The present disclosure relates to a semiconductor laser device and a method for manufacturing a semiconductor laser device.
In an edge emitting semiconductor laser device, an important issue is to reduce optical damage on an output facet. The optical damage is caused through the following process. That is, when a defect occurs in the output facet, electrons and holes are coupled via the defect, causing the temperature of the facet to increase, and accordingly, reducing the bandgap of the semiconductor material at the facet, and as a result, light absorption increases. The increase in the light absorption causes a cycle in which the temperature of the facet further increases, the bandgap further decreases, and the light absorption further increases, which may finally cause the semiconductor material to melt.
Forming a window region on the facet by impurity diffusion or hole diffusion is known as a technique to reduce such optical damage (for example, U.S. Pat. No. 5,703,894 and JP 4128898 B2). Since the bandgap near the facet can widen with the window region, light absorption is reduced, and optical damage can be reduced.
In such a semiconductor laser device, occurrence of a disadvantageous event such as a decrease in light output due to the configuration for reducing optical damage is unfavorable.
Therefore, it is desirable to provide a semiconductor laser device having a further improved novel configuration capable of, for example, reducing optical damage, and a method for manufacturing the semiconductor laser device.
In some embodiments, a semiconductor laser device includes: a layered structure in which a first conductivity type cladding layer, an active layer, a second conductivity type cladding layer, and a contact layer are layered in a first direction, the layered structure including a facet in a second direction intersecting the first direction, the facet outputting laser light, a non-window region formed at least in a central portion in the second direction, and a window region formed between the non-window region and the facet, the window region having a bandgap larger than a bandgap of the non-window region; a first electrode electrically connected to the first conductivity type cladding layer; a second electrode that is formed on the contact layer and constitutes a current path through the layered structure with the first electrode; a passivation layer formed on the facet and having a bandgap larger than the bandgap of the window region; and a dielectric reflecting coating configured to cover an opposite side of the passivation layer from the facet.
In some embodiments, provided is a method for manufacturing a semiconductor laser device. The method includes: forming a layered structure in which a first conductivity type cladding layer, an active layer, a second conductivity type cladding layer, and a contact layer are layered in a first direction, the layered structure being formed with a non-window region and a window region adjacent to the non-window region in a second direction intersecting the first direction and having a bandgap larger than a bandgap of the non-window region; cleaving the layered structure in the window region in atmosphere to form a facet in the second direction; purifying the facet in ultra-high vacuum; forming a passivation layer having a bandgap larger than the bandgap of the window region on the purified facet in ultra-high vacuum; and forming a dielectric reflecting coating on an opposite side of the passivation layer from the facet.
In some embodiments, provided is a method for manufacturing a semiconductor laser device. The method includes: forming a layered structure in which a first conductivity type cladding layer, an active layer, a second conductivity type cladding layer, and a contact layer doped with a second conductivity type impurity are layered on a semiconductor substrate in a first direction, the layered structure being formed with a non-window region and a window region adjacent to the non-window region in a second direction intersecting the first direction and having a bandgap larger than a bandgap of the non-window region; cleaving the layered structure in the window region in ultra-high vacuum to form a facet in the second direction; forming a passivation layer on the facet in ultra-high vacuum; and forming a dielectric reflecting coating on an opposite side of the passivation layer from the facet.
The above and other objects, features, advantages and technical and industrial significance of this disclosure will be better understood by reading the following detailed description of presently preferred embodiments of the disclosure, when considered in connection with the accompanying drawings.
Hereinafter, an exemplary embodiment and a modification of the disclosure are disclosed. Configurations of the embodiment and the modification described below, and functions and results (effects) provided by the configurations are examples. The disclosure can be realized by configurations other than those disclosed in the following embodiment and modification. In addition, the disclosure can make it possible to obtain at least one of various effects (including derivative effects) obtained by the configurations.
In the present specification, ordinal numbers are given for convenience to distinguish directions, parts, and the like, and they do not indicate priority or order.
In each drawing, an X direction is represented by an arrow X, a Y direction is represented by an arrow Y, and a Z direction is represented by an arrow Z. The X direction, the Y direction, and the Z direction intersect each other and are orthogonal to each other.
Configuration of Semiconductor Laser Device
As illustrated in
Further, as illustrated in
As illustrated in
As illustrated in
A current path through the layered structure 10 is formed between the lower electrode 21 and the upper electrode 20. The lower electrode 21 is an example of a first electrode, and the upper electrode 20 is an example of a second electrode. The n-cladding layer 13 is an example of a first conductivity type cladding layer, and the p-cladding layer 17 is an example of a second conductivity type cladding layer.
