Lasers that operate at high temperatures are in demand for many applications in telecommunications since packaging and operating costs are lower for lasers that can operate at high temperatures. Distributed feedback (DFB) lasers which contain Al(In,Ga)As in the active region have shown promise for high-temperature applications due to their relatively stable threshold current and efficiency over a wide temperature range. This behavior is described in publications such as T. J. Houle, et al, “A detailed comparison of temperature sensitivity of threshold for InGaAsP/InP, AlGaAs/GaAs, and AlInGaAs/InP lasers,” CLEO, CTuO1, Baltimore, Md., 2001; J. Piprek, et al, “What limits the maximum output power of long-wavelength AlGaInAs/InP laser diodes?” IEEE J. Quantum Electron. 38, 1253 (2002); and J. C. L. Yong, et al, “1.3-mm quantum-well InGaAsP, AlGaInAs, and InGaAsN laser material gain: A theoretical study,” IEEE J. Quantum Electron. 38, 1553 (2002).
Many semiconductor lasers, including DFB lasers and distributed Bragg reflector (DBR) lasers, contain a grating. This grating provides periodic reflections, either through all or a portion of the laser cavity or external to the laser cavity. The properties of the grating influence many properties of the laser including the efficiency, threshold current, operating wavelength and resistance to external perturbations. It is not unusual for DFB lasers in telecommunications applications to have gratings with periods as low as 200 nm, with feature sizes less than 100 nm.
There are two types of DFB lasers, namely index-coupled and gain-coupled. In index-coupled lasers, the grating is adjacent to the active region which is the material that emits the light. Because the grating doesn't enter the active region, the active region is not physically modified by the index-coupled grating, and therefore no etching or overgrowth is performed within the active region. One of the disadvantages of index-coupled DFB lasers is that their performance is heavily influenced by the position of the front and the rear facets with respect to the grating. In manufacturing, it is not possible to control this phenomenon, facet phase, in order to maximize yields. Furthermore, even when favorable facet phase is achieved, whether by accident or design, index-coupled lasers are sensitive to perturbation from reflections from other components in their packaging. Compared to DFB lasers with gain-coupled gratings, they can also have relatively slow response times. Despite these disadvantages, in research, manufacturing, and deployment in the telecommunications industry, most emphasis to date has been on index-coupled DFB lasers due to their ease of fabrication.
In gain-coupled DFB lasers the grating extends into the active region of the device. The grating's periodic interruption of the active region favors one mode of operation, the right-Bragg mode, and reduces sensitivity to the position of the facets with respect to the grating. This reduced sensitivity to facet phase improves the manufacturing yield of the laser. Furthermore, the gain-coupling makes the laser more resistant to external perturbation than an index-coupled laser, making it cheaper to package the laser with other optical components.
One of the least expensive ways to put a signal on a laser beam is to turn the source laser on and off at high speeds. This direct modulation is often cheaper than paying for a laser and a separate external modulator. In DFB lasers, the maximum effective modulation frequency is related to the relaxation oscillation frequency of the laser, which is the frequency at which the average small-signal modulation output power is maximized. Increasing the relaxation oscillation frequency increases the speed at which the laser can be directly modulated. Gain-coupled gratings increase the relaxation oscillation frequency by increasing the differential gain of the active region. This is another reason that there is an increasing demand for DFB lasers with gain-coupled gratings.
Distributed-feedback lasers with gain-coupled gratings are manufactured by growing semiconductor materials that comprise the active region onto a substrate wafer using an epitaxial technique such as metal-organic chemical-vapor deposition (MOCVD), molecular-beam epitaxy (MBE), chemical-beam epitaxy (CBE), or liquid-phase epitaxy (LPE). The grating is etched into the active region, and then the wafer is returned to the epitaxial reactor to cover the grating with additional semiconductor material. In conventional manufacturing techniques, the active region is exposed to the atmosphere before the overgrowth stage and the active region is exposed where the gain-coupled grating penetrates into the active region.
It is relatively straightforward to make the grating in an index-coupled laser with an active region containing semiconductor material that readily oxidises using known methods in the art. Conventional manufacturing techniques can be applied because the index-coupled grating doesn't extend into the active region and the etching of the grating can be terminated prior to reaching the active region, thereby not exposing the active region to the atmosphere. However, as described above, gain-coupled gratings are desired to reduce sensitivity to facet phase in the manufacturing process, increase resistance to external perturbations, and increase relaxation oscillation frequency by increasing differential gain. Therefore making gain-coupled gratings in active regions containing materials that readily oxidise, for example aluminum, is a challenge.
