JP2009038408A - Semiconductor light emitting element - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a semiconductor light emitting element achieving a low initial deterioration rate and a long life. <P>SOLUTION: The semiconductor light-emitting element includes a nitride gallium substrate, an n-type cladding layer which is formed on the nitride gallium substrate and is made of a nitride compound semiconductor, an active layer which is formed on the n-type cladding layer and is made of a nitride compound semiconductor, and a p-type cladding layer which is formed on the active layer and is made of a nitride compound semiconductor. The p-type cladding layer contains hydrogen and magnesium as impurities. An n-type diffusion blocking layer made of a nitride compound semiconductor represented by Al<SB>y</SB>Ga<SB>1-x</SB>N (0≤x≤1) is provided between the active layer and the p-type cladding layer, and an undoped InGaN layer is provided between the n-type diffusion blocking layer and a p-type electron barrier layer. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

  The present invention relates to a semiconductor light emitting device such as a semiconductor laser or a light emitting diode using a nitride compound semiconductor.

  In recent years, research on III-V nitride compound semiconductors has been actively conducted as materials for light-emitting elements and electronic devices. In addition, using the characteristics, blue light emitting diodes, green light emitting diodes, and blue-violet semiconductor lasers as light sources for next-generation high-density optical disks have already been put into practical use.

  Examples of conventional semiconductor lasers include those disclosed in Patent Document 1 or Patent Document 2.

In Patent Literature 1, an active layer made of a nitride semiconductor containing indium (In) and gallium (Ga), having an first layer and a second surface, and In _x Ga _{1 in contact with} the first surface of the active layer. an n-type nitride semiconductor layer made of _{-x n (0 ≦ x <1} ), Al y Ga 1-y n in contact with the second surface of the active layer (0 <y <1) p-type nitride consisting A nitride semiconductor light emitting device comprising a semiconductor layer is described.

  In Patent Document 2, an active layer made of a first nitride-based III-V compound semiconductor containing indium and gallium is in contact with the active layer and is different from the first nitride-based III-V compound semiconductor. An intermediate layer made of a second nitride III-V compound semiconductor containing indium and gallium, and a third nitride III-V compound semiconductor containing aluminum (Al) and gallium in contact with the intermediate layer A semiconductor light emitting device having a cap layer is described.

Japanese Patent No. 2780691 JP 2002-261395 A

  However, in the semiconductor laser of Patent Document 1, the initial deterioration rate during energization is large, and the operating current gradually increases with time. For this reason, there is a problem that it is difficult to extend the life and the yield is greatly reduced.

  On the other hand, Patent Document 2 proposes that a nitride III-V compound semiconductor layer containing indium such as InGaN and gallium is interposed between the active layer and the cap layer. However, this structure alone does not provide a sufficiently long lifetime, and problems such as deterioration in light emission characteristics and reduction in reliability still remain unsolved.

  The present invention has been made in view of these points. That is, an object of the present invention is to provide a semiconductor light emitting device having a low initial deterioration rate and a long lifetime.

  Other objects and advantages of the present invention will become apparent from the following description.

The present invention relates to a gallium nitride substrate, an n-type clad layer formed on the gallium nitride substrate and made of a nitride compound semiconductor, and formed on the n-type clad layer and made of a nitride compound semiconductor. In a semiconductor light emitting device comprising an active layer and a p-type cladding layer formed on the active layer and made of a nitride compound semiconductor, the p-type cladding layer contains hydrogen and magnesium as impurities, and the active layer An n-type diffusion prevention layer made of a nitride compound semiconductor represented by Al _y Ga _1-x N (where 0 ≦ x <1) is provided between the p-type cladding layer and the p-type cladding layer. An undoped InGaN layer is provided between a p-type diffusion barrier layer and the p-type electron barrier layer.

  According to the present invention, since the n-type diffusion preventing layer is provided between the active layer and the p-type cladding layer, it is possible to prevent magnesium and hydrogen from moving from the p-type cladding layer to the active layer. Therefore, a semiconductor light emitting device having a low initial deterioration rate and a long life can be obtained.

  In the nitride-based compound semiconductor light-emitting device, the cause of an increase in the initial deterioration rate when energized is that magnesium, which is a dopant in the p-type semiconductor layer, diffuses into the active layer during operation. On the other hand, when a compound containing hydrogen is used as a raw material in the manufacturing process of the semiconductor light emitting device, hydrogen remains in the semiconductor layer. The present inventor considered that the diffusion of hydrogen into the active layer is also a cause of increasing the initial deterioration rate, and has led to the present invention.

