SEMICONDUCTOR LIGHT-EMITTING DEVICE AND PRODUCTION METHOD THEREOF

Abstract: A semiconductor light-emitting device with a double hetero structure, including: an active layer made of Ga 1-x In x N (0 ≤ x ≤ 0.3) doped with a p-type impurity and an n-type impurity; and first and second cladding layers provided so as to sandwich the active layer.

Description: TECHNICAL FIELD The present invention relates to a light-emitting device made of gallium nitride type compound semiconductor used for semiconductor light-emitting devices such as blue light-emitting diodes and blue semiconductor lasers and a method for producing the same. BACKGROUND ART In recent years, it was reported that a semiconductor device using an Al x Ga y In z N (where 0 ≤ x ≤ 1, 0 ≤ y ≤ 1, 0 ≤ z ≤ 1) type compound semiconductor, which is a III-V-group compound semiconductor containing nitrogen as a V-group element, has outstanding light-emitting characteristics at room temperature. This type of compound semiconductor has been expected to be a material for realizing a blue light-emitting device (e.g., Japanese Journal of Applied Physics 32 (1993) L8-L11). Semiconductor devices having such a gallium nitride type compound semiconductor are obtained by epitaxially growing an n-type semiconductor layer, an i-type semiconductor layer, or a p-type semiconductor layer made of Al x Ga 1-x N and In y Ga 1-y N (where 0 ≤ x ≤ 1, 0 ≤ y ≤ 1) on a sapphire substrate. As a method of epitaxial growth, a Metalorganic Vapor Phase Epitaxy (MOVPE) method, a Molecular Beam Epitaxy (MBE) method, and the like are generally used. For example, the MOVPE method will be briefly described. Organic metal such as trimethylgallium (TMGa; Ga(CH 3 ) 3 ), trimethylaluminum (TMAl; Al(CH 3 ) 3 ) and trimethylindium (TMIn; In(CH 3 ) 3 ) and ammonia (NH 3 ) gas are supplied as a reaction gas into a reaction chamber in which a sapphire substrate is provided. An AlGaInN type compound semiconductor is epitaxially grown on the sapphire substrate while the surface temperature of the substrate is kept at a high temperature of 700 to 1100°C. At this time, the AlGaInN type compound semiconductor can be controlled so as to have p-type conductivity, i-type conductivity, or n-type conductivity by supplying diethylzinc (DEZn; Zn(C 2 H 5 ) 2 ), silane (SiH 4 ) or the like to the reaction chamber. As a known typical device using an AlGaInN type compound semiconductor, there is a blue light-emitting diode (e.g., Japanese Journal of Applied Physics 32 (1993) L8-L11). This light-emitting diode has a double hetero structure including an active layer made of In 0.05 Ga 0.95 N, to which zinc (Zn) is added. This is because the light-emission wavelength is adjusted to about 0.45 µm. In this manner, only zinc is added to an active layer in the conventional light-emitting diode using an InGaN active layer. Furthermore, a light-emitting diode having an MIS structure including an active layer made of Al x Ga 1-x N is reported (Japanese Laid-Open Patent Publication Nos. 4-10665, 4-10666, and 4-10667). In this light-emitting diode, Zn and Si are simultaneously added to an i-type GaN which is to form a light-emitting layer, so as to change the wavelength of the emitted light. However, these conventional light-emitting diodes have the following problems: In the case where only Zn is added to an In y Ga 1-y N layer, a Zn atom pairs off with an intrinsic defect such as vacancy in the In y Ga 1-y N layer to be stabilized. However, this decreases the emission efficiency because the intrinsic defect becomes a non-radiative center. In addition, the intrinsic defect increases under the application of an electric field, causing adverse effects such as an increased driving current and decreased reliability of the light-emitting device. In particular, these problems become serious in semiconductor lasers requiring high optical density and carrier density. Furthermore, in the case of using Zn as a p-type impurity, a large amount of Zn should be added because of its low activation ratio. In order to increase the light-emission wavelength, an increase in the In composition of In y Ga 1-y N used for an active layer is required. For example, the wavelength is desirably in a blue-green region, i.e., about 520 nm in the case of traffic lights and the like. For this purpose, the amount of In in an In y Ga 1-y N active layer is required to increase. However, the increase in amount of In decreases the quality of crystal, resulting in the decrease in emission efficiency. Thus, it is difficult to obtain a light-emitting device emitting light having a long wavelength by increasing a composition ratio (mole fraction) of In. In the case where an AlGaN layer is used as an active layer, its bandgap energy is 3.44 eV or more at room temperature, that is, the wavelength of the emitted light is 360 nm or less. Therefore, even when zinc and silicon are simultaneously added in large amounts, the light-emission wavelength is not in a blue region. Thus, it is very difficult to obtain a blue light-emitting device by using an AlGaN layer as an active layer. The AlGaN layer also has a problem in that a deep impurity level is likely to be formed, causing unnecessary light emitted through the deep impurity level; thereby increasing a working current of the light-emitting device. III-group nitrides, such as Al x Ga 1-x N and In y Ga 1-y N, are stable materials which are not subject to corrosion by chemical agents and are difficult to etch. Thus, it is difficult to form a structure for confining carriers in an active layer in a light-emitting device such as a semiconductor laser. Furthermore, it is difficult to form a cavity of a semiconductor laser by cleavage because a sapphire substrate is used in a GaN type light-emitting device. The formation of a cavity can be considered to be done by dry etching such as reactive ion etching, ion milling, and focused ion beam etching. In this case, defects are formed in a semiconductor