For example, materials from the Al(In,Ga)As material system, such as AlInAs, AlInGaAs, AlGaAs, and AlAs, oxidise readily when exposed to air. The oxide is very difficult to remove, and even if it could be removed, there would be a loss of resolution of the small features in the grating. This is a particular problem when making a gain-coupled distributed feedback laser where aluminum-containing materials are used in the active region. A grating that is etched in the conventional manner will oxidise before it can be installed in the MOCVD reactor for growth of the topside epitaxial layers. This oxide results in poor electrical, thermal, and physical properties of the material at the grating interface and as such results in a severe impact on chip performance and reliability.
Research groups in Asia and Europe have etched gratings into aluminum-containing materials, exposed the grating to ambient atmosphere, and then attempted to clean off or passivate the resulting oxide prior to the next epitaxial growth. For example, Chen et al., in their publication “A novel 1.3 μm high T0 AlGaInAs/InP strained-compensated multi-quantum well complex-coupled distributed feedback laser diode,” Jpn. J. Appl. Phys., 1999, describe their attempt to passivate a surface of AlInAs using an etch in sulphuric acid. They attribute unfavorable device results, including high threshold current and low slope efficiency to non-radiative recombination at the resulting, imperfect, grating regrowth interface. Another research group, Kunzel et al., in their publication “MBE regrowth on AlGaInAs DFB gratings using in-situ hydrogen radical cleaning,” J. Crystal Gr, 1997, used reactive hydrogen radicals in an MBE system to clean a growth interface prior to growth. They demonstrate that the resulting material exhibits a PL intensity nearly 10-times lower than a structure grown without a regrowth interface, which is an indication of non-radiative recombination at the regrowth interface. Furthermore, their technique has not been demonstrated in an MOCVD reactor, the epitaxial technique that is overwhelmingly favored in the industry. Existing art has been of academic interest, since these results do not meet current standards for products in telecommunication applications; there is insufficient control of grating morphology in addition to little control of material quality at the growth interface.
An existing approach to reduce contamination at a growth interface, while achieving good etch control, is in-situ etching. In-situ etching is etching inside a reactor that is conventionally used for epitaxial growth, such as a reactor for MBE, CBE, or MOCVD. After etching, the same reactor can be used to grow a semiconductor material on top of the etched surface. For example, Knight in U.S. Pat. No. 5,869,398 has shown that InP may be etched in an MOCVD reactor and then additional InP may be grown on the etched surface without exposing the surface to atmosphere. This in-situ etch and overgrowth procedure reduced the levels of silicon and oxygen contamination at the growth interface compared to samples that did not receive in-situ etching prior to overgrowth. A limitation of this approach is that conventional methods of defining the pattern to be etched are not suitable. With conventional methods of defining the pattern to be etched, the sample must be removed from the reactor to remove the mask material. For example, if a pattern were defined in photoresist or dielectric (such as SiO2 or SiNx), the wafer would have to be removed from the reactor to strip this masking material, exposing the etched surface to contamination.
Therefore there is a need for a suitable method for etching gratings into semiconductor material that readily oxidises.
This background information is provided for the purpose of making known information believed by the applicant to be of possible relevance to the present invention. No admission is necessarily intended, nor should be construed, that any of the preceding information constitutes prior art against the present invention.
An object of the present invention is to provide a method for manufacturing gratings in semiconductor materials that readily oxidise. In accordance with an aspect of the present invention, there is provided a method for manufacturing a grating pattern in one or more layers of semiconductor material that readily oxidises, the method comprising the steps of: forming a protective layer on top of the one or more layers, the protective layer formed from a semiconductor material and providing protection to the one or more layers; forming a grating pattern in a semiconductor material grown on the protective layer, thereby forming a semiconductor grating mask; transferring the grating pattern into the one or more layers using in-situ etching in an epitaxial growth reactor; and overgrowing semiconductor material on the one or more layers prior to removal from the epitaxial growth reactor.