The semiconductor substrate 11 contains n-GaAs as a material. The n-buffer layer 12 is a buffer layer necessary for growing a layered structure of a high-quality epitaxial layer on the semiconductor substrate 11 and contains n-GaAs as a layer material. The refractive index and the thickness of the n-cladding layer 13 and the n-guide layer 14 are set to realize a free-selected optical confinement state with respect to the layered direction. The n-cladding layer 13 and the n-guide layer 14 contain n-AlGaAs as a layer material. The Al composition of the n-guide layer 14 is desirably 15 [%] or more and less than 45 [%]. The Al composition of the n-cladding layer 13 is typically made higher than the Al composition of the n-guide layer 14 to reduce the refractive index. In a high-power edge-emitting multimode semiconductor laser device including the window region 23 of the present embodiment, the coating thickness of the n-guide layer 14 is desirably 200 [nm] or more, for example, about 400 [nm]. The thickness of the n-cladding layer 13 is desirably 1 [μm] or more, for example, about 3 [μm]. As the n-guide layer 14, a layer that is not intentionally doped may be used, but when the thickness of the n-guide layer 14 is set to 100 [nm] or more, the influence of residual impurities is large, and thus doping is preferably performed. The structure and method of the present embodiment may also be applied to an edge-emitting single-mode semiconductor laser device depending on the application.
The active layer 15 includes a lower barrier layer 15a, a quantum well layer 15b, and an upper barrier layer 15c. The lower barrier layer 15a and the upper barrier layer 15c have a function of a barrier that confines carriers in the quantum well layer 15b, and they contain AlGaAs that is not intentionally doped as a material. The quantum well layer 15b contains InGaAs that is not intentionally doped as a material. The emission recombination energy of the confined carriers is determined depending on the structure of the potential well determined by the In composition and coating thickness of the quantum well layer 15b and the composition of the lower barrier layer 15a and the upper barrier layer 15c. The case where the active layer 15 has a configuration of a single quantum well layer (SQW) has been described here. However, the active layer 15 is not limited thereto, and the layer may have a configuration of a multiple quantum well layer (MQW) in which the quantum well layer 15b, the lower barrier layer 15a, and the upper barrier layer 15c are repeatedly layered a predetermined number of times. In addition, here, the configuration with a layer not intentionally doped has been described, but a donor or an acceptor may be intentionally added to the quantum well layer 15b, the lower barrier layer 15a, and the upper barrier layer 15c. Further, since the lower barrier layer 15a and the n-guide layer 14 may have the same composition, and the upper barrier layer 15c and the p-guide layer 16 may have the same composition, the lower barrier layer 15a and the upper barrier layer 15c do not have to be configured.
The p-guide layer 16 and the p-cladding layer 17 are paired with the n-cladding layer 13 and the n-guide layer 14, and their refractive index and the thickness are set to realize a free-selected optical confinement state with respect to the layered direction. The p-guide layer 16 and the p-cladding layer 17 contain p-AlGaAs as a layer material. The Al composition of the p-guide layer 16 is about 20 [%]. The Al composition of the p-cladding layer 17 is typically set higher than the Al composition of the p-guide layer 16. In addition, to reduce the waveguide loss by shifting the optical field in the layer in the direction of the n-cladding layer 13, the Al composition of the p-cladding layer 17 is set slightly higher than that of the n-cladding layer 13. The Al composition of the p-guide layer 16 is set to be lower than the Al composition of the p-cladding layer 17.
In a high-power edge-emitting multimode semiconductor laser device including the window region 23 as in the present embodiment, the coating thickness of the p-guide layer 16 is desirably 200 [nm] or more, and the thickness of the p-cladding layer 17 is desirably about 1 to 2 [μm]. As the p-guide layer 16, a layer that is not intentionally doped may be configured, but when the thickness of the guide layer is set to be thick, the influence of conductivity fluctuation due to residual impurities is large, and thus intentional doping is preferably performed to enhance manufacturing reproducibility. The p-cladding layer 17 is formed of an n-type semiconductor layer. Since the p-contact layer 18 needs to be in contact with an electrode to inject holes into the active layer 15, the p-contact layer is doped with a p-type impurity at a high concentration. A current confinement layer that narrows the injection current and increases the current density in the active layer 15 may be formed in the p-cladding layer 17.
In the semiconductor laser device 1 of the present embodiment, the current injected from the upper electrode 20 and the lower electrode 21 concentrates on a part of the active layer 15 because of the ridge 6 formed by processing a part of the layered structure 10, and the laser light 4 is extracted to the outside of the semiconductor laser device 1. Since the light density of the laser light 4 radiated from a radiation region 5 (see
In the window region 23, at least a part of the semiconductor layer constituting the layered structure 10 of the window region 23 is alloyed. In
Impurities or holes are diffused in the window region 23. The impurity is, for example, at least one of Zn, Si, and Mg. The length of the window region 23 in the X direction is typically about several μm in the case of impurity diffusion and about several 10 μm in the case of hole diffusion.