layer in the vicinity of facets of the cavity. These defects cause problems similar to those caused by the above-mentioned intrinsic defect. In a semiconductor light-emitting device using an insulating substrate such as a sapphire substrate, electrodes cannot be provided on a substrate side. Therefore, a step difference is provided in a part of a semiconductor layer forming the light-emitting device, and electrodes are required to be respectively provided on a convex portion and a concave portion formed by the step difference. In the case of a GaN type light-emitting device, a step difference of 1 µm or more is required. However, in this case, it becomes difficult to allow a semiconductor layered structure forming a semiconductor light-emitting device to adhere to a heat sink having good heat conduction. In the case where heat-releasing of a semiconductor light-emitting device having a step difference is imperfect, there are problems in that a working current increases along with the increase in temperature of the device and reliability of the device decreases. Furthermore, when excess stress is applied to an active layer while the semiconductor layered structure forming the semiconductor light-emitting device is allowed to adhere to the heat sink, there is a possibility that light-emission stops. Even in the case where the amount of stress is small, there is a problem in that birefringence is caused in materials forming the semiconductor layered structure, and plane of polarization of light emitted from the semiconductor light-emitting device rotates. For example, this causes inconvenience in the case where a semiconductor laser is used for an optical disk or the like. The present invention solves the above-mentioned problems in the prior art and provides a highly reliable light-emitting device capable of emitting light with a wavelength in the blue region at high emission efficiency. Moreover, the present invention provides a semiconductor light-emitting device which has an outstanding heat-releasing property and in which there is less rotation of the plane of polarization of emitted light. Furthermore, the present invention provides a method for producing such a blue light-emitting device in simple steps with high yield. EP 0 599 224 A1 relates to a light-emitting galium nitride-based compound semiconductor device of a douhle-heterostructure and discloses in an example to form an Si-doped n-type Ga 0.8 Al 0.2 N layer as a first clad layer. A light-ernitting layer is grown to form an n-type In 0.14 Ga 0.86 N light-emitting layer, doped with Si and Zn on the first clad layer. Subsequently a second clad layer is grown to form an Mg-doped Ga 0.8 Al 0.2 N layer on the light-emitting layer. JP-A-6037390 of the applicant discloses a semiconductor light-emitting device with a double-heterostructure made of AlGaInN comprising an active layer, an n-type cladding layer and a p-type cladding layer provided so as to sandwich the active layer. DISCLOSURE OF THE INVENTION A semiconductor light-emitting device according to the present invention is defined in claim 1. Preferred embodiments are defined in the dependent claim. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 shows a cross-section of a semiconductor light-emitting device of the first comparative example. Figure 2 schematically shows bandgap energy of active layers of the semiconductor light-emitting device shown in Figure 1 and a conventional semiconductor light-emitting device. Figure 3 is a graph showing the relationship between the impurity concentration and the light-emission intensity. Figures 4(a) through 4(e) are cross-sectional views showing the fabrication process for the semiconductor light-emitting device shown in Figure 1 . Figures 5(a) and 5(b) show electrical characteristics and optical characteristics of the semiconductor light-emitting device of the first comparative example according to the present invention. Figure 6 shows the distribution of the impurity concentration in an active layer of the first example according to the invention. Figure 7(a) is a cross-sectional view showing the structure of another active layer of the first example ; Figure 7(b) is the distribution of the impurity concentration in the structure shown in Figure 7(a) . Figure 7(c) shows another distribution of the impurity concentration in the structure shown in Figure 7(a) . Figure 8 is a cross-sectional view showing the structure of still another active layer of the first example. Figure 9 shows a cross-section of a semiconductor light-emitting device of the secon comparative example according to the present invention. Figures 10(a) and 10(b) are cross-sectional views showing the first half of the fabrication process for the semiconductor light-emitting device shown in Figure 9 . Figure 11 schematically shows a cross-section of an electron cyclotron resonance apparatus used in the present example. Figures 12(a) through (d) are cross-sectional views showing the second half of the fabrication process for the semiconductor light-emitting device shown in Figure 9 . Figure 13 is a perspective view showing one of the fabrication process for the semiconductor light-emitting device shown in Figure 9 . Figure 14 is a cross-sectional view showing another structure of the second example. Figure 15 is a cross-sectional view showing the structure of a semiconductor light-emitting device used in the third example. Figure 16 is a cross-sectional view illustrating a method for mounting a light-emitting device shown in Figure 15 on a mount. Figure 17 is a cross-sectional view illustrating another method for mounting a light-emitting device on a mount, according to the third example. Figure 18 shows a cross-section of the semiconductor light-emitting device mounted according the method illustrated in Figure 17. Figure 19 shows another structure of a mount used in the third example. BEST MODE FOR CARRYNG OUT THE INVENTION (Example 1) Figure 1 is a