In accordance with another aspect of the present invention there is provided a semiconductor device comprising: one or more layers of semiconductor material that readily oxidises, said one or more layers having a grating pattern etched therein; a protective layer on the one or more layers, said protective layer having the grating pattern therein; an overgrowth layer of semiconductor material grown on the protective layer, said overgrowth layer encapsulating the grating pattern in the one or more layers.
The present invention provides a method of manufacturing gratings in semiconductor material that readily oxidises. The method is suitable for a wide range of applications, and is particularly appropriate for fabricating gratings for distributed feedback lasers, gratings for distributed Bragg reflectors, and filters based on optical waveguides with grating structures, for example. The invention provides an improved accuracy of the grating depth and shape, and a reduction in contaminants and oxidants within the gratings etched into the semiconductor material that readily oxidises, with consequent improved performance and manufacturing repeatability thereof, for example.
The present invention is a combination of in-situ etching with a grating mask pattern comprised only of semiconductor material, together with the fabrication of a protective layer beneath the semiconductor grating mask that protects the semiconductor material that readily oxidises. As such the present invention is based on a two-stage process. First the grating pattern is defined in a semiconductor material, wherein this pattern is called the semiconductor grating mask. The semiconductor grating mask sits on top of a layer of protective material, which in turn is on top of the semiconductor material that readily oxidises, wherein the protective layer prevents oxidation of the material below. The semiconductor structure is then moved to a reactor, where, in the second stage, the mask pattern is transferred into the underlying protective layer and the semiconductor material that readily oxidises, by in-situ etching. The grating is then overgrown in the same reactor without exposing the etched grating to the atmosphere. The overgrown material protects the underlying semiconductor material from oxidation when the structure is removed from the reactor.
The protective layer between the semiconductor grating mask and the semiconductor material that readily oxidises, protects this material from oxidation until the protective layer is pierced during the in-situ etching process. The semiconductor grating mask and the protective layer are partially etched, or entirely etched away, during in-situ etching, wherein the material that remains is incorporated into the finished structure during the overgrowth stage. This incorporation of the masking and protective material into the final structure means that the structure doesn't have to be removed from the reactor between etching and overgrowth in order to remove the masking material. When the semiconductor material that readily oxidises is exposed after the in-situ etching process, the structure is in an environment that precludes oxidation until the overgrown material seals in this semiconductor material in the subsequent step.
The combination of the semiconductor material grating mask together with in-situ etching and overgrowth additionally allows the formation of gratings on a semiconductor with minimal contamination. As such, there is no need to compensate for n-type doping from the contamination by addition of excessive p-type dopants and thereby increasing the optical absorption of the waveguide. This invention has the added benefit of providing exceptional grating depth uniformity over a full wafer, and process repeatability.
In addition the present invention can provide a means for overcoming the difficulties with creating a grating in the active region of a semiconductor laser wherein this active region comprises semiconductor material that readily oxidises.
The present invention is suitable for manufacturing a wide range of grating structures, provided a semiconductor material grating mask and a protective layer can be produced. Suitable grating structures include regularly-spaced corrugations, such as those found in a conventional DFB laser, variable-spaced corrugations, such as those found in devices containing a chirped grating, and more complicated groups of corrugations, such as those found in devices containing a distributed Bragg reflector.
The invention is appropriate for the manufacturing of a grating in a variety of semiconductor materials, but it is of greatest benefit for materials that oxidise readily when exposed to air, for example materials of a Al(In,Ga)As type compound such as AlInGaAs, AlGaAs, and AlInAs. The invention is suitable for making gain-coupled gratings into active regions comprised of multiple quantum-well/quantum-barrier stacks of various In(Ga,As)P and Al(In,Ga)As materials. While the present invention is described such that the semiconductor material that readily oxidises contains aluminum, the invention is suitable for any material that readily oxidises, wherein this material can provide a desired effect on the functionality of the semiconductor laser. In addition, embodiments of the present invention describe the use of this manufacturing method enabling the creation of gratings in the active region of a semiconductor laser, however other layers of the semiconductor laser may comprise semiconductor materials that readily oxidise and require a grating structure therein. As such these other layers can equally be manufactured using the method according to the present invention.
