MOCVD system injector for fast growth of AlInGaBN material

A conical supply tube is provided, along with deposition systems using such a tube and methods of its use. The conical supply tube includes a conical head formed from a hollow structure defining a having a fitting end and an opposite, shower end, with the fitting end has an initial diameter that is less than a diameter at the shower end. A MOCVD chamber is also generally provided that includes such a conical supply tube and a susceptor configured to hold a substrate facing the shower end of the conical supply tube. Methods are provided for growing a group III nitride layer on a surface of a substrate.

BACKGROUND

Group III-nitride and its ternary and quaternary compounds are prime candidates for fabrication of visible and ultraviolet high-power and high-performance optoelectronic devices and electronic devices. These devices are typically grown epitaxially as thin films by growth techniques including molecular beam epitaxy (MBE), metalorganic chemical vapor deposition (MOCVD), or hydride vapor phase epitaxy (HVPE).

In conventional MOCVD, the precursors (such tri-methyl gallium, ammonia etc.) are supplied continuously to the reactant chamber. Growing AlInGaBN requires a very high growth temperature (e.g., about 1000° C. to about 1100° C.). Even higher temperatures are required for growth utilizing relatively large percentages of Al and/or B, such as at growth temperatures of about 1300° C. to about 1450° C. At these extremely high temperatures, however, the precursors tend to combine in the chamber and “rain down” onto the surface of the substrate, effectively forming adduct particles thereon. These adduct formations during MOCVD hampers the subsequent epilayer growths by increasing the number of stacking faults and dislocation density.

A pulsed metal organic chemical vapor deposition (P-MOCVD) or pulsed atomic layer epitaxy (PALE), in which the precursors are supplied with alternative supply of sources, alleviates the above mentioned problem. This alternative or pulsing technique not only suppress the adduct formation but also provides a unique opportunity to bend the dislocation propagation, to deposit monolayers of material thereby decreasing the slip (which is often the reason for stacking fault generation). Thus, P-MOCVD makes an attractive technique for substrate and epilayer growth and device fabrication.

Although the P-MOCVD alleviates some of the potential problems plaguing III-N devices (especially over non-polar substrates and materials) and represents an enabling technology for the growth of non-polar III-N devices, the relatively high defect density in the directly-grown non-polar or semi-polar III-N films reduces the efficiency of subsequently grown devices compared to what could be achieved by homoepitaxial growth on a perfect substrate. In particular, these P-MOCVD systems are more complicated to design and run growth.

Thus, a need exists for a simplified and efficient method and system for high temperature MOCVD growth of AlInGaBN material while suppressing or eliminating adduct formation.

SUMMARY

A conical supply tube is generally provided, along with deposition systems using such a tube and methods of its use. In one embodiment, the conical supply tube includes a conical head formed from a hollow structure defining a having a fitting end and an opposite, shower end, with the fitting end has an initial diameter that is less than a diameter at the shower end. A MOCVD chamber is also generally provided that includes such a conical supply tube and a susceptor configured to hold a substrate facing the shower end of the conical supply tube.

Methods are also provided for growing a group III nitride layer on a surface of a substrate. In one embodiment, the method includes introducing a source gas into the MOCVD chamber though the supply tube of any preceding claim. The supply tube defines a terminal end at a distance of about 1 to about 10 inches from the surface of the substrate, and the MOCVD chamber has a temperature of about 1000° C. to about 1450° C. The source gas comprises at least one of a metal-organic source gas, a boron source gas, or a nitrogen source gas.

Definitions

Chemical elements are discussed in the present disclosure using their common chemical abbreviation, such as commonly found on a periodic table of elements. For example, hydrogen is represented by its common chemical abbreviation H; helium is represented by its common chemical abbreviation He; and so forth.

As used herein, the term “substantially free” means no more than an insignificant trace amount present and encompasses completely free (e.g., 0 molar % up to 0.01 molar %).

DETAILED DESCRIPTION

Reference now will be made to the embodiments of the invention, one or more examples of which are set forth below. Each example is provided by way of an explanation of the invention, not as a limitation of the invention. In fact, it will be apparent to those skilled in the art that various modifications and variations can be made in the invention without departing from the scope or spirit of the invention. For instance, features illustrated or described as one embodiment can be used on another embodiment to yield still a further embodiment. Thus, it is intended that the present invention cover such modifications and variations as come within the scope of the appended claims and their equivalents. It is to be understood by one of ordinary skill in the art that the present discussion is a description of exemplary embodiments only, and is not intended as limiting the broader aspects of the present invention, which broader aspects are embodied exemplary constructions.

