer 2 was formed the 4 μm thick GaN n-layer 3 with carrier concentration of 1.5×10 17 /cm 3 by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, and TMG at a flow rate of 1.7×10 −4 mol/min with stopping the feeding of TMA, with the sapphire substrate 1 kept at 1150° C.

On the n-layer 3 was formed the 0.2 μm thick GaN i L -layer 5 of low impurity concentration (5×10 19 /cm 3 of Zn) by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG at a flow rate of 1.7×10 −4 mol/min, and DEZ at a flow rate of 1.5×10 −4 mol/min, with the sapphire substrate 1 kept at 1000° C.

On the i L -layer 5 was formed the 0.2 μm thick GaN i H -layer 6 of high impurity concentration (2×10 20 /cm 3 of Zn) by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG at a flow rate of 1.7×10 −4 mol/min, and DEZ at a flow rate of 1.5×10−4 mol/min, with the sapphire substrate 1 kept at 900° C.

Thus there was obtained the multi-layer structure as shown in FIG. 10 .

On the i H -layer 6 was formed the 2000 Å thick SiO 2 layer 11 by sputtering as shown in FIG. 11 . On the SiO 2 layer 11 was formed a photoresist layer 12 which subsequently underwent photolithographic processing to make a pattern corresponding to the figure of the electrode connected to the n-layer 3 .

The exposed part (not covered by the photoresist layer 12 ) of the SiO 2 layer 11 underwent etching with hydrofluoric acid for its removal, as shown in FIG. 12 .

The exposed part (not covered by the photoresist layer 12 and the SiO 2 layer 11 ) of the i H -layer 6 underwent dry etching with CCl 2 F 2 gas at a flow rate of 10 cc/min and a high-frequency electric power of 0.44 W/cm2 in a vacuum of 0.04 Torr and subsequently underwent dry etching with argon. The dry etching removed not only the exposed part of the i H -layer 6 but also the i L -layer 5 and the upper part of the n-layer 3 which are underneath the exposed part of the i H -layer 6 , as shown in FIG. 13 .

The SiO 2 layer 11 remaining on the i H -layer 6 was removed with hydrofluoric acid as shown in FIG. 14 .

On the entire surface of the sample was formed an Al layer 13 by vapor deposition as shown in FIG. 15 . On the Al layer 13 was formed the photoresist layer 14 which subsequently underwent the photolithographic processing to make a pattern corresponding to the figure of the electrodes connected to the n-layer 3 and the i H layer 6 , respectively.

The exposed part (not covered by the photoresist layer 14 ) of the Al layer 13 underwent etching with nitric acid as shown in FIG. 15 . The photoresist 14 was removed with acetone. Thus there were formed the electrode 8 for the n-layer 3 and the electrode 7 for the i H -layer 6 .

Such an above-mentioned process could make a gallium nitride light-emitting element of MIS structure as shown in FIG. 9 .

The thus obtained light-emitting diode 10 was found to have a luminous intensity of 0.2 mcd. This value is 4 times higher than that of the conventional light-emitting diode which is composed simply of a 0.2 μm thick i-layer with impurity concentration of 2×10 20 /cm 3 and a 4 μm thick n-layer with carrier concentration of 5×10 17 /cm 3 .

In addition, inspection of the luminescent surface revealed that the number of luminescent points is much greater than that of the conventional light-emitting diode.

Several samples were prepared in the same manner as mentioned above except that the impurity concentration in the i H -layer 6 of high impurity concentration was varied, and they were tested for luminous intensity and emission spectrum. The results are shown in FIG. 16 . It is noted that the luminous intensity has a peak value and the emission spectrum shifts to a longer wavelength side when the impurity concentration increases.

Example 3

In FIG. 17 there is shown a light-emitting diode 10 which has a sapphire substrate 1 on which is formed a 500 Å thick AlN buffer layer 2 . On the buffer layer 2 are consecutively formed a 2.2 μm thick GaN n + -layer 3 of high carrier concentration (1.5×10 18 /cm 3 ), a 1.5 μm thick GaN n-layer 4 of low carrier concentration (1×10 15 /cm 3 ), an i L -layer 5 of low impurity concentration (5×10 19 /cm 3 of Zn), and an i H -layer 6 of high impurity concentration (2×10 20 /cm 3 of Zn). To the i H layer 6 and n + -layer 3 are connected aluminum electrodes 7 and 8 , respectively. This light-emitting diode 10 was produced by the MOVPE with an organometallic compound in the following manner.