cross-sectional view of a light-emitting diode 30 of the first comparative example. The light-emitting diode 30 has an active layer 38 and cladding layers 36 and 40 which are provided so as to sandwich the active layer 38 . The active layer 38 is made of In 0.05 Ga 0.95 N. On the other hand, the cladding layer 36 is made of Al 0.1 Ga 0.9 N doped with silicon as an n-type impurity, and the cladding layer 40 is made of Al 0.1 Ga 0.9 N doped with magnesium as a p-type impurity. Therefore, the light-emitting diode 30 has a double hetero structure in which heterojunctions are formed between the active layer and the cladding layers. The n-type cladding layer 36 is provided on a sapphire substrate 32 having, for example, a (0001) plane via a contact layer 34 made of n-type GaN:Si. A contact layer 42 made of p-type GaN:Mg is provided on the p-type cladding layer 40 . Furthermore, an electrode 46 made of two layers of Au and Ni is provided on the contact layer 42 . Furthermore, the contact layer 42 , the cladding layer 40, the active layer 38, and the cladding layer 36 are partially removed by etching. A part of the contact layer 34 is also etched up to approximately midpoint in the thickness direction, and an electrode 44 made of Al is provided on a face of the contact layer 34 exposed by etching. The active layer 38 has a thickness of about 1 µm, and the active layer 38 is substantially uniformly doped with zinc (Zn) functioning as a p-type impurity and silicon (Si) functioning as an n-type impurity. The wavelength of light emitted by the active layer 38 is about 460 nm. In the case where the active layer 38 is doped with both an n-type impurity and a p-type impurity, the wavelength λ of emitted light is given by the following equations: hν = E g - (E a + E d ) + e/εr λ = 1.2395/hν where E g is the bandgap of an active layer; E a is activation energy of an acceptor level; E d is activation energy of a donor level; r is the distance between donor atoms and acceptor atoms; ε is the dielectric constant of an active layer; and e is the electron charge. In the case where E d is larger than e/εr, the active layer 38 can emit light having a wavelength longer than that determined by the bandgap of the active layer. This will be described in more detail with reference to Figure 2 . In the case where the active layer 38 is doped with zinc and silicon, a donor level 54 of silicon is formed at a position lower from a conduction band 50 by E d and an acceptor level 56 of zinc is formed at a position higher than a valence band 52 by E a . Electrons in the conduction band 50 are capable of transferring to the donor level 54 by non-radiative transition and transferring to the acceptor level 56 while emitting light. Thus, in a conventional light-emitting device including an active layer with a bandgap E g2 , light having a wavelength λ emitted in the case where electrons transfer directly from the conduction band 50 to the acceptor level 56 is allowed to be emitted from an active layer with a bandgap E g1 which is larger than E g2 . As a result, it becomes possible to emit light having a long wavelength even when a composition ratio of indium (In) is small, and a highly reliable light-emitting diode can be obtained which emits light having a wavelength in a blue region at high emission efficiency, by using high-quality crystal with a small composition ratio of indium. Also, a recombination probability increases due to the acceptor level and the donor level formed by doping zinc and silicon, so that an emission efficiency also improves. Furthermore, in the case where an InGaN layer is doped only with zinc, a zinc atom pairs off with an intrinsic defect such as vacancy to be stabilized in the InGaN layer. However, by doping the InGaN layer with both zinc and silicon, the generation of an intrinsic defect is suppressed and emission efficiency improves. When the added amount of zinc and silicon is large, the acceptor level and the donor level are formed in great numbers, so that the emission efficiency of the light-emitting diode 30 increases. However, when the added amount is too large, the emission efficiency decreases. This is because impurity atoms enter interstitial positions and the like, when their amount is large, thereby decreasing the quality of the crystal itself. Figure 3 shows the relationship between the light-emission intensity and the impurity concentration of doped silicon. As shown in Figure 3 , in the case where impurity concentration of doped silicon is in the order of 10 18 cm -3 , high light-emission intensity can be obtained. Assuming that the highest light-emission intensity is 1 and a practically preferable range is up to the impurity concentration giving an intensity of 1/e, it is understood that impurities are doped preferably in the range of about 10 17 cm -3 to about 10 20 cm -3 . The added amounts of zinc and silicon can be the same or either one of them may be larger. However, the same amounts of zinc and silicon are preferably doped, because impurity level densities become equal to each other. Generally, since the activation efficiency of silicon is larger than that of zinc, in the case where zinc and silicon are doped in the impurity concentration at the same level, the conductivity of the active layer becomes an n-type. However, in order to improve the emission efficiency by increasing the hole concentration, the concentration of zinc can be increased so that the conductivity of the active layer 38 becomes a p-type. As is understood from the above description, in order to obtain a high quality active layer, the composition ratio x of In in In x Ga 1-x N forming the active layer is preferably small. However, it is technically possible to obtain an active layer containing In in the range of 0 ≤ x ≤ 0.3. In the case where zinc and silicon are doped as impurities, the light-emission wavelength can be adjusted by regulating the composition ratio of In in this range. On the other