  As described above, the p-type semiconductor layer contains magnesium as a dopant. Further, since hydrogen is bonded to magnesium, the p-type semiconductor layer contains more hydrogen than in the n-type semiconductor layer. For this reason, the factor that increases the initial deterioration rate is the diffusion of hydrogen and magnesium from the p-type semiconductor layer to the active layer.

  Therefore, in the present invention, an n-type diffusion prevention layer made of a compound represented by the formula (1) is provided between the active layer and the p-type semiconductor layer, more specifically, between the active layer and the p-type cladding layer. Examples of the n-type impurity doped in the n-type diffusion prevention layer include silicon (Si), selenium (Se), and sulfur (S).

_{In x Al y Ga 1-x} -y N (x ≧ 0, y ≧ 0, x + y <1) (1)

In the present invention, the n-type diffusion prevention layer may consist of only one layer or a plurality of layers. In the former case, the doping concentration of the n-type impurity in the n-type diffusion prevention layer is preferably 5 × 10 ¹⁷ cm ⁻³ or more and 5 × 10 ¹⁹ cm ⁻³ or less. On the other hand, in the latter case, the n-type impurity may be contained in at least one layer constituting the n-type diffusion prevention layer.

  By providing the n-type diffusion prevention layer, it is possible to prevent hydrogen and magnesium from diffusing into the active layer from the p-type semiconductor layer, so that the initial deterioration rate during energization can be made smaller than before.

  Hereinafter, the present invention will be described in detail with reference to the drawings.

Embodiment 1 FIG.
FIG. 1 is a cross-sectional view of a group III-V nitride compound semiconductor laser device in the present embodiment.

  As shown in FIG. 1, a semiconductor laser device 101 includes an n-type GaN layer 103, an n-type cladding layer 104, an n-type light guide layer 105, a multiple quantum well (MQW) on the surface of a substrate 102 made of gallium nitride (GaN). ) The active layer 106, the n-type diffusion prevention layer 107, the p-type electron barrier layer 108, the p-type cladding layer 109, and the p-type contact layer 110 are sequentially stacked. A striped ridge 111 is formed on the p-type cladding layer 109 and the p-type contact layer 110. The ridge 111 is provided to define a waveguide that is a region where current is confined inside the active layer 106. Note that the n-type GaN layer 103 and the n-type light guide layer 105 may be omitted.

  On the p-type electron barrier layer 108, an insulating film 112 is formed so as to cover the ridge 111. However, an opening 113 is provided in the insulating film 112 on the ridge 111, and the p-side electrode 114 is in contact with the p-type contact layer 110 in the opening 113. On the other hand, an n-side electrode 115 is provided on the surface of the substrate 102 where the n-type GaN layer 103 is not formed.

  When a forward current is supplied between the p-side electrode 114 and the n-side electrode 115, electrons and holes are injected into the active layer 106 to generate light. This light is confined in the waveguide and amplified, and is emitted as laser light from the emission end face side of the resonance surface.

  Next, a method for manufacturing the semiconductor laser element 101 will be described.

  In general, as a method for crystal growth of a group III-V nitride compound semiconductor layer, a metal organic vapor phase epitaxy method (MOCVD method), a molecular beam epitaxy method (MBE method), a hydride vapor phase epitaxy method (HVPE method), etc. Is mentioned. In this embodiment, the MOCVD method is used, but other methods may be used.

In the present embodiment, trimethylgallium (TMG), trimethylaluminum (TMA), and trimethylindium (TMI) are used as the group III compound material, and ammonia (NH ₃ ) is used as the group V compound material. Further, monosilane (SiH ₄ ) is used as a raw material for n-type impurities, and cyclopentadienyl magnesium (Cp ₂ Mg) is used as a raw material for p-type impurities. Furthermore, hydrogen (H ₂ ) and nitrogen (N ₂ ) are used as carrier gases for these raw materials.