In the present embodiment, a passivation layer 30 is formed by layering a material having a bandgap larger than that of the window region 23 on the facet 10a where the window region 23 is formed through facet growth. The passivation layer 30 is a layer having a bandgap larger than that of the window region 23, which makes it possible to further improve the effect of reducing optical damage.
In the present embodiment, the low reflecting coating 3 as a dielectric reflecting coating is provided to cover an opposite side of the passivation layer 30 from the facet 10a.
There is conventionally known a semiconductor laser device in which an alloyed region (window region) is formed by impurity diffusion at an end portion in the X direction of the layered structure 10, and a dielectric reflecting coating is further formed on a facet in the X direction of the alloyed region without forming a passivation layer as in the present embodiment. In this configuration, since an optical loss occurs in the alloyed region, it is difficult to lengthen the alloyed region in the X direction. Accordingly, the length in the X direction of the active layer adjacent to the center side in the X direction with respect to the alloyed region becomes long, and an interval where no current flows is generated in the active layer, the section being adjacent to the alloyed region. In such an interval where no current flows, light is absorbed, which causes a decrease in light output and an increase in energy loss.
In addition, there is conventionally known a semiconductor laser device in which a passivation layer is formed without forming a window region at an end portion of an active layer in an X direction. In this configuration, since a current cannot flow through the interface between the passivation layer and the active layer, it is necessary to provide an interval where no current flows in the active layer, the interval being adjacent to the passivation layer. As described above, in such an interval where no current flows, light is absorbed, which causes a decrease in light output and an increase in energy loss.
In this regard, the present embodiment, in which the non-window region 24, the window region 23, the passivation layer 30, and the low reflecting coating 3 are formed in this order in the X direction as illustrated in
Manufacturing Method
In S11, the plurality of bars 101 each including the layered structure 10, the window region 23, and the non-window region 24 described above are formed on the wafer (wafer piece 100) by a known semiconductor process. In other words, the layered structure 10, the window region 23, and the non-window region 24 are collectively formed for the plurality of bars 101 by being formed with respect to the wafer (wafer piece 100).
The window region 23 is formed in such a manner to extend in the Y direction having a substantially constant width w in the X direction with respect to the wafer piece 100 about a position (virtual line PL) where a scribe 100a (scratch) is provided. The line PL is a position to be an end portion of each bar 101 in the longitudinal direction in the subsequent step S12.
As illustrated in
As illustrated in
As illustrated in
The passivation layer 30 is a layer substantially lattice matched with the layered structure 10. The passivation layer 30 is formed by epitaxial growth. As described above, the layered structure 10 is made of a GaAs-based semiconductor material. Correspondingly, the passivation layer 30 contains, for example, a III-V compound such as GaAs or a II-IV compound such as ZnSe as a layer material (semiconductor material).
The passivation layer 30 is formed in a facet growth chamber 1003 (see
In the example of
When the passivation layer 30 containing a ZnSe compound as a II-IV compound is formed, the molecular beam generator 1031 may be realized by using, for example, a Knudsen cell. In this case, the molecular beam generator 1031 generates a molecular beam of Zn and low molecular weight Se from a ZnSe compound raw material held therein and irradiates the facets 10a of the plurality of arrays 102 with the molecular beam. This causes a ZnSe coating to form on the facets 10a through epitaxial growth. Since the rate of epitaxial growth is determined by the element with a lower molecular beam intensity among the constituent elements of the molecular beam, a high-quality ZnSe coating can be obtained even in epitaxial growth using one molecular beam generator 1031.
In the example of
When the passivation layer 30 containing a ZnSe compound as a II-IV compound is formed, the two molecular beam generators 1031 may be realized using a Knudseng cell or a valved cell. As an example, one molecular beam generator 1031 generates and emits a molecular beam of Zn, and the other molecular beam generator 1031 generates and emits a molecular beam of Se. This causes a ZnSe coating to form on the facets 10a through epitaxial growth. The molecular beam generator 1031 that emits a molecular beam of Sn is preferably realized using a valved cracking cell to reduce the molecular weight of Se.
The combination of the two molecular beam generators 1031 in the case of forming the passivation layer 30 containing a ZnSe compound is not limited to the above-described combination, and various settings may be taken. For example, one molecular beam generator 1031 may emit a molecular beam of ZnSe, and the other molecular beam generator 1031 may emit a molecular beam of either Zn or Se. The two molecular beam generators may each emit a molecular beam of ZnSe.
When the passivation layer 30 containing a ZnSe compound is formed, the facet 10a may be first irradiated with only a molecular beam of Zn from the molecular beam generator 1031. This configuration can reduce the occurrence of through transition at the interface between the layered structure 10 made of a GaAs-based semiconductor material and the passivation layer 30 containing a ZnSe compound and can further improve the reliability of the semiconductor laser device 1.