hand, the cladding layers 36 and 40 are made of Al y Ga 1-y N having an arbitrary Al composition ratio y in the range of 0 ≤ y ≤ 1. However, considering the lattice matching with the active layer, the Al composition ratio y is preferably in the range of 0 ≤ y ≤ 0.3. Furthermore, in order to confine carriers in the active layer efficiently, the energy difference ΔE c of the conduction band between the active layer 38 and at least the p-type cladding layer 40 is preferably 0.3 eV or more. The cladding layers 36 and 40 can have different compositions. For example, the cladding layer 36 made of GaN and the cladding layer 40 made of Al 0.15 Ga 0.85 N may be used. Hereinafter, an example of a method for producing the light-emitting diode 30 will be described with reference to Figures 4(a) through 4(e) . The contact layer 34 made of n-GaN, the cladding layer 36 made of n-Al 0.1 Ga 0.9 N, the active layer 38 made of In 0.05 Ga 0.95 N doped with Si, the cladding layer 40 made of p-Al 0.1 Ga 0.9 N, and the contact layer 42 made of p-GaN are epitaxially grown on the sapphire substrate 32 having a (0001) plane, by a crystal growth method such as a Metalorganic Vapor Phase Epitaxy (MOVPE) method. Furthernore, a SiO 2 film 60 is deposited on the contact layer 42 by using a thermal CVD method or the like (Figure 4(a) ). The SiO 2 film 60 is partially removed by etching, using a photolithography technique and an etching technique, whereby a part 64 of the contact layer 42 is exposed (Figure 4(b) ). Si is implanted by an ion implantation method through the surface of the contact layer 42 using the etched SiO 2 film 60 as a mask so as to reach the midpoint of the contact layer 34 (Figure 4(c) ). This damages a region 62 with Si implanted therein and degrades crystallinity. Thereafter, the region 60 with Si ions implanted therein, i.e., portions of the contact layer 42 , the cladding layer 40 , the active layer 38 , the cladding layer 36 , and the contact layer 34 ; are removed by soaking in sulfuric acid (H 2 SO 4 ) (Figure 4(d) ). Etching of the region 62 with Si ions implanted therein is relatively easy. Other etchants such as phosphoric acid (H 3 PO 4 ) and sodium hydroxide (NaOH) can be used. On the other hand, a region without Si ions implanted therein is not etched by sulfuric acid. Thereafter, the SiO 2 film 60 is removed, and the electrodes 46 and 44 are formed on the contact layer 42 and the exposed portion 64 of the contact layer 34 , respectively (Figure 4(e) ). According to the method as described above, the light-emitting diode 30 as shown in Figure 1 can be produced. Because of the use of wet etching, the steps of producing the light-emitting diode are simplified, whereby production yield can be enhanced. The electrical characteristics and optical characteristics of the light-emitting diode 30 thus produced are shown in Figures 5(a) and (b) . It is understood that a satisfactory diode with a threshold voltage of 2 volts is obtained and the light-emission wavelength is in a blue region of 460 nm. It is possible to make various alterations as described below with respect to the active layer 38 used for the light-emitting diode 30 shown in the above example. First, the wavelength of light emitted from the active layer can be regulated by appropriately selecting the composition of the active layer 38 and a p-type impurity and an n-type impurity with which the active layer 38 is doped. More specifically, light in the vicinity of a wavelength of 460 nm can be emitted by doping In 0.10 Ga 0.90 N with zinc and silicon as the p-type impurity and the n-type impurity. Light with the same wavelength can also be emitted even by doping In 0.20 Ga 0.80 N with magnesium (Mg) as the p-type impurity, and with either of sulfur (S), selenium (Se), or tellurium (Te) as the n-type impurity. Light in the vicinity of a wavelength of 500 nm can be emitted by doping In 0.30 Ga 0.70 N with magnesium and silicon as the p-type impurity and the n-type impurity, respectively. Magnesium is not likely to diffuse in a semiconductor, so that the emission efficiency increases when magnesium is selected as the p-type impurity. In addition, when magnesium is selected, the process steps of producing a device become simplified because magnesium is the same material as the p-type impurity used in the cladding layer. Carbon (C) can be used in place of the above-mentioned p-type impurities. Carbon is not likely to diffuse in a semiconductor, so that it can be doped in a high concentration, thereby increasing the emission efficiency. For example, when GaN is doped with Si and C, light with a wavelength of 430 nm can be emitted. Since the acceptor level of C is low, energy between the donor level of Si and the acceptor level of C increases, and the wavelength shortens. The impurity concentration can have a gradient in the active layer of the light-emitting diode. Figure 6 shows the impurity concentration of an active layer 70 between cladding layers 36 and 40 . The active layer 70 is the same as the active layer 38 in that it is doped with zinc and silicon. However, the concentration of zinc which is a p-type impurity increases from a face 72 in contact with the cladding layer 40 made of p-type Al 0.1 G 0.9 N, to a face 74 in contact with the cladding layer 36 made of n-type Al 0.1 Ga 0.1 N. The concentration of zinc on the face 72 is about 10 17 cm -3 and that on the face 74 is about 10 19 cm -3 . On the other hand, the concentration of silicon which is an n-type impurity increases from the face 74 in contact with the cladding layer 360 made of n-type Al 0.1 Ga 0.9 N, to the face 72 in contact with the cladding layer 40 made of p-type Al 0.1 Ga 0.9 N. The concentration of silicon on the face 74 is about 10 17 cm -3 and that on the face 72 is about 10 19 cm -3 . Figure 6 exemplifies that the concentration of impurities linearly change. However, as long as the concentration of zinc is smaller on the face 72 side and larger on the