The gases employed in this process are NH 3 , H 2 (as carrier gas), trimethyl gallium (Ga(CH 3 ) 3 ) (TMG), trimethyl aluminum (Al(CH 3 ) 3 ) (TMA), silane (SiH 4 ), and diethyl zinc (DEZ).

The sapphire substrate 1 of single crystal, with its principal crystal plane (c-surface {0001}) cleaned by solvent washing and heat treatment, was set on the susceptor placed in the reaction chamber of the MOVPE apparatus.

The sapphire substrate 1 underwent vapor phase etching at 1100° C. with H 2 flowing through the reaction chamber at a flow rate of 2 l/min under normal pressure.

On the sapphire substrate 1 was formed the AlN buffer layer 2 (about 500 Å thick) at 400° C. by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, and TMA at a flow rate of 1.8×10 −5 mol/min.

On the buffer layer 2 was formed the 2.2 μm thick GaN n + -layer 3 of high carrier concentration (1.5×10 18 /cm 3 ) by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG at a flow rate of 1.7×10 −4 mol/min, and silane (diluted to 0.86 ppm with H 2 ) at a flow rate of 200 ml/min for 30 minutes, with the sapphire substrate 1 kept at 1150° C.

On the n + -layer 3 was formed the 1.5 μm thick GaN n-layer 4 of low carrier concentration (1×10 15 /cm 3 ) by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, and TMG at a flow rate of 1.7×10 −4 mol/min, with the sapphire substrate 1 kept at 1150° C.

On the n-layer 4 was formed the 0.2 μm thick GaN i L -layer 5 of low impurity concentration (5×10 19 /cm 3 of Zn) by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG at a flow rate of 1.7×10 −4 mol/min, and DEZ at a flow rate of 1.5×10 −4 mol/min, with the sapphire substrate 1 kept at 1000° C.

On the i L -layer 5 was formed the 0.2 μm thick GaN i H -layer 6 of high impurity concentration (2×10 20 /cm 3 of Zn) by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG at a flow rate of 1.7×10 −4 mol/min, and DEZ at a flow rate of 1.5×10 −4 mol/min, with the sapphire substrate 1 kept at 900° C.

Thus there was obtained the multi-layer structure as shown in FIG. 18 .

On the i H -layer 6 was formed the 2000 Å thick SiO 2 layer 11 by sputtering as shown in FIG. 19 . On the SiO 2 layer 11 was formed a photoresist layer 12 which subsequently underwent the photolithographic processing to make a pattern for the electrode connected to the n + -layer 3 .

The exposed part (not covered by the photoresist layer 12 ) of the SiO 2 layer 11 underwent etching with hydrofluoric acid for its removal, as shown in FIG. 20 .

The exposed part (not covered by the photoresist layer 12 and the SiO 2 layer 11 ) of the i H -layer 6 underwent dry etching with CCr 2 F 2 gas at a flow rate of 10 cc/min and a high-frequency electric power of 0.44 W/cm 2 in a vacuum of 0.04 Torr and subsequently underwent dry etching with argon. The dry etching removed not only the exposed part of the i H -layer 6 but also the i L -layer 5 and the n-layer 4 and the upper part of the n + -layer 3 which are underneath the exposed part of the i H -layer 6 , as shown in FIG. 21 .

The SiO 2 layer 11 remaining on the i H -layer 6 was removed with hydrofluoric arid as shown in FIG. 22 .

On the entire surface of the sample was formed an Al layer 13 by vapor deposition as shown in FIG. 23 . On the Al layer 13 was formed the photoresist layer 14 which subsequently underwent the photolithographic processing to make a pattern for the electrodes connected to the n + -layer 3 and the i H -layer 6 , respectively.

The exposed part (not covered by the photoresist layer 14 ) of the Al layer 13 underwent etching with nitric acid as shown in FIG. 23 . The photoresist 14 was removed with acetone. Thus there were formed the electrode 8 for the n + -layer 3 and the electrode 7 for the i H -layer 6 .

Such an above-mentioned process could make a gallium nitride light-emitting element of MIS structure as shown in FIG. 17 .