First, a substrate 102 made of gallium nitride (GaN) and having a (0001) plane as a main surface is prepared. Here, a substrate that is off-angled by 0.1 degrees or more and 1 degree or less in the <1-100> direction or the <11-20> direction with respect to the main surface (0001) is used as the substrate orientation. Accordingly, the step direction and density are defined, so that a semiconductor layer having excellent crystallinity and flatness can be formed. Therefore, since the density of point defects and stacking faults in the p-type semiconductor layer can be reduced, diffusion of residual hydrogen and magnesium in the p-type semiconductor can be reduced. Next, after placing the substrate 102 in the MOCVD apparatus, the temperature is raised to 1,000 ° C. while supplying ammonia (NH ₃ ) gas. Next, trimethylgallium (TMG) gas and monosilane (SiH ₄ ) gas are supplied to form an n-type GaN layer 103 on the main surface of the substrate 102. The film thickness of the n-type GaN layer 103 can be about 1 μm, for example.

Subsequently, trimethylaluminum (TMA) gas is further supplied to form an n-type cladding layer 104 made of n-type aluminum gallium nitride (Al _0.07 Ga _0.93 N) on the n-type GaN layer 103. . The film thickness of the n-type cladding layer 104 can be about 1.0 μm, for example.

  Next, the supply of trimethylaluminum (TMA) gas is stopped. The supply of other gases remains the same. Thereby, the n-type light guide layer 105 made of n-type GaN is formed on the n-type cladding layer 104. The film thickness of the n-type light guide layer 105 can be set to, for example, about 0.1 μm.

Next, the supply of trimethylgallium (TMG) gas and monosilane (SiH ₄ ) gas is stopped, and the temperature is lowered to 700 ° C. Then, a multiple quantum well active layer 106 made of indium gallium nitride (InGaN) is formed on the n-type light guide layer 105.

Specifically, first, a well layer made of In _0.12 Ga _0.88 N is grown by supplying trimethylgallium (TMG) gas, trimethylindium (TMI) gas, and ammonia (NH ₃ ) gas. Next, the supply of trimethylindium (TMI) gas is stopped, and a barrier layer made of GaN is formed. The thickness of the well layer can be, for example, about 3.5 nm. Further, the thickness of the barrier layer can be set to, for example, about 7.0 nm. By forming the well layers and the barrier layers alternately, the active layer 106 that is a laminate of these layers can be formed. For example, the active layer 106 can be formed by forming three pairs of well layers and barrier layers.

Next, the temperature is raised again to 1,000 ° C. while supplying ammonia (NH ₃ ) gas. Then, trimethylgallium (TMG) gas, trimethylaluminum (TMA) gas, and monosilane (SiH ₄ ) gas are supplied to prevent n-type diffusion of n-type Al _0.03 Ga _0.97 N on the active layer 106. Layer 107 is formed. The film thickness of the N-type diffusion prevention layer 107 can be set to, for example, 50 nm, and the doping concentration can be set to, for example, 1 × 10 ¹⁸ cm ⁻³ .

Next, after the supply of monosilane (SiH ₄ ) gas is stopped, cyclopentadienyl magnesium (Cp ₂ Mg) gas is supplied. A p-type electron barrier layer 108 made of p-type Al _0.2 Ga _0.8 N and a p-type cladding layer made of p-type Al _0.07 Ga _0.93 N are formed on the n-type diffusion prevention layer 107. 109 in order. The film thickness of the p-type electron barrier layer 108 can be set to, for example, about 0.02 μm. The film thickness of the p-type cladding layer 109 can be set to, for example, about 0.4 μm.

  Next, when the supply of trimethylaluminum (TMA) gas is stopped, the p-type contact layer 110 made of p-type GaN can be formed on the p-type cladding layer 109. The film thickness of the p-type contact layer 110 can be about 0.1 μm, for example.

After the p-type contact layer 110 is formed, the supply of trimethylgallium (TMG) gas and cyclopentadienyl magnesium (Cp ₂ Mg) gas is stopped, and the temperature is lowered to room temperature.

  After the above steps are completed, the ridge 111 is formed using a lithography method. Specifically, after applying a resist on the entire surface, the resist is processed into a pattern corresponding to a predetermined shape. Next, the p-type contact layer 110 and the p-type cladding layer 109 are etched by reactive ion etching (RIE) using the obtained resist pattern as a mask. Thereby, the ridge 111 can be formed. As an etching gas in the RIE method, for example, a chlorine-based gas can be used.