face 74 side, the concentration may change in stages or may have a curved gradient. In such a structure, the p-type impurity concentration in the active layer 70 increases with the distance from the p-type cladding layer 40 , so that holes with small mobility can be allowed to diffuse in the active layer 70 far away from the face 72 in contact with the cladding layer 40 . Thus, it becomes possible to enlarge the thickness of the active layer 70 and to further increase the emission efficiency. Herein, the case is illustrated in which the distributions of the concentrations of Si as an n-type impurity and a p-type impurity are symmetric. However, the n-type impurity may be uniformly distributed across the active layer 7 . Furthermore, the active layer can have a so-called modulation doping structure. As shown in Figure 7(a) , in an active layer 80 sandwiched between the cladding layers 36 and 40, a plurality of Tn 0.05 Ga 0.95 N layers 76 doped only with a p-type impurity and a plurality of In 0.05 Ga 0.95 N layers 78 doped only with an n-type impurity are alternately layered. In this structure, electrons and holes are spatially separated from each other. Therefore, the recombination probability increases and the emission efficiency is enhanced by an order of magnitude compared with the case where electrons and holes are not spatially separated from each other. The impurity concentration of each In 0.05 Ga 0.95 N layer 76 and In 0.05 Ga 0.95 N layer 78 can be the same as shown in Figure 7(b) . In this case, the respective concentration was prescribed to be about 10 19 cm -3 . Furthermore, as described with reference to Figure 6 , the respective concentration may have a gradient. More specifically, as shown in Figure 7(c) , of a plurality of GaInN layers 76, the p-type impurity concentration of the In 0.05 Ga 0.95 N layer 76 close to the cladding layer 36 is higher, while that of the In 0.05 Ga 0.95 N layer 76 close to the cladding layer 40 is lower. On the other hand, of a plurality of In 0.05 Ga 0.95 N layers 78, the n-type impurity concentration of the In 0.05 Ga 0.95 N layer 76 close to the cladding layer 36 is lower, while the p-type impurity concentration of the In 0.05 Ga 0.95 N layer 76 close to the cladding layer 40 is higher. Such a structure enables the further increase in emission efficiency. Alternatively, as shown in Figure 8 , an active layer 86 with a layered structure including InN 82 layers and GaN layers 84 can be provided between the cladding layers 36 and 40 . By alternately layering the InN layers 82 having a thickness of a 1-atom layer and the GaN layers 84 having a thickness of a 9-atoms layer in the active layer 86 , the active layer 86 having a composition of In 0.1 Ga 0.9 N as a whole can be formed. In this case, only the InN layers 82 are preferably doped with both zinc and silicon. This is because In has a vapor pressure higher than that of Ga and is likely to be replaced by impurities. This allows both zinc and silicon to enter the positions of In atoms in crystal and to respectively become p-type and n-type impurities without fail. Consequently, the activation ratio of the p-type impurity and the emission efficiency can be enhanced. The active layer 86 is grown by Atomic Layer Epitaxy. More specifically, nine GaN layers can be grown on the substrate by alternately introducing trimethylgallium and ammonia into a growth chamber nine times, and one InN layer can be grown by alternately introducing trimethylindium and ammonia into a growth chamber once. The InN layers are grown by simultaneously supplying dimethylzinc and silane, and doping the InN layers with both zinc and silicon. In the present example, although the case where sapphire is used for a substrate is described, other substrates made of SiC, spinel, ZnO, or the like can be used. (Example 2) Figure 9 is a cross-sectional view of a blue semiconductor laser 90 of the second example according to the present invention. The semiconductor laser 90 includes an active layer 98 and cladding layers 96 and 100 provided so as to sandwich the active layer 98 . The active layer 98 is made of In 0.1 Ga 0.9 N. The cladding layer 96 is made of Al 0.1 Ga 0.9 N doped with silicon as an n-type impurity, and the cladding layer 10 is made of Al 0.1 Ga 0.9 N doped with magnesium as a p-type impurity. Therefore, the light-emitting diode 90 has a double hetero structure in which heterojunctions are formed between the active layer and the cladding layers. The active layer 98 is an InGaN type semiconductor layer doped with both a p-type impurity and an n-type impurity described in detail in Example 1. More specifically, the active layer 98 can be an InGaN type semiconductor layer doped with p-type and n-type impurities by an impurity doping method similar to that used for the active layer 38 of the light-emitting device shown in Figure 1 or by an impurity doping method shown in Figures 6 through 8 . Furthermore, as described later, the active layer 98 is doped with hydrogen in the vicinity of two facets forming a cavity, whereby the active layer 98 is provided with a high resistance. The cladding layer 96 is provided on a sapphire substrate 92 having, for example, a (0001) plane via a contact layer 94 made of n-type GaN. A contact layer 102 made of p-type GaN is provided on the cladding layer 100 . Furthermore, an electrode 106 is provided on the contact layer 102 . Furthermore, the contact layer 102 , the cladding layer 100 , the active layer 98 , and the cladding layer 96 are partially removed by etching. A part of the contact layer 94 is also etched up to approximately midpoint in the thickness direction, and an electrode 104 is provided on a face of the contact layer 94 exposed by etching. A region 108 containing hydrogen is formed in portions of the contact layer 102 and the cladding layer 100 . The region 108 has a high resistance because of hydrogen contained therein. The region containing no hydrogen has a stripe