The disclosed technique relates to gallium nitride crystal growth in general, and to methods and apparatus for forming gallium nitride crystal sheets, in particular.
Group-III metals of the periodic table (i.e., aluminum, gallium and indium) can form nitrides, i.e., aluminum nitride (AlN), gallium nitride (GaN) and indium nitride (InN). Group-III metal nitrides are semiconductors having various energy gaps (between two adjacent allowable bands), e.g., a narrow gap of 0.7 eV for InN, an intermediate gap of 3.4 eV for GaN, and a wide gap of 6.2 eV for AlN. Solid group-III metal nitrides have an ordered crystalline structure, giving them advantageous chemical and physical properties, such that electronic devices made from group-III metal nitrides can operate at conditions of high temperature, high power and high frequency. Furthermore, group-III metal nitrides are considered relatively chemically inert.
Electronic devices made from group-III metal nitrides may emit or absorb electromagnetic radiation having wavelengths ranging from the UV region to the IR region of the spectrum, which is particularly relevant for constructing light emitting diodes (LED), solid-state lights and the like. Other examples of applications of group-III metal nitride crystals are solid-state full color displays, optical storage devices, signal amplification devices, photovoltaic cells, under-water communication devices, space communication devices and the like. Furthermore, group-III metal nitrides may be used for other devices exhibiting solid state physical effects such as high semi-conducting electron mobility and saturation, opto-electricity, photo-luminescence, electro-luminescence, electron-emission, piezo-electricity, piezo-optics, diluted magnetism and the like.
To be used in various technological applications, the group-III metal nitride crystals may be in the form of a free-standing wafer or a thin film, attached to an arbitrary platform of conducting, semi-conducting, or dielectric nature. For other uses, group-III metal nitrides may be in the form of a free-standing bulk crystal. For industrial applications, group-III metal nitride crystals of large size (i.e., substantially 25 mm or larger) are required. However, crystals of large size, having a low defect density, are difficult to manufacture.
Group-III metal nitride crystals are not found naturally and are artificially produced as thin films on a crystalline substrate, by methods known in the art. Among the group-III metal nitrides, gallium nitride can be produced using hetero-epitaxy, wherein the substrate used as a hetero-epitaxial template can be, for example, a single-crystalline wafer of sapphire (Al2O3), on which a layer of GaN is deposited. Alternatively, a silicon carbide (SiC) wafer may be used as a substrate. However, due to the difference in lattice parameters between the substrate and the GaN layer, various crystal defects may appear in the GaN crystal.
Other known methods for growing group-III metal nitride crystals use a metallic melt, typically of the group-III metal. Nitrogen is supplied to the melt and chemically reacts with the group-III metal in the melt, thereby enabling crystal growth. Such methods are often expensive, and the crystal dimensions achieved, as well as the quantity of crystals produced, are typically small for industrial applications. Group-III metal nitride crystals, manufactured according to methods known in the art usually have crystal defects therein, such as dislocations, misorientations, vacancies, interstitial atoms, impurities, grain boundaries, and the like. In particular, none of the above mentioned methods are used to produce GaN crystal sheets of large dimensions, having a low defect density of less than 103 defects per centimeter squared.