Next, an insulating film 112 is formed on the p-type electron barrier layer 108 so as to cover the ridge 111. Next, an opening 113 is formed in the insulating film 112 on the ridge 111 by using a lift-off method. Specifically, first, the insulating film 112 is formed on the entire surface by a chemical vapor deposition method (CVD method), a vacuum evaporation method, a sputtering method, or the like with the resist pattern remaining. As the insulating film 112, for example, a SiO ₂ film having a thickness of about 0.2 μm can be used. Next, when the insulating film 112 is removed together with the resist pattern, an opening 113 is formed in the ridge 111 portion.

  Next, a platinum (Pt) film and a gold (Au) film are sequentially formed on the entire surface by a vacuum deposition method or the like. Next, these films are removed using a lithography method, leaving at least the opening 113 part. Thereby, the p-side electrode 114 that is in ohmic contact with the p-type contact layer 110 through the opening 113 can be formed.

  Next, a titanium (Ti) film, a platinum (Pt) film, and a gold (Au) film are sequentially formed on the entire back surface of the substrate 102 by a vacuum deposition method or the like. Thereafter, an alloy process is performed to form an n-type electrode 115 functioning as an ohmic electrode.

  After the above steps are completed, the substrate 102 is processed into a rod shape by cleavage or the like to form both resonator end faces (not shown). Then, after applying an appropriate coating to these end faces, it is further processed into chips by cleavage or the like. Thereby, the semiconductor laser element 101 can be obtained.

In the above method, an organic metal, ammonia and hydrogen are used as raw materials. For this reason, hydrogen is taken into the nitride-based compound semiconductor layer. In particular, in the p-type semiconductor layer, magnesium used as a dopant is combined with hydrogen, so that more hydrogen remains than in the n-type semiconductor layer. In general, the amount of magnesium doped in the p-type semiconductor layer is 1 × 10 ¹⁸ cm ⁻³ or more, and the amount of residual hydrogen is the same as or less than that of magnesium.

  If hydrogen remains in the semiconductor layer, along with the defects, it causes a decrease in characteristics and lifetime of the semiconductor laser element. This is because the active layer deteriorates due to the diffusion of hydrogen into the active layer. In particular, as described above, the p-type semiconductor layer contains magnesium as a dopant, and since this magnesium is bonded to hydrogen, more hydrogen is contained in the p-type semiconductor layer than in the n-type semiconductor layer. Will be included. Therefore, in order to reduce the initial deterioration rate of the semiconductor laser element, it is effective to suppress diffusion of hydrogen and magnesium from the p-type semiconductor layer to the active layer.

According to the present embodiment, since the n-type diffusion prevention layer is provided between the diffusion layer and the p-type semiconductor layer, it is possible to prevent hydrogen and magnesium from diffusing from the p-type semiconductor layer to the active layer. This residual hydrogen in the p-type semiconductor is present in the form of H ^+, H ⁺ is because not diffuse to the active layer to be easily trapped in electrons present in the N-type diffusion preventing layer. FIG. 8 is a diagram showing the concentration profile results of magnesium, hydrogen, and silicon in the depth direction of the semiconductor laser device according to the first embodiment. It can be seen that the N-type diffusion prevention layer prevents diffusion of hydrogen and magnesium in the p-type semiconductor into the active layer. Therefore, since the initial deterioration rate can be reduced as compared with the prior art, it is possible to obtain a semiconductor laser element having a long life and high reliability.

FIG. 2 shows the result of conducting an energization test on the semiconductor laser device according to the present embodiment. As a comparative example, a semiconductor laser device manufactured in the same manner as described above except that an undoped Al _0.03 Ga _0.97 N layer having a thickness of 50 nm was provided instead of the n-type diffusion prevention layer. It also shows.

  The energization test was performed at a temperature of 80 ° C. and an optical output of 80 mW. In FIG. 2, the horizontal axis represents energization time. The vertical axis represents the rate of increase in operating current, that is, the rate of increase in operating current relative to the operating current immediately after the start of energization.

  As shown in FIG. 2, in the semiconductor laser device of the comparative example, the rate of increase in operating current after 200 hours from the start of energization exceeds 10%. For this reason, the practical level for optical discs cannot be satisfied. On the other hand, in the semiconductor laser device of the present embodiment, the increase rate of the operating current is less than 10% even after 1,000 hours have elapsed from the start of energization. Accordingly, it has been found that by providing the n-type diffusion prevention layer, a semiconductor laser element having a low initial deterioration rate and a long lifetime can be realized.