shape extending in the cavity direction, and this region is kept in a low resistance state. Thus, holes are effectively injected from the electrode 106 into a part 110 of the active layer 98 under the region of the cladding layer 100 containing no hydrogen, which enables carriers to be effectively confined and reduces a threshold current of the semiconductor laser. In this manner, a highly reliable semiconductor laser can be obtained by providing a current confinement function on a p-Al 0.1 Ga 0.9 N cladding layer side. The reason why the region 108 has a high resistance is as follows: Atomic hydrogen having entered crystal binds to a p-type impurity (acceptor impurity) or the most adjacent constituent element to degrade the function of the p-type impurity as an acceptor and inactivate the p-type impurity. This allows the region 108 to be equivalent to a semiconductor doped with no impurities and increases the resistance thereof. Although similar inactivation is considered to be caused even in an n-type impurity, the effect of inactivation by hydrogen atoms is more conspicuous in a p-type semiconductor. Therefore, the function as a current confinement is desirably provided on the side of the p-type contact layer 102 and the p-type cladding layer 100 . Furthermore, inactivation by atomic hydrogen particularly has a greater effect on materials of Al x Ga y In z N type. Atomic hydrogen allows p-Al x Ga y In z N to have a semi-insulating state and rapidly increases the resistance thereof, whereby carriers can be effectively confined. Therefore, a laser having a structure as shown in Figure 4 can be produced. Next, a method for producing this semiconductor laser will be described with reference to Figures 10(a) , 10(b) , 11 , and 12(a) through 12(d) . First, the contact layer 94 made of n-GaN, the cladding layer 96 made of n-Al 0.1 Ga 0.9 N, the active layer 98 made of In 0.1 Ga 0.9 N, the cladding layer 100 made of p-Al 0.1 Ga 0.9 N, and the contact layer 102 made of p-GaN are epitaxially grown on the sapphire substrate 92 having a (0001) plane by using a crystal growth method such as a MOVPE method (Figure 10(a) ). Furthermore, a mask layer 112 is formed on the contact layer 102 . As the mask layer 112 , semiconductor layers made of materials other than a p-type semiconductor or insulating layers can be used, as long as they do not allow hydrogen ions to pass through. For example, undoped GaN, n-type GaAs, p-type GaN, SiO 2 , Si 3 N 4 , Si, and the like can be used for the mask layer. The mask layer 112 is formed into a stripe shape by using a photolithography technique and an etching technique, thereby exposing a part of the contact layer 102 (Figure 10(b) ). Hydrogen ions are introduced into a semiconductor structure shown in Figure 10(b) by using an electron cyclotron resonance (ECR) apparatus 120 as shown in Figure 11 . The electron cyclotron resonance apparatus 120 is equipped with a chamber 124 , magnet coils 122 provided on the periphery of the chamber 124 , a sample holder 126 , a shutter 130 , and a gas inlet 132 . Hydrogen introduced into the chamber 124 through the gas inlet 132 is excited with a microwave to form plasma 128 in the chamber 124 . The flow of plasma 128 is radiated to the sapphire substrate 92 set on the sample holder 126 . At this time, the sapphire substrate 92 is kept at a temperature of about 350°C. As a result, atomic hydrogen is injected from the surface of the contact layer 102 which is not covered with the mask layer 112 into the contact layer 102 and the cladding layer 100 (Figure 12(a) ). This is because atomic hydrogen cannot pass through the mask layer 112 and the mask layer 112 functions as a mask. During this step, the region 108 in which an acceptor is inactivated is formed. Thereafter, the semiconductor layer 112 is removed so as to expose the entire surface of the contact layer 102 , and then the electrode 106 is formed (Figure 12(b) ). Thereafter, the sapphire substrate 92 with the structure shown in Figure 12(b) is introduced into the electron cyclotron resonance (ECR) apparatus 120 , and portions of the contact layer 102 , the cladding layer 100 , the active layer 98 , and the cladding layer 96 are etched, and a portion of the contact layer 94 is etched to a midpoint thereof (Figure 12(c) ). Furthermore, as shown in Figure 13 , facets of a cavity 136 and 138 are formed by etching. Then, hydrogen is introduced into the chamber 124 through the gas inlet 132 while the sapphire substrate 92 is kept at about 350°C, and the etched facets are exposed to an atmosphere of hydrogen which has been excited into plasma by electron cyclotron resonance. This allows atomic hydrogen to enter the cavity through the facets 136 and 138 thereof, and an intrinsic defect such as vacancy in the vicinity of the facets of the cavity are compensated by hydrogen. As a result, a non-radiative center is prevented from being formed, and the increase in working current and the decrease in reliability can be suppressed. Finally, the electrode 104 is formed on the contact layer 94 , whereby the semiconductor laser 90 is completed. According to such a method, a highly reliable semiconductor laser can be produced easily with good yield without subjecting regions close to the active layer to processings such as etching. Electron cyclotron resonance enables a high-resistant region to be efficiently formed because of good excitation efficiency of hydrogen. In addition, unlike ion implantation or the like, almost no damage is caused with respect to semiconductor crystal. Electron cyclotron resonance enables a high-resistant region to be efficiently formed because of good excitation efficiency of hydrogen. Furthermore, according to electron cyclotron resonance, since hydrogen plasma is not likely to diffuse in a magnetic field direction, i.e., in a horizontal direction of each layer forming a semiconductor laser, atomic hydrogen can be allowed to enter the layered structure