PCT Publication WO 98/19964, to Angus et al., entitled “Method for the Synthesis of Group III Nitride Crystals”, is directed to a method for producing group-III nitride crystals from a liquid. The method is directed, in particular, to producing gallium nitride crystals. In one example, liquid gallium is held in a boron nitride crucible. The pressure inside the reaction chamber is reduced and the liquid is then heated to promote the desorption of trapped gas. An argon beam plasma and a hydrogen plasma are then used to remove impurities from the surface of the liquid gallium. An active nitrogen plasma is then used and the crucible is heated slowly, while pressure inside the crucible is maintained. Once the final temperature of 700° C. is attained, the nitrogen plasma beam is maintained on the surface of the liquid gallium for 12 hours. A supersaturation of the nitrogen is obtained and spontaneous crystallization occurs without cooling. Gallium nitride crystallizes on the surface of the liquid and forms a solid crust of GaN. A temperature gradient is imposed across the liquid surface such that one side of the liquid is held at a higher temperature than the other side. The solid GaN crust dissolves at the high temperature side and nitrogen is transported through the melt to the low temperature side, where the solid GaN recrystallizes. In this manner small crystals of solid GaN can be converted into larger crystals. In one example, a solid GaN polycrystalline dome, about 0.1 mm thick and having a surface area of 70 mm2, was obtained. Scanning electron micrographs revealed randomly oriented crystallites of different structures (
Li, H., and Sunkara, M., “Self-Oriented Growth of Gallium Nitride Films on Amorphous Substrates,” Proceedings of the 4th Symposium on Non-Stoichiometric III-V Compounds (2002) is directed to a method for growing gallium nitride crystal films from a melt of gallium. Thin films of molten gallium are spread on an amorphous substrate. The gallium films are exposed to nitrogen plasma (i.e., nitrogen ions) and heated to a temperature of 900°-1,000° C. for 1-3 hours at a pressure of 100 mtorr. Gallium nitride crystals nucleate from the molten gallium, and self-orient with respect to each other due to the mobility of the melt. Separate platelets of GaN join together and form a larger GaN film. It is noted that the self-orientation of gallium nitride crystals described in the method of Li and Sunkara is not perfect, and that certain regions of the GaN film obtained contain joined crystals which are misorientated in a common plane with respect to one another. Such misorientations create gaps, or holes, between adjacent crystals, and render that region and layer of the crystal not useful for industrial applications. Other regions of the GaN film obtained contain platelets which are misoriented and are not in a common plane, whereby the platelets point in different directions with respect to one another. It is also noted that the GaN film obtained by the method of Li and Sunkara exhibits grain boundaries, which, between some platelets, is hardly seen due to complete joining of the platelets.
It is an object of the disclosed technique to provide a novel method and system for forming a gallium nitride crystal sheet. In accordance with the disclosed technique, there is thus provided a method for forming a gallium nitride crystal sheet, including providing a metal melt, which contains gallium. The method further includes bringing the pressure over said metal melt to 0.01 Pa or lower. The metal melt is heated to a growth temperature of between approximately 860° C. and approximately 870° C. The method also includes applying nitrogen plasma to the surface of the metal melt at a working pressure of between approximately 0.05 Pa and approximately 2.5 Pa, until a gallium nitride crystal sheet is formed on top of the metal melt. The gallium nitride crystal sheet is formed on top of a gallium nitride crystals layer (especially having a dendritic form), which crystallizes on said metal melt. Preferably, the growth temperature is of 863° C., and the working pressure is of 0.1 Pa. According an embodiment of the disclosed technique, the method further includes separating the gallium nitride crystal sheet from the metal melt, after applying the plasma. The method can also include post-processing of the gallium nitride crystal sheet. The method can further include growing epitaxial layers on said gallium nitride crystal sheet. According to another aspect of the disclosed technique there is provided a gallium nitride crystal sheet formed by the novel method.
The disclosed technique will be understood and appreciated more fully from the following detailed description taken in conjunction with the drawings in which:
The disclosed technique overcomes the disadvantages of the prior art by providing a method and apparatus for forming a gallium nitride crystal sheet of large dimensions having a low defect density, from a metal melt and a nitrogen plasma, by providing exact pressure and temperature growth conditions.
Reference is now made to
Reference is now made to
In procedure 120, a metal melt is provided, which contains gallium. The metal melt can be contained in a container. In procedure 122, the pressure over the metal melt is brought to a vacuum of at least 0.01 Pa (pascals). To achieve such a pressure, the metal melt can be placed, for example, in a vacuum chamber, or a pressure (vacuum) bell (i.e., a compartment open at its bottom) may be partially submerged in the metal melt, or in outer space. This vacuum is also referred to as “base pressure”. With reference to
According to the disclosed technique, gallium nitride crystals of dendritic form are grown from the metal melt, by applying nitrogen plasma to the surface of the metal melt. The metal melt can be a pure gallium melt, or alternatively, a gallium-indium melt, which contains gallium as well as indium at a selected concentration. For example, the gallium-indium melt can contain 70 weight percent indium and 30 weight percent gallium. With reference to
In procedure 124, the metal melt is heated to a growth temperature of between approximately 860° C.-870° C., which is suitable for GaN dendrite crystal growth. In particular, an effective growth temperature can be of 863° C. With reference to
In procedure 125, nitrogen plasma is applied to the surface of the metal melt, at a sub-atmospheric pressure selected from the range of between approximately 0.05 Pa and approximately 2.5 Pa, until a GaN crystal sheet is formed on top of the metal melt. This sub-atmospheric pressure is also referred to as “working pressure”. Preferably, the working pressure is selected from the range of between approximately 0.05 Pa and approximately 0.2 Pa. In particular, a working pressure of about 0.1 Pa is most suitable.