  FIG. 3 shows the results of conducting an energization test on the semiconductor laser device according to the present embodiment while changing the impurity doping concentration in the diffusion prevention layer. Here, the film thickness of the n-type diffusion preventing layer is 50 nm.

In FIG. 3, the horizontal axis represents the doping concentration of silicon as an impurity, and varies in the range of 1 × 10 ¹⁷ cm ^{−3 to} 5 × 10 ²⁰ cm ⁻³ . The vertical axis represents the rate of increase in operating current after 1,000 hours have elapsed since the start of energization. The energization test was performed at a temperature of 80 ° C. and an optical output of 80 mW.

As shown in FIG. 3, when the silicon doping concentration is smaller than 5 × 10 ¹⁷ cm ^{−3, the} rate of increase in operating current increases and the degree of deterioration increases. This is considered to be because magnesium and hydrogen in the p-type semiconductor layer are not effectively prevented from diffusing into the active layer due to the low concentration of the n-type impurity in the diffusion prevention layer. Also, when the doping concentration of silicon is higher than 5 × 10 ¹⁹ cm ^{−3, the} rate of increase in operating current increases. This is presumably because the deterioration of the semiconductor laser device increases due to the decrease in crystallinity of the n-type AlGaN layer constituting the diffusion prevention layer.

FIG. 3 shows that when the silicon doping concentration is 5 × 10 ¹⁷ cm ⁻³ or more and 5 × 10 ¹⁹ cm ⁻³ or less, the increase rate of the operating current is 10% or less. In particular, when the doping concentration is 1 × 10 ¹⁸ cm ⁻³ or more and 2 × 10 ¹⁹ cm ⁻³ or less, the increase rate of the operating current is suppressed to a low value. In other words, if the doping concentration is within this range, it is possible to effectively prevent magnesium and hydrogen in the p-type semiconductor layer from diffusing into the active layer. can do.

Even when selenium or sulfur is used instead of silicon as the n-type impurity, the doping concentration is preferably 5 × 10 ¹⁷ cm ⁻³ or more and 5 × 10 ¹⁹ cm ⁻³ or less, and 1 × 10 ^18. More preferably, the doping concentration is from cm ⁻³ to 2 × 10 ¹⁹ cm ⁻³ .

FIG. 4 shows the result of conducting an energization test on the semiconductor laser device according to the present embodiment while changing the film thickness of the n-type AlGaN diffusion prevention layer. The horizontal axis is the film thickness of the diffusion preventing layer, and changes in the range of 0 nm to 300 nm. The vertical axis shows the rate of increase in operating current after 1000 hours from the start of energization and the operating voltage. The energization test was performed at a temperature of 80 ° C. and an optical output of 80 mW. The doping concentration of silicon as an n-type impurity was 1 × 10 ¹⁸ cm ⁻³ .

  As shown in FIG. 4, when the film thickness of the diffusion prevention layer becomes thinner than 5 nm, the rate of increase in operating current increases and the degree of deterioration increases. This is presumably because magnesium and hydrogen in the p-type semiconductor layer are not effectively prevented from diffusing into the active layer due to the small amount of n-type impurities contained in the diffusion prevention layer. On the other hand, if the thickness of the diffusion preventing layer is 5 nm or more, the rate of increase in operating current can be reduced. That is, if the film thickness is 5 nm or more, it is possible to effectively prevent magnesium and hydrogen in the p-type semiconductor layer from diffusing into the active layer.

  However, as the thickness of the diffusion prevention layer increases, the operating voltage gradually increases. This is because as the N-type diffusion prevention layer becomes thicker, the PN junction becomes a state called a remote junction and the potential barrier increases. The film thickness of the N-type diffusion prevention layer, which is less affected by the formation of the remote junction, is up to about 200 nm, and the operating voltage exceeds 6 V if it is thicker than that. When a semiconductor laser element is used for an optical disk, this is not preferable because it results in an increase in power consumption. In addition, when the thickness of the N-type diffusion prevention layer is increased, the efficiency of injection of carriers into the active layer is also reduced, resulting in deterioration of laser characteristics.

  From the above, the film thickness of the diffusion prevention layer is preferably 5 nm or more and 200 nm or less, and particularly preferably 10 nm or more and 150 nm or less from the viewpoint of effectively suppressing the increase rate of the operating current. More preferably, the thickness is 100 nm or less.