Methods are generally provided that increase the growth rate, while maintaining the single crystal material quality for AlInGaBN material, along with apparatus and systems for performing the same. Simply reducing the distance between the injector and the susceptor in a normal MOCVD system creates a significant issue for growth, because of rf-coupling to the metallic top plate. In one embodiment, a modified nozzle injector is generally provided for a MOCVD system. The nozzle injector is configured to introduce the metallic precursor gas(es), such as metal organic gas(es), very close to the susceptor, and thus the growth surface.

Methods are also generally provided for growing extremely low defect density non-polar and semi-polar III-nitride layers over a base layer, and the resulting structures. In particular, an AlInGaBN can be achieved on a non-polar or semi-polar base layer, with little or no defect density, while maintaining uniformity across the AlInGaBN layer and a relatively fast growth rate.

I. Base Layer

According to the present invention, the group III nitride epilayer to be selectively doped can be formed on any suitable non-polar or semi-polar base layer. Suitable base layers can include materials such as but are not limited to, sapphire, silicon carbide, lithium aluminate, spinel, gallium nitride, aluminum nitride, aluminum gallium nitride, indium gallium nitride, aluminum indium gallium nitride, and the like. In one particular embodiment, the base layer is in the form of a substrate. Any suitable non-polar or semi-polar substrate can be used as the base layer to grow the group III nitride epilayer. Although the following description discusses a “substrate”, other types of base layers can be used in accordance with the present invention.

Non-polar substrates generally encompass those grown in a-plane, r-plane, or m-plane. For example, the non-polar substrate can be an m-face or r-plane sapphire substrate such that there is no polarization charge supplied in the device layers of this structure.

Non-polar and semi-polar III-Nitride substrates are of great interest to the nitride semiconductor device community because they enable the deposition of improved device active regions that can be used to realize new and improved high performance optoelectronic and electronic nitride semiconductor devices. Some theoretical predictions believe that non-polar and semi-polar GaN will enable higher quantum efficiencies and improved electrical characteristics for light emitting diodes (LEDs) and laser diodes and will enable the development of very high performance enhancement mode (e-mode) high electron mobility transistors (HEMTs). While such predictions have been partially corroborated by experiment, previous attempts to fabricate devices on non-polar GaN were severely hampered by the presence of very high defect densities in the active regions which had origins in the substrates and which derived from the heteroepitaxial approaches used in the non-native approach to their fabrication.

No matter the starting base layer for forming the substrate, a group III nitride epilayer is grown over the base layer. “Group III nitride” refers to those semiconducting compounds formed between elements in Group III of the periodic table and nitrogen. More preferably the Group III element is selected from the group consisting of aluminum (Al), gallium (Ga), and/or indium (In). Ternary and quaternary compounds (e.g., AlGaN and AlInGaN) are particularly preferred. As is well understood in the art, the Group III elements can combine with nitrogen to form binary compounds (e.g., GaN, AlN and InN), ternary compounds (e.g., AlGaN, AlInN, and GaInN), and quaternary compounds (i.e., AlInGaN).

In one particular embodiment, the methods can be utilized to grow a layer of AlInGaBN. In this embodiment, the group III nitride epilayer can be composed of any combination of group III elements (e.g., Al, In, and Ga), boron, and nitride. In one particular embodiment, the group III-nitride epilayer can be represented by the formula AlxInyGa1-x-yBN, wherein 0≤x≤1, 0≤y≤1 and 0<x+y≤1. In employing growth techniques to grow the group III nitride epilayer, the precursor source gases typically include at least one metal-organic source (e.g., trimethyl aluminum, trimethyl gallium, triethyl gallium, trimethyl indium, triethylalluminum, AlCl, AlCl3or combinations thereof), a boron source (e.g., trimethy boron, triethyl boron), a nitrogen source (e.g., ammonia), a carrier gas (e.g., argon, hydrogen, nitrogen, etc.), and an optionally doping source (e.g., silane, biscyclopentadienyl magnesium, etc.). Of course, other materials can be utilized to grow the group III nitride epilayer, and the present invention is not intended to be limited by the above listed materials. For example, another type of metal-organic source, boron source, and/or nitrogen source can be utilized to grow the group III nitride epilayer.

During MOCVD growth of the group III nitride epilayer, the source gases are supplied in a vapor phase to the growth chamber. Referring toFIGS. 1aand 1b, schematic of exemplary MOCVD growth chambers10are generally shown. The MOCVD growth chamber10includes a susceptor18configured to hold or support a wafer17, as is known in the art. Vacuum line15is configured to control the pressure within the MOCVD growth chamber10, also as known in the art.

InFIG. 1a, multiple supply lines12a,12b,12care shown connected to the MOCVD growth chamber10in order to introduce supply gases therein, with flow controllable via respective supply valves14a,14b,14c, from a respective supply tank (not shown). Each supply line12a,12b,12cis configured to introduce a supply gas generally into the MOCVD growth chamber10, and can be used as purge gases, growth gases, etc. Although shown with three general supply lines12a,12b,12c, any suitable number of supply lines can be utilized within the scope of this invention. Supply line16is shown introducing a supply gas into the internal supply tube20. The internal supply tube20is configured to introduce the supply gas into the MOCVD growth chamber10at a close proximity to the surface19of the wafer17on the susceptor18.