One embodiment of the current invention is depicted in
The structure represented in
The structure represented in
Without removing the wafer from the reactor, semiconductor material from the In(Ga,As)P or Al(In,Ga)As or other suitable semiconductor material system that is compatible with the substrate and other semiconductor layers, labeled as layer 40, is grown on top of the patterned layers 10′ and 20′ to yield the structure represented in
A further aspect of the invention is the means of forming the semiconductor grating mask, illustrated by layer 30′ in
Conventional means are used to create a grating pattern in a masking material on top of layer 30, as represented by layer 50 in
In one embodiment of the invention, layer 10 is the active region of a DFB laser. The active region comprises a quantum-well/quantum barrier stack including materials from the Al(In,Ga)As and In(Ga,As)P material systems. In this embodiment, layer 20 is a 5-nm thick layer of InP that protects the underlying active region from oxidation. In this embodiment, layer 30 is a 50-nm thick layer of InGaAs. It will be obvious to workers skilled in the art that other layer thicknesses and materials could be applied to the same conceptual process, and such other thicknesses and materials are within the scope of this invention. In this embodiment of the invention, the material grown in layer 40 is the same composition as the material in layer 20′, and as such layers 40 and 20′ are virtually indistinguishable.
In one embodiment of the invention, the etch that patterns layer 30 of
Other embodiments of the invention are possible wherein the etchant that patterns layer 30 self-terminates when it reaches layer 20. In such an embodiment there is no need to stop etching when the structure resembles that illustrated in
In one embodiment of the invention, the masking material in layer 50 is a dielectric material, for example silicon oxide, silicon nitride or silicon oxynitride, wherein this dielectric may be patterned using methods known in the art. For example, it can be etched in a plasma etch process or a wet etch process using a photoresist mask. The photoresist can be patterned holographically, which is a technique well known in the art. Those skilled in the art will appreciate that any other suitable lithography process may be used to create the photoresist grating mask, including electron-beam lithography, near-field holography, and nano-imprint lithography. Those skilled in the art will recognize that the grating pattern defined in layer 50 may be a uniform corrugation, or it may include phase jumps, chirped periods, or patches of gratings, and that in cases where the grating pattern is irregular, electron-beam lithography would be a favorable means of patterning the photoresist.
In one embodiment of the invention the in-situ etching and overgrowth is conducted in an MOCVD reactor. It will be obvious to a worker skilled in the art that application of other epitaxial growth technologies is possible, including chemical-beam epitaxy (CBE), molecular-beam epitaxy (MBE) and liquid-phase epitaxy (LPE). A key part of this process is the control of the physical depth of the transfer of the pattern into layer 10, wherein the etch rate is dependent on the materials being etched, the etchant, the etchant flux and the temperature. In one embodiment of the invention, the transfer of the grating pattern from layer 30′ to layer 10 is accomplished with in-situ etching using HCl. It would be obvious to a worker skilled in the art that other halogen-containing compounds would be suitable etchants, including, but not limited to methyl chloride, tertiarybutyl chloride, hydrogen iodide, diiodomethane, triiodomethane, carbon tetraiodide, iodoethane, n-propyl iodide and isopropyl iodide. However, HCl is used in this embodiment because it etches Al(In,Ga)As compounds, and it etches the InP protective layer, while it does not etch InGaAs too quickly. As would be readily understood, the control of the temperature and other parameters is critical to the accuracy of the depth of the grating that is etched into the active layer comprising semiconductor material that readily oxidises.
After the processing steps described in this invention are complete the semiconductor structure will be processed by conventional means to complete the device fabrication.
As illustrated in the Figures, the sizes of layers or regions are exaggerated for illustrative purposes and, thus, are provided to illustrate the general structures of the present invention. Various aspects of the present invention are described with reference to a layer or structure being formed on a substrate or other layer or structure. As will be appreciated by those of skill in the art, references to a layer being formed “on” another layer or substrate contemplates that additional layers may intervene.
In addition it would be readily understood by a worker skilled in the art that while the Figures illustrate a particular number of layers, each of these identified layers can be formed by a plurality of layers depending on the targeted application.
The invention being thus described, it will be obvious that the same may be varied in many ways. Such variations are not to be regarded as a departure from the spirit and scope of the invention, and all such modifications as would be obvious to one skilled in the art are intended to be included within the scope of the following claims.
This application incorporates by reference and claims priority from Provisional Patent Application, Ser. No. 60/516,408, Filed Oct. 31, 2003. The present invention pertains to the field of semiconductor lasers, and in particular to the method of manufacturing gratings in semiconductor materials that readily oxidise.
Number | Date | Country | |
---|---|---|---|
60516408 | Oct 2003 | US |