Thus, by providing the n-type diffusion prevention layer between the active layer and the p-type cladding layer, it is possible to prevent magnesium and hydrogen from moving from the p-type cladding layer to the active layer. Therefore, it is possible to obtain a semiconductor laser element having a lower initial deterioration rate and a longer life than the conventional one. In this case, the doping concentration of the n-type impurity in the n-type diffusion prevention layer is preferably 5 × 10 ¹⁷ cm ⁻³ or more and 5 × 10 ¹⁹ cm ⁻³ or less. The thickness of the n-type diffusion prevention layer is preferably 5 nm or more and 200 nm or less.

  In the above embodiment, the p-type electron barrier layer is provided between the n-type diffusion prevention layer and the p-type cladding layer so as to be in contact with the n-type diffusion prevention layer. In the present invention, the p-type electron barrier layer is not necessarily provided, but the provision of the p-type electron barrier layer further effectively suppresses diffusion of magnesium and hydrogen from the p-type cladding layer to the active layer. It becomes possible to do.

  In the present embodiment, as shown in FIG. 5, an undoped guide layer 116 may be provided between the active layer 106 and the n-type diffusion prevention layer 107. In FIG. 5, the parts denoted by the same reference numerals as those in FIG. 1 are the same.

As the guide layer 116, for example, an undoped In _0.02 Ga _0.98 N layer having a thickness of 30 nm can be used. By providing the guide layer 116, light confinement can be improved, and a desired far-field pattern (FFP) can be obtained.

  Furthermore, in this embodiment, as shown in FIG. 6, an undoped GaN layer 117 can be provided between the n-type diffusion prevention layer 107 and the p-type electron barrier layer 108. In FIG. 6, the same reference numerals as those in FIG. 1 or 5 indicate the same parts.

The film thickness of the GaN layer 117 can be about 5 nm, for example. By providing the GaN layer 117, the blocking effect against overflow of electrons injected into the active layer 106 can be enhanced by the conduction band energy difference (ΔE _c ) between the p-type electron barrier layer 108 and the GaN layer 117. . Therefore, excellent laser characteristics can be obtained even at high temperatures and high outputs. Note that an undoped In _0.02 Ga _0.98 N layer may be used instead of the undoped GaN layer. In this case, since ΔE _c can be further increased, it is possible to further suppress the overflow of electrons.

Embodiment 2. FIG.
In the first embodiment, an n-type AlGaN layer composed of a single layer is used as the n-type diffusion prevention layer. On the other hand, in this embodiment, an n-type diffusion prevention layer formed of a compound represented by the formula (2) and including a plurality of layers is used.

_{In x Al y Ga 1-x} -y N (x ≧ 0, y ≧ 0, x + y <1) (2)

  FIG. 7 is a cross-sectional view of a III-V group nitride compound semiconductor laser device in the present embodiment.

  As shown in FIG. 7, a semiconductor laser device 201 includes an n-type GaN layer 203, an n-type cladding layer 204, an n-type light guide layer 205, a multiple quantum well (MQW) on the surface of a substrate 202 made of gallium nitride (GaN). ) The active layer 206, the n-type diffusion prevention layer 207, the p-type electron barrier layer 208, the p-type cladding layer 209, and the p-type contact layer 210 are stacked in this order. The p-type cladding layer 209 and the p-type contact layer 210 are formed with striped ridges 211. The ridge 211 is provided to define a waveguide which is a region where current is confined inside the active layer 206. Note that the n-type GaN layer 203 and the n-type light guide layer 205 may not be provided.

  An insulating film 212 is formed on the p-type electron barrier layer 208 so as to cover the ridge 211. However, an opening 213 is provided in the insulating film 212 on the ridge 211, and the p-side electrode 214 is in contact with the p-type contact layer 210 in the opening 213. On the other hand, an n-side electrode 215 is provided on the surface of the substrate 202 where the n-type GaN layer 203 is not formed.

  When a forward current is supplied between the p-side electrode 214 and the n-side electrode 215, electrons and holes are injected into the active layer 206 to generate light. This light is confined in the waveguide and amplified, and is emitted as laser light from the emission end face side of the resonance surface.