The thus obtained light-emitting diode 10 was found to have a luminous intensity of 0.4 mcd. This value is 8 times higher than that of the conventional light-emitting diode which is composed simply of a 0.2 μm thick i-layer with impurity concentration of 2×10 20 /cm 3 and a 4 μm thick n-layer with a carrier concentration of 5×10 17 cm 3 .

In addition, the inspection of the luminescent surface revealed that the number of luminescent points is much greater than that of the conventional light-emitting diode.

Several samples were prepared in the same manner as mentioned above except that the carrier concentration in the n-layer 4 of low carrier concentration was varied, and they were tested for luminous intensity and emission spectrum. The results are shown in FIG. 24 . It is noted that the luminous intensity decreases and the emission spectrum shifts to the red side according as the carrier concentration increases.

Also, several samples were prepared in the same manner as mentioned above except that the impurity concentration in the i H -layer 6 of high impurity concentration was varied, and they were tested for luminous intensity and emission spectrum. The results are shown in FIG. 25 . It is noted that the luminous intensity has a peak value and the emission spectrum shifts to a longer wavelength side when the impurity concentration increases.

Example 4

A light-emitting diode 10 of the same structure as in Example 1 was prepared in the same manner as in Example 1 according to the steps shown in FIGS. 2 to 7 . The resistivity of the n + -layer 3 was varied in the range of 3×10 −1 Ωcm to 8×10 −3 Ω cm by changing the conditions of the vapor phase epitaxy for the n + -layer 3 of high carrier concentration, as shown in FIG. 26 . The vapor phase epitaxy was carried out by supplying H 2 at a flow rate of 20 l/min, NH 3 at a flow rate of 10 l/min, TMG-carrying H 2 at a flow rate of 100 cc/min, and H 2 -diluted silane (0.86 ppm) at a flow rate of 10 cc/min to 300 cc/min. (The TMG-carrying H 2 was prepared by bubbling H 2 in TMG cooled at −15° C.)

In the above-mentioned case, the resistivity of the n + -layer 3 was varied by changing the flow rate of silane, but it is also possible to achieve the same object by changing the flow rate of other raw material gases or by changing the mixing ratio of silane and other raw material gases.

In this example, silane was used as the Si dopant, but it can be replaced by an organosilicon compound such as tetraethylsilane (Si(C 2 H 5 ) 4 ) in a gaseous state prepared by bubbling with H 2 .

The process mentioned above permits one to prepare the n + -layer 3 of high carrier concentration and the n-layer 4 of low carrier concentration in such a manner that their resistivity can be controlled as desired.

The thus obtained light-emitting diode 10 was found to have a luminous intensity of 0.2 mcd. This value is 4 times higher than that of the conventional light-emitting diode which is composed simply of an i-layer and an n-layer. In addition, the inspection of the luminescent surface revealed that the number of luminescent points is much greater than that of the conventional light-emitting diode.

Claims

1. A semiconductor device comprising:an n-type layer of a gallium nitride compound satisfies the formula that: AlxGa1−xN; 0≦x≦1; is doped with silicon (Si); and has a resistivity ranging from 3×10−1 Ωcm to 8×10−3 Ωcm.

2. A semiconductor device as claimed in claim 1, wherein said semiconductor device is a light-emitting device.

3. A semiconductor device as claimed in claim 1, further comprising a sapphire substrate over which said n-type layer is formed.

4. A semiconductor device as claimed in claim 3, further comprising a buffer layer between said sapphire substrate and said n-type layer.

5. A semiconductor device as claimed in claim 4, wherein said buffer layer is formed at a temperature lower than a temperature at which said n-type layer is formed.

6. A semiconductor device as claimed in claim 1, wherein said n-type layer comprises a gallium nitride compound.

7. A semiconductor device as claimed in claim 1, wherein said n-type layer is formed by organometallic compound vapor phase epitaxy.

8. A semiconductor device comprising:an n-type layer of a gallium nitride compound that is doped with silicon at a predetermined doping rate and that has a resistivity not larger than 3×10−1 Ωcm.

9. A semiconductor device comprising:an n-type layer of a gallium nitride compound that is doped with silicon at a predetermined doping rate and that has a resistivity not larger than 3×10−1 Ωcm and a carrier concentration not smaller than 6×1016/cm3.