with width almost equal to that of the mask layer 112 formed into a stripe shape. This effect is great, because the width of the stripe is small, i.e., about 4 µm. Furthermore, implantation of atomic hydrogen into the vicinity of the facets 136 and 138 of the cavity increases the resistance of the semiconductor layer in the vicinity of the facets. Thus, heat generation can be suppressed in the vicinity of the facets of the cavity, whereby the increase in temperature of the facets of the cavity is reduced, resulting in enhanced reliability of the semiconductor laser. Although the temperature of the sample placed in hydrogen excited into plasma is kept at about 350°C in the above example, inactivation of acceptors by hydrogen atoms can be controlled by changing this temperature. Furthermore, the example is described using hydrogen as a gas containing a hydrogen element. However, any gas such as ammonia (NH 3 ) can be used, as long as it is a gas containing a hydrogen element. The above example is described using an AlGaInN type material as that for forming the semiconductor laser. However, other materials with large bandgap can be used. Even a ZnMgSSe type material which is a II-VI-group compound is used, the effect of the present invention is great. For example, as shown in Figure 14 , the idea of the present invention can be applied to a semiconductor laser 200 including a cladding layer 204 made of n-ZnMgSSe, a light confinement layer 208 made of n-ZnSe, an active layer 210 made of CdZnSe, a light confinement layer 212 made of p-ZnSe, a cladding layer 214 made of p-ZnMgSSe, and a contact layer 216 made of p-ZnSe on a substrate 202 made of semi-insulating ZnSe. A region 220 doped with hydrogen is formed in portions of the contact layer 216 , the cladding layer 214 , and the light confinement layer 212 . A current flowing through the active layer 210 is confined by a voltage applied across an electrode 218 formed on the contact layer 216 and an electrode 204 formed on the cladding layer 204 . In the present example, although the case where sapphire is used for a substrate is described, other materials such as SiC, spinel, and ZnO can be used for the substrate. (Example 3) In the present example, a method for mounting a semiconductor laser according to the present invention will be described. A semiconductor laser 302 used in the present example has a semiconductor structure 304 formed on a substrate 320 made of sapphire or the like, as shown in Figure 15 . The semiconductor structure 304 includes an active layer 308 and cladding layers 306 and 310 sandwiching the active layer. The active layer 306 is made of In x Ga 1-x N, and the cladding layers 306 and 310 are made of p-Al y Ga 1-y N and n-AlyGa 1-y N, respectively. The semiconductor structure 304 has a step difference, which forms a concave portion 314 and a projected portion 312 . At least the active layer 306 is included in the projected portion 312 . An electrode 316 is formed on the surface of the projected portion 312 so as to be electrically connected to the cladding layer 306 , and an electrode 318 is formed on the surface of the concave portion 314 so as to be electrically connected to the cladding layer 310 . There is a gap D1 of 2.8 µm between the surface of the electrode 316 and that of the electrode 318 . As shown in Figure 16 , a mount 324 on which a semiconductor laser 302 is mounted also has a step difference, forming a projected portion 326 and a concave portion 328 . On the surfaces of the projected portion 326 and the concave portion 328 , bumps 330 and 332 are respectively provided. The mount 324 is made of a heat sink, Si, and the bumps 330 and 332 are made of an alloy of gold and tin. There is a gap D2 of 3.0 µm between the surfaces of the bumps 330 and 332 . A mounting method will be described with reference to Figure 16 . The semiconductor laser 302 is set on a submount 324 by using a vacuum collet 322 . When the semiconductor laser 302 is brought closer to the mount 324 , the electrode 318 on the semiconductor laser 302 first comes into contact with the bump 330 because D2 is larger than D1 . A load is imposed from the semiconductor laser 302 side to crush the bump 330 so as to make it thinner, whereby the electrode 316 is brought into contact with the bump 332 . Thereafter, a Si submount 301 is heated to 280°C to melt the bumps 330 and 332 , whereby the semiconductor 302 is brought into contact with the submount 324. According to the above-mentioned method, a semiconductor laser with unevenness can be brought into contact with a heat sink with good heat conduction. Thus, the increase in temperature of the semiconductor laser can be suppressed, and reliability of the device can be prevented from decreasing. Furthermore, the electrode 318 provided on the concave portion 314 of the semiconductor laser 302 comes into contact with the bump 330 , so that the active layer 308 of the semiconductor laser is not excessively pressurized. Thus, the semiconductor laser is not adversely affected. In particular, there is no problem that plane of polarization of emitted light rotates due to birefringence of the constituent materials caused by stress. In the above example, an alloy of gold and tin is used for bumps. However, any materials can be used, which are capable of being melted to bring the semiconductor laser into contact with the heat sink. For example, an alloy of lead and gold, indium, and the like can be used. As described below, a UV-curable resin can be injected between the semiconductor laser 302 and the mount 324 . As shown in Figures 17 and 18 , a UV-curable resin 336 is coated onto the surface of the mount 324 so as to cover the electrode bumps 338 and 340 respectively provided on the projected portion 326 and the concave portion 328 of the submount 306 . In this case, the bumps 338 and 340 are gold-plated. As described above, first, the electrode 318 of the semiconductor laser 302 is brought into contact