InFIG. 1b, multiple supply lines16a,16b,16care shown connected to the internal supply tube20and are configured to, collectively, introduce multiple supply gases therein. Thus, a mixture of supply gases can be introduce into the MOCVD growth chamber10at a close proximity to the surface19of the wafer17on the susceptor18.

The internal supply tube20can have several configurations, each of which are discussed in greater detail below.

A. Straight Supply Tube

In one embodiment, a straight supply tube20ais generally provided, as shown inFIGS. 2aand 2b, for introducing a supply gas (e.g.,FIG. 1a) or multiple supply gases (e.g.,FIG. 1b) into the MOCVD growth chamber10at a close proximity to the surface19of the wafer17on the susceptor18. The straight supply tube20aincludes a single supply tube22that is substantially straight, and pointing towards the center of the substrate17. A supply head24is attached to the end of the single supply tube22, and defines a substantially flat, straight bar over the surface19of the substrate17. A plurality of apertures25are defined in the bottom surface26of the supply head24, and are configured to supply at least one supply gas21to the surface19of the substrate17.

In some embodiments, however, use of straight supply tube20ahad an issue with excessive velocity of the reactants, and led to hazy centers formed on the surface19. This may be due to a growth rate well above 10 um/hour which may not be sustainable at a temperature range of about 1300° C. to about 1400° C. thereby degrading the crystalline quality.

B. Bent Supply Tube

In another embodiment, a bent supply tube20bis generally provided, as shown inFIGS. 3aand 3b, for introducing a supply gas (e.g.,FIG. 1a) or multiple supply gases (e.g.,FIG. 1b) into the MOCVD growth chamber10at a close proximity to the surface19of the wafer17on the susceptor18. The bent supply tube20bis similar to the straight supply tube20a, described above, but has been modified to a bent tube32that is pointing towards the edges of the substrate17.

The tube32is positioned below a plate34defining apertures35allowing carrier gas33(e.g., ammonia) to flow therethrough and towards the surface17of the substrate19. The supply gas(es)21are carried from the supply line(s)16through the tube32and out of apertures36defined by the tube32in close proximity to the surface17of the substrate16. The flow of the carrier gas33helps to direct the exiting supply gas21from the apertures36onto the surface17of the substrate16.

FIG. 4shows an exemplary cross-section of the bent tube32having a first bend40aand a second bend40b. Collectively, the first bend40aand second bend40bhelp to slow the flow of the supply gas(es) therethrough, which would otherwise be unimpeded in a straight tube. The final bend41curves the end portion of the bent tube32such that apertures36may be directed toward the surface17of the substrate16.

C. Conical Supply Tube

In a preferred embodiment, a conical supply tube20cis generally shown inFIGS. 5aand 5b. The conical supply tube20cincludes a conical head60that has an expanding area62in at least some portion of its length where the average diameter of the conical head60is increasing. Thus, the initial diameter (D1) at the fitting end65of the conical head60is less than the diameter (D2) at the shower end68.

As show, the expanding area62is integral to a tube area61to form the conical head60. In one particular embodiment, the conical head60is a hollow structure attached to a shower plate70that defines a plurality of apertures72such that the supply gas flows through the shower plate70, as shown inFIG. 6. In use, the bottom surface74of the shower plate70can be approximately between 1 to 10 inches from the surface17of the substrate19. It can be positioned anywhere from about ½ inch to all the way where the top steel plate of the chamber is.

The conical head60is, in one embodiment, constructed from quartz so as to avoid affecting the rf-coupling or creating other electrical issues during growth. As such, the conical head60brings the growth species (i.e., the supply gases) closer to the growing surface17and hence adduct formation is severely reduced and the metalorganic incorporation efficiency is significantly higher. It can also be constructed out of ceramics such as BN, AlN or sapphire.

When combined with a higher growth temperatures required for AlInGaBN growth (e.g., about 1000° C. to about 1450° C., such as about 1100° C. to about 1350° C.), growth rates as high as about 0.5 μm per hour to about 10 μm per hour are easily achievable for the AlInGaBN layer growth while maintaining good uniformity.

When constructed from quartz, a steal sealing64can be utilized wherein the quartz tube60exits the fitting66(e.g., a Swagelock fitting) on growth chamber wall to avoid gas leakage around an O-ring or other linkage at the quartz-to-steel connection. Thus, Variable Compression Ratio (VCR) fittings between the quartz tube and the steel tube can completely avoiding any leaks.