When the passivation layer 30 containing a GaAs compound as a III-V compound is formed using two molecular beam generators 1031, one molecular beam generator 1031 emits a molecular beam of Ga, and the other molecular beam generator 1031 emits a molecular beam of As. In this case, as an example, the molecular beam generator 1031 that emits a molecular beam of Ga may be realized by using a Knudsen cell, and the molecular beam generator 1031 that emits a molecular beam of As may be realized by using a valved cracking cell. The irradiation of a molecular beam from the molecular beam generator 1031 forms a GaAs coating on the facet 10a through epitaxial growth.
Using a plurality of molecular beam generators 1031 can reduce variations in the components and the thickness of the passivation layer 30 depending on the position of the facet 10a as compared with the case where the molecular beam generator 1031 is used. The number of molecular beam generators 1031 is not limited to two, and the number may be three or more.
The passivation layer 30 is formed on the facets 10a in the X direction of the arrays 102 and is also formed on the facets 10a in the direction opposite to the X direction of the arrays 102. To form the passivation layer 30 on both facets 10a, a support device 1032 is equipped with, for example, a turntable that can rotate at least 180° around a central axis C extending in the Z direction.
As illustrated in
In this manner, in the present embodiment, the passivation layer 30 having a larger bandgap than that of the window region 23 is formed on the facet 10a provided in the window region 23, and the low reflecting coating 3 (dielectric reflecting coating) is formed on an opposite side of the passivation layer 30 from the facet 10a.
According to such a configuration and method, an interval where no current flows in the active layer 15 can be shortened or eliminated, for example, and thus it is possible to reduce or avoid occurrence of a disadvantageous event such as a decrease in light output or an increase in energy loss due to a presence of an interval where no current flows in the active layer 15 in the conventional structure. That is, the present embodiment can make it possible to obtain the semiconductor laser device 1 having further improved novel configuration capable of reducing optical damage, and a method for manufacturing the semiconductor laser device 1.
In addition, a gate valve 1005 that opens and closes between the chambers and hermetically seals the chambers in a closed state is provided between the chambers. The manufacturing apparatus 1000 is provided with a conveyance mechanism 1006 that conveys the wafer piece 100 and the arrays 102 between the chambers. The conveyance mechanism 1006 may be configured as, for example, a conveyance trolley, a conveyance arm, or the like.
The load lock chamber 1001 includes an opening/closing door (not illustrated). In the load lock chamber 1001, loading of the wafer piece 100 and unloading of the arrays 102 are performed.
In the cleaving chamber 1002, cleaving (S12) as illustrated in
The facet growth chamber 1003 is an epitaxial growth device. In the facet growth chamber 1003, the passivation layer 30 as illustrated in
In the coating chamber 1004, the low reflecting coating 3 and the high reflecting coating 2 are formed (S15). In the present modification, the facet growth chamber 1003 and the coating chamber 1004 are connected to each other, but the disclosure is not limited thereto, and the facet growth chamber 1003 and the coating chamber 1004 may be independent from each other. In this case, between the facet growth chamber 1003 and the coating chamber 1004, the arrays 102 may be exposed to atmosphere.
Although the embodiment and the modification of the disclosure have been exemplified above, the embodiment and the modification are merely examples, and are not intended to limit the scope of the disclosure. The above-described embodiment and modification can be implemented in various other forms, and various omissions, substitutions, combinations, and changes can be made without departing from the gist of the disclosure. In addition, specifications (structure, type, direction, model, size, length, width, thickness, height, number, arrangement, position, material, and the like) of each configuration, shape, and the like can be appropriately changed and implemented.
For example, the semiconductor laser device does not have to include a ridge.
The disclosure can be used for a semiconductor laser device and a method for manufacturing a semiconductor laser device.
The disclosure makes it possible to obtain a semiconductor laser device having a further improved novel configuration capable of, for example, reducing optical damage, and a method for manufacturing the semiconductor laser device.
Although the disclosure has been described with respect to specific embodiments for a complete and clear disclosure, the appended claims are not to be thus limited but are to be construed as embodying all modifications and alternative constructions that may occur to one skilled in the art that fairly fall within the basic teaching herein set forth.
Number | Date | Country | Kind |
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2021-052700 | Mar 2021 | JP | national |
This application is a continuation of International Application No. PCT/JP2022/003663, filed on Jan. 31, 2022 which claims the benefit of priority of the prior Japanese Patent Application No. 2021-052700, filed on Mar. 26, 2021, the entire contents of which are incorporated herein by reference.
Number | Date | Country | |
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Parent | PCT/JP2022/003663 | Jan 2022 | US |
Child | 18468800 | US |