The present application claims priority from Japanese patent application serial no. 2005-074991, filed on Mar. 16, 2005, the content of which is hereby incorporated by reference into this application.
1. Field of the Invention
The present invention relates to an optical semiconductor element, a method of manufacturing the optical semiconductor element, and an optical module which are able to use in the field of optical communications and so on.
2. Description of the Related Art
As optical communications systems have increased in speed and functionality in recent years, semiconductor lasers with high wavelength stability have been demanded as the light sources of the systems. Semiconductor lasers for communications are distributed feedback (DFB) lasers having an excellent single wavelength property.
DFB lasers have an excellent single wavelength property because an oscillation wavelength is defined by a diffraction grating provided in a laser structure. In a buried heterostructure DFB laser, a multilayer structure for laser oscillation is formed by crystal growth, and then a diffraction grating pattern which is periodically stepped is formed on an upper guide layer by an interference exposure apparatus and wet etching. A p-type InP clad layer and a contact layer undergo crystal growth so as to fill in periodic steps, and then a mesa stripe serving as an optical waveguide is formed by etching. The side of a semiconductor mesa and an end region are filled with an semi-insulating compound semiconductor. In this structure, a diffraction grating layer having a thickness of several tens nm is formed on a surface of the upper guide layer by wet etching. Wet etching, however, has poor controllability in the depth direction, thereby degrading laser characteristics including an optical output, a threshold current, and a slope efficiency (inclination of optical output power vs current curve) which are variables of the thickness of the diffraction grating.
As a structure for improving the depth control of a diffraction grating layer, a floating diffraction grating is available in which an InP layer serves as an etching stop layer under the diffraction grating layer. JP-A No. 2004-179274 describes that the structure of a floating diffraction grating can provide stable element characteristics with no variations in the depth direction.
However, when a p-type InP clad layer is grown, an InGaAsP layer serving as a diffraction grating and an InP layer serving as an etching stop layer are different from each other in the solid solubility of p-type dopant. Thus, in the structure described in JP-A No. 2004-179274, the amount of thermal diffusion of the dopant to the vicinity of an active layer tends to depend on an aperture width or the presence or absence of a diffraction grating. The amount of thermal diffusion affects element characteristics such as an optical output power, a threshold current, and slope efficiency. Consequently, an optical semiconductor element described in JP 2004-179274 A includes factors that may reduce the manufacturing yield of the optical semiconductor element.
An optical semiconductor element has an InGaAsP thin film layer inserted between a p-type InP clad layer and a diffraction grating composed of an InGaAsP layer. In this structure, a diffusion prevention layer having a high solid solubility of p-type dopant is present over an active layer. Thus, the amount of thermal diffusion of the dopant to the vicinity of the active layer does not depend on an aperture width or the presence or absence of a diffraction grating when the p-type InP clad layer is grown, thereby obtaining a stable optical output power, a threshold current, and slope efficiency.
Preferred embodiments of the present invention will now be described in conjunction with the accompanying drawings, in which:
Referring to the accompanying drawings, embodiments of the present invention will be described below in accordance with the following examples. The same members are indicated by the same reference numerals and a repeated explanation thereof is omitted.
Referring to
Referring to
Thereafter, a p-type InP clad layer 8, a contact layer 9, and an InGaAsP thin film layer 16 almost identical in composition to the InGaAsP layer 6 are epitaxially grown by MOCVD so as to fill in the periodic steps.
In the process of epitaxial growth, the substrate is entirely heated to about 600 ° C., and thus thermal diffusion of dopant occurs from the p-type InP clad layer 8. However, since the InGaAsP layer 3 having a high solid solubility of dopant is present over the active layer, the amount of thermal diffusion of dopant does not depend on an aperture width or the presence or absence of a diffraction grating. Consequently, it is possible to obtain a stable optical output power, a threshold current, and slop efficiency.
Subsequently, to form a semiconductor mesa acting as an optical waveguide, a mesa stripe structure is formed by wet etching using Br-methanol etchant. An SiO2 film (not shown) having been formed by CVD with a thickness of 300 nm is used as a mask. The mesa strip structure has a reversed-mesa shape with an active layer having a width of 2 μm. Thereafter, SiO2 is removed and an SiO2 film (not shown) is conversely formed on the semiconductor mesa. According to this selective growth using the SiO2 mask, both sides of the semiconductor mesa are subjected to buried growth by a semi-insulating film (Fe-InP) 11 using Fe as dopant.
After the stripe SiO2 film is removed, a passivation film 12 having a thickness of 500 nm is formed over the substrate by CVD. Only the passivation film serving as a current injection region on the semiconductor mesa is opened by photolithography and etching, and a p-side electrode 13 made of Ti/Pt/Au with a thickness of about 1 μm is formed by electron beam (EB) vapor deposition. Then, after the p-side electrode 13 is patterned by ion milling, the back side of the substrate is ground to a thickness of 100 μm, an n-side electrode 14 is formed, and the process of an electrode alloy is performed, in which a semiconductor and a metal are mutually diffused.
After these processes, a wafer is cleaved into a bar having an element length of 200 μm, a reflection protecting film 15 (\\\ in
With the optical semiconductor element of the present example, the threshold current was reduced from 10 mA to 5.0 mA at 25° C. The slope efficiency was increased from 0.2 W/A to 0.33 W/A. Further, the maximum optical output power was increased by 66%.