  The semiconductor laser element 201 can be manufactured in the same manner as in the first embodiment. However, in the first embodiment, the n-type diffusion prevention layer 207 includes an n-type AlGaN layer 207a and an n-type InGaN layer 207b. It is different in point. These layers can be formed by using, for example, a metal organic chemical vapor deposition method (MOCVD method).

The n-type AlGaN layer 207a is formed, for example, by raising the temperature to 1,000 ° C. while supplying ammonia (NH ₃ ) gas, and then trimethylgallium (TMG) gas, trimethylaluminum (TMA) gas, and monosilane (SiH ₄ ). It can be formed by supplying a gas. In this case, the composition ratio of aluminum and gallium can be 3%: 97%.

The n-type InGaN layer 207b can be formed, for example, by lowering the temperature to 700 ° C. and then supplying trimethylgallium (TMG) gas, trimethylindium (TMI) gas, and ammonia (NH ₃ ) gas. In this case, the composition ratio of indium and gallium can be 2%: 98%.

Examples of the n-type impurity used for the n-type AlGaN layer 207a and the n-type InGaN layer 207b include silicon (Si), selenium (Se), and sulfur (S). These doping concentrations are preferably 5 × 10 ¹⁷ cm ⁻³ or more in the entire n-type diffusion prevention layer 207. When the doping concentration is less than 5 × 10 ¹⁷ cm ⁻³ , magnesium and hydrogen in the p-type cladding layer 209 diffuse into the active layer 206 due to the low concentration of the n-type impurity in the diffusion prevention layer 207. Cannot be effectively prevented. For this reason, the rate of increase in operating current increases, and the degree of degradation increases. On the other hand, the upper limit of the doping concentration can be determined in consideration of the crystallinity of the n-type AlGaN layer 207a and the n-type InGaN layer 207b. Specifically, each of the n-type AlGaN layer 207a and the n-type InGaN layer 207b is preferably set to 5 × 10 ¹⁹ cm ⁻³ or less.

  The thickness of the n-type diffusion prevention layer 207, that is, the total thickness of the n-type AlGaN layer 207a and the n-type InGaN layer 207b is preferably 5 nm or more and 200 nm or less, and preferably 10 nm or more and 150 nm or less. Is more preferable, and 50 nm or more and 100 nm or less is more preferable. When the film thickness of the n-type diffusion prevention layer 207 is thinner than 5 nm, the rate of increase in operating current increases and the degree of deterioration increases. On the other hand, if the film thickness of the n-type diffusion prevention layer 207 is 5 nm or more, the rate of increase in operating current can be reduced, but the operating voltage increases as the film thickness increases. Thickness is preferred.

  According to the configuration of the present embodiment, magnesium and hydrogen can be prevented from moving from the p-type cladding layer to the active layer, as in the first embodiment. Therefore, it is possible to obtain a semiconductor laser element having a lower initial deterioration rate and a longer life than the conventional one.

  In the present embodiment, the example in which the n-type diffusion prevention layer 207 includes two layers, the n-type AlGaN layer 207a and the n-type InGaN layer 207b, has been described. However, the n-type diffusion preventing layer of the present invention is not limited to this, and it is composed of three or more layers as long as it is formed from a compound represented by the formula (2) and is composed of a plurality of layers. Also good.

  In this embodiment, an example in which an n-type impurity is doped in any of the layers forming the n-type diffusion prevention layer 207 has been described. However, the present invention is not limited to this, and it is only necessary that at least one of the layers forming the n-type diffusion prevention layer is doped with an n-type impurity. For example, the n-type diffusion prevention layer may be composed of an n-type AlGaN layer and an undoped InGaN layer. Even with such a configuration, it is possible to prevent magnesium and hydrogen from moving from the p-type cladding layer to the active layer, so that a semiconductor laser device having a longer initial lifetime and a longer lifetime than the conventional one can be obtained. .

  In this embodiment, the p-type electron barrier layer is provided between the n-type diffusion prevention layer and the p-type cladding layer so as to be in contact with the n-type diffusion prevention layer. In the present invention, the p-type electron barrier layer is not necessarily provided, but the provision of the p-type electron barrier layer further effectively suppresses diffusion of magnesium and hydrogen from the p-type cladding layer to the active layer. It becomes possible to do.