with the bump 338 . A load is imposed from the semiconductor laser 302 side to crush the bump 338 so as to make it thinner, whereby the electrode 316 is brought into contact with the bump 340 . At this time, the contact between the electrode 318 and the bump 338 can be confirmed by monitoring resistance between the bumps 338 and 340 . Thereafter, a voltage is applied to the semiconductor laser 302 , thereby allowing the laser to emit light. In this case, the laser is not necessarily oscillated. The UV-curable resin 336 is cured by absorbing light having leaked from the semiconductor laser 302 , whereby the semiconductor laser 302 can be mounted on the submount 324 . Examples of materials for the semiconductor laser emitting light with a wavelength capable of efficiently curing the UV-curable resin include those of an AlGaInN type, ZnMgSSe type, and the like. A semiconductor laser with unevenness can be brought into contact with a heat sink with good heat conduction by the above-mentioned method. Thus, the increase in temperature of the semiconductor laser can be reduced, preventing reliability of the semiconductor laser from decreasing. Furthermore, the electrode 318 provided on the concave portion 314 of the semiconductor laser 302 comes into contact with the bump 338 , so that the active layer 308 of the semiconductor laser is not excessively pressurized. Thus, the semiconductor laser is not adversely affected. In particular, there is no problem that the plane of polarization of the emitted light rotates due to birefringence of the constituent materials caused by stress. In the above example, the UV-curable resin is cured by allowing the semiconductor laser to emit light. However, the UV-curable resin can be cured by being irradiated with UV-rays from outside. In the above example, although a UV-curable resin is used as that for mounting the semiconductor laser onto the submount, a thermosetting resin can also be used. Furthermore, even when other materials having a good heat-releasing property, such as SiC, C, and AlN, are used for the submount; the effect of the present invention is great. Furthermore, the Si submount has unevenness in the above example. However, two bumps 342 and 344 having difference D2 in thickness are provided on a mount 346 with a flat surface as shown in Figure 19 . The semiconductor laser can be mounted on the mount in the same way as the above. INDUSTRIAL APPLICABILITY According to the present invention, a highly reliable light-emitting device can be obtained, which is capable of emitting light with a wavelength in a blue region at a high emission efficiency. Furthermore, a semiconductor light-emitting device with an outstanding heat-releasing property can be obtained, in which there is less rotation of the plane of polarization of emitted light. Additionally, a method for producing such a blue light-emitting device by simple steps with high yield can be provided.

Claims: A semiconductor light-emitting device with a double hetero structure, comprising: an active layer (70) made of Ga 1-x In x N (0 ≤ x ≤ 0.3) doped with a p-type impurity and an n-type impurity; first and second cladding layers (36, 40) provided so as to sandwich the active layer (70), wherein the first cladding layer (40) has a p-type conductivity, characterized in that the concentration of the p-type impurity in the active layer (70) is lower on a side adjacent to the first cladding layer (40), and concentration of the p-type impurity in the active layer (70) is higher on a side adjacent to the second cladding layer (36). A semiconductor light-emitting device according to claim 1, wherein the active layer (70) is substantially uniformly doped with the n-type impurity. A semiconductor light-emitting device according to claim 1, wherein the active layer (80) has a structure in which a plurality of p-type layers (76) doped only with a p-type impurity and a plurality of n-type layers (78) doped only with an n-type impurity are alternately layered. A semiconductor light-emitting device according to claim 3, wherein the impurity concentration of the plurality of p-type layers (76) in the active layer (80) increases from a side adjacent to the first cladding layer (40) to a side adjacent to the second cladding layer (36). A semiconductor light-emitting device according to claim 4, wherein the plurality of p-type layers (76) and the plurality of n-type layers (78) are substantially uniformly doped with the p-type impurity and the n-type impurity, respectively. A semiconductor light-emitting device according to claim 1, wherein the active layer (86) has a structure in which a plurality of GaN layers (84) and a plurality of InN layers (82) are alternately layered, and only the plurality of InN layers (82) are doped with the p-type impurity and the n-type impurity. A semiconductor light-emitting device according to claim 1, wherein the active layer (70) is doped with the p-type impurity and the n-type impurity respectively in an impurity concentration in the range of 10 17 cm -3 to 10 20 cm -3 . A semiconductor light-emitting device according to claim 1, wherein the p-type impurity is either of zinc, magnesium, or carbon, and the n-type impurity is either of silicon, sulfur, selenium, or tellurium. A semiconductor light-emitting device according to claim 1, wherein the first and second cladding layers (36, 40) are made of Al y Ga 1-y N (0 ≤ y ≤ 0.3). A semiconductor light-emitting device according to claim 1, wherein the energy difference of the conduction bands of the active layer (70) and the first cladding layer (40) 0.3 eV or more.

Inventors: ADACHI HIDETO, BAN YUZABURO, ISHIBASHI AKIHIKO, KIDOGUCHI ISAO, KUBO MINORU, OHNAKA KIYOSHI, ADACHI, HIDETO, BAN, YUZABURO, ISHIBASHI, AKIHIKO, KIDOGUCHI, ISAO, KUBO, MINORU, OHNAKA, KIYOSHI
Applicants: MATSUSHITA ELECTRIC IND CO LTD, MATSUSHITA ELECTRIC INDUSTRIAL CO., LTD.
Application year: 1995
Main classification: H01L33
IPC codes: H01S5, H01L33