The optical semiconductor element of the present example dramatically improved the manufacturing yield of the semiconductor laser. The manufacturing yield is affected by thermal diffusion of dopant in a crystal growth process.
In this case, the material of the active layer is InGaAsP. The material may be InGaAlAs and is not particularly limited. In the present example, the InGaAsP diffraction grating and thin film layer are used. As a matter of course, an InxGa(1−x)AsyP(1−y) (0≦x≦1, 0≦y 1) crystal may be used. The present example described a buried heterostructure and is also applicable to a ridge waveguide structure.
The above example described a semiconductor laser. An electro absorption/distributed feedback (EA/DFB) laser is also applicable. The lasers both have optical semiconductor elements.
The InGaAsP thin film layer 16 is acceptable when the thin film layer 16 has almost the same index of refraction as the InGaAsP layer 6. The InGaAsP thin film layer 16 is a diffusion prevention layer for preventing the dopant of the p-type InP clad layer from thermally diffusing to the active layer. The above modification is applicable to the other examples of this specification.
Referring to
Referring to
Thereafter, a p-type InP clad layer 8, a contact layer 9, and an InGaAsP thin film layer 16 having almost the same index of refraction as the refraction grating layer are epitaxially grown by MOCVD so as to fill in the periodic steps.
In the process of epitaxial growth, the substrate is entirely heated to about 600° C., and thus thermal diffusion of dopant occurs from the p-type InP clad layer 8. However, since the InAlAs layer 19 having a high solid solubility of dopant is present over the active layer, the amount of thermal diffusion of dopant does not depend on an aperture width or the presence or absence of a diffraction grating. Consequently, it is possible to obtain a stable optical output power, a threshold current, and slop efficiency.
The contact layer 9 is worked into a stripe structure with a stripe width of 2.0 μm and a groove width of 10 μm on both sides of the stripe. An SiO2 film (not shown) having been formed by CVD with a thickness of 300 nm is used as a mask.
Then, after the SiO2 film is entirely removed, the p-type InP clad layer 8 is selectively etched by wet etching using a mixed solution of hydrochloric acid and phosphoric acid while the contact layer 9 having been worked into the stripe structure is used as a mask, so that a reversed-mesa ridge waveguide is formed.
In the case where the InGaAsP thin film layer 16 is absent, etching is performed on not only the p-type InP clad layer 8 but also on the InP etching stop layer 5 during the formation of the reversed-mesa ridge waveguide, and the etching stops on the p-type InAlAs layer 18. Thus, in the working process, a material containing Al is exposed on a crystal surface. Al is oxidized, a leakage current component is generated through a surface of the oxidized Al, and thus a threshold current increases. In contrast, in the present example, the etching of the p-type InP clad layer 8 stops on the InGaAsP thin film layer 16 and thus the p-type InAlAs layer 19 disposed below the InGaAsP thin film layer 16 is not exposed or oxidized during the manufacturing process. Therefore, it is possible to reduce a threshold current and increase a slope efficiency.
Subsequently, an SiO2 passivation film 12 having a thickness of 500 nm is formed over the substrate by CVD. Only the passivation film serving as a current injection region on the semiconductor mesa is opened by photolithography and etching, and a p-side electrode 13 made of Ti/Pt/Au with a thickness of about 1 μm is formed by EB vapor deposition. After the p-side electrode 13 is patterned (not shown) by ion milling, the back side of the substrate is ground to a thickness of 100 μm, an n-side electrode 14 is formed, and the process of an electrode alloy or the like is performed.
After these processes, a wafer is cleaved into a bar having an element length of 200 μm, a reflection protecting film 15 is formed on a cleavage plane, and then the element is cut into chips.
The semiconductor laser of the present example has an Al ridge structure with excellent laser characteristics at high temperatures, and thus the threshold current was reduced from 22 mA to 16 mA at a high temperature of 85° C. The slope efficiency was increased from 0.15 W/A to 0.2 W/A. Further, the maximum optical output power was increased by 66%.
According to the present example, the threshold current was reduced and the slope efficiency was increased in the semiconductor laser, thereby manufacturing a high-quality optical semiconductor element with a high yield.
The active layer may be made of either InGaAsP or other materials. The InGaAsP thin film layer 16 also acts as a diffusion prevention layer and an etching stop layer.
Referring to
In
The optical module 300 includes a housing (not shown). The input terminal of the optical fiber and optical components mounted on the silicon substrate 23 are housed in the housing.
The optical module of the present example has an Al ridge structure with excellent laser characteristics at high temperatures, and thus a threshold current was reduced from 22 mA to 16 mA at a high temperature of 85° C. A slope efficiency has been increased from 0.15 W/A to 0.2 W/A. Further, the maximum optical output was increased by 66%.
The optical module of the present example has been manufactured at low cost because of the high yield of the semiconductor laser.
The semiconductor laser of the present example may be the semiconductor laser 100 of Example 1 instead of the semiconductor laser 200 of Example 2. In this case, the optical module can reduce the threshold current from 10 mA to 5.0 mA at 25° C. The slope efficiency can be increased from 0.2 W/A to 0.33 W/A. Further, the maximum optical output can be increased by 66%.
According to the present invention, it is possible to dramatically improve the laser characteristics and the manufacturing yield of an optical semiconductor element. The laser characteristics and the manufacturing yield are affected by thermal diffusion of dopant in a crystal growth process.
Number | Date | Country | Kind |
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2005-074991 | Mar 2005 | JP | national |