When providing a p-type electron barrier layer, it is preferable to provide an undoped GaN layer between the n-type diffusion barrier layer and the p-type electron barrier layer. The film thickness of the GaN layer can be about 5 nm, for example. By providing the GaN layer, the blocking effect against overflow of electrons injected into the active layer can be enhanced by the conduction band energy difference (ΔE _c ) between the p-type electron barrier layer and the GaN layer. Therefore, excellent laser characteristics can be obtained even at high temperatures and high outputs. Note that an undoped In _0.02 Ga _0.98 N layer may be used instead of the undoped GaN layer. In this case, since ΔE _c can be further increased, it is possible to further suppress the overflow of electrons.

In the present embodiment, similarly to the first embodiment, an undoped guide layer can be provided between the active layer and the n-type diffusion prevention layer. As the guide layer, for example, an undoped In _0.02 Ga _0.98 N layer having a thickness of 30 nm can be used. By providing the guide layer, light confinement can be improved, and a desired far-field pattern (FFP) can be obtained.

  The present invention is not limited to the above-described embodiments, and various modifications can be made without departing from the spirit of the present invention.

  For example, in each of the above embodiments, the semiconductor laser element has been described as an example. However, the present invention is not limited to this, and the present invention can also be applied to other semiconductor light emitting elements such as a light emitting diode.

2 is a cross-sectional view of the semiconductor laser element in the first embodiment. FIG. It is a figure which shows the result of having conducted the electricity supply test about the semiconductor laser element by Embodiment 1. FIG. FIG. 6 is a diagram showing a result of conducting an energization test on the semiconductor laser device according to the first embodiment while changing the impurity doping concentration in the n-type diffusion prevention layer. It is a figure which shows the result of having conducted the electricity supply test about the semiconductor laser element by Embodiment 1, changing the film thickness of an n-type diffusion prevention layer. FIG. 6 is a cross-sectional view of another semiconductor laser element in the first embodiment. FIG. 6 is a cross-sectional view of another semiconductor laser element in the first embodiment. FIG. 5 is a cross-sectional view of a semiconductor laser element in a second embodiment. FIG. 6 is a diagram showing the concentration profile results of magnesium, hydrogen, and silicon in the depth direction of the semiconductor laser device according to the first embodiment.

Explanation of symbols

101, 201 Semiconductor laser element 102, 202 Substrate 103, 203 n-type GaN layer 104, 204 n-type cladding layer 105, 205 n-type guide layer 106, 206 active layer 107, 207 n-type diffusion prevention layer 108, 208 p-type electrons Barrier layer 109, 209 p-type cladding layer 110, 210 p-type contact layer 111, 211 ridge 112, 212 insulating film 113, 213 opening 114, 214 p-side electrode 115, 215 n-side electrode 116 undoped guide layer 117 undoped GaN layer

Claims (6)

A gallium nitride substrate, an n-type cladding layer formed on the gallium nitride substrate and made of a nitride-based compound semiconductor, an active layer formed on the n-type cladding layer and made of a nitride-based compound semiconductor, In a semiconductor light emitting device comprising a p-type cladding layer formed on the active layer and made of a nitride compound semiconductor,
The p-type cladding layer includes hydrogen and magnesium as impurities,
Al _y Ga _1-x N (where 0 ≦ x <1) is provided between the active layer and the p-type cladding layer.
An n-type diffusion prevention layer made of a nitride compound semiconductor represented by
An undoped InGaN layer is provided between the n-type diffusion prevention layer and the p-type electron barrier layer. The n-type diffusion prevention layer is composed of only one layer, and the doping concentration of the n-type impurity in the layer is 5 × 10 ¹⁷ cm ⁻³ or more and 5 × 10 ¹⁹ cm ⁻³ or less. The semiconductor light emitting device according to claim 1.   The semiconductor light emitting device according to claim 1, wherein the n-type diffusion prevention layer includes a plurality of layers, and at least one of the layers includes an n-type impurity.   4. The semiconductor light emitting element according to claim 1, wherein a thickness of the n-type diffusion prevention layer is 5 nm or more and 200 nm or less.   5. The p-type electron barrier layer made of a nitride compound semiconductor is provided between the undoped InGaN layer and the p-type cladding layer. The semiconductor light emitting element as described.   The undoped guide layer made of a nitride-based compound semiconductor is provided between the active layer and the n-type diffusion barrier layer, according to any one of claims 1 to 5. Semiconductor light emitting device.

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