It is noted, that the nitrogen plasma applied to the surface of metal melt 104, must include an appropriate amount of nitrogen ions. Obtaining an appropriate amount of nitrogen ions is achieved by the procedure of applying nitrogen plasma to the surface of metal melt 104 at working pressure. An appropriate amount of nitrogen ions can also be obtained by employing a faucet for controlling the flow of nitrogen ions applied to the surface of the metal melt, at a given working pressure, within or outside the sub-atmospheric pressure ranges mentioned above.
Reference is now made to
In sub-procedure 128, the nitrogen plasma is directed to the surface of the metal melt, until GaN crystals crystallize on the metal melt. It is noted that sub-procedure 127 and sub-procedure 128 may be performed in conjunction (i.e., as a single procedure, for example where a plasmatron ionizes the nitrogen and emits plasma of ionized nitrogen toward the surface of the metal melt. The active nitrogen reaching the surface of the metal melt reacts with or saturates the metal melt surface. As a result, dendrite GaN crystallizes on the surface of the metal melt. It is noted that certain plasma generators (i.e., plasmatrons) require a bias voltage. If such a plasma generator is used, a negative bias potential may be applied to the metal melt. The bias potential can be applied by direct current (DC), if a required potential is lower than approximately minus 1 Kilovolt. If a higher potential is required, negative alternating current (AC) may be used.
As the nitrogen plasma is directed to the metal melt, the active nitrogen reacts with the gallium in the metal melt, thereby causing crystallization of GaN crystals from the metal melt. The GaN crystals which crystallize from the metal melt posses substantially the same crystallographic orientation (e.g., 002 orientation, perpendicular to the metal melt surface). The GaN crystals may crystallize in different crystalline structures, for example some may crystallize as dendritic GaN, while others may crystallize as GaN platelets, or single crystal GaN bulky grains. The formation of the various GaN crystal structures depends mainly on the temperature of the metal melt. Under the given temperature and pressure conditions (i.e., 0.1 Pa and 863° C.), most of the GaN is likely to crystallize in the dendritic form on the surface of the metal melt. As the area covered by dendritic GaN crystals which crystallize on the metal melt increases, they form a net-like layer on the metal melt surface. With reference to
In sub-procedure 129, the working pressure of the metal melt and the directed stream of nitrogen plasma are maintained until a GaN crystal sheet is formed on top of the GaN crystal net-like layer. Sub-procedure 129 can be performed for a predetermined amount of time, which can range from 1 minute to 5 minutes. In particular, this amount of time can be 3 minutes. The GaN crystal sheet forms in a wave-like expanding manner, starting from one particular location of the dendritic GaN crystal net-like layer, and spreading out there from. Sometimes there are several such particular locations, in which case the GaN crystal sheet spreads outwardly from all these particular locations to eventually meet and unite into one sheet. In this case, the GaN crystal sheet is constructed of two dimensional grains, each grain having a radius of a few millimeters. The grains have a typical lateral orientation (i.e., along the x and y axes, if taken in a Cartesian reference frame), and their perpendicular orientation (i.e., normal to the melt surface, along the z axis) remains constant (002). Although the GaN dendrite crystals, which crystallized on the metal melt in sub-procedure 128, may have different lateral crystalline orientations, the formed GaN crystal sheet (formed on the GaN dendrite crystals), or the grains of which the sheet is constructed, are not affected by these crystalline orientations and possess a uniform structure of an oriented single-crystal GaN sheet. Furthermore, although the GaN crystal net-like layer on the metal melt surface may inhibit holes or gaps, the GaN crystal sheet is formed over such holes or gaps and “bridges” them by covering the entire area in which the GaN crystals are present. The formed GaN crystal sheet typically contains a low crystal defect density of less than 103 defects per centimeter squared. With reference to
Reference is further made to
According to another embodiment of the disclosed technique, separating of the GaN crystal sheet from the metal melt can be performed by pulling the GaN crystal sheet out of the metal melt, for example by using a tweezers. With reference to
According to a further embodiment, the metal melt can be drained from the container, leaving only the GaN crystal sheet in the container. The sides of the container may be equipped with protruding elements, such that they are located beneath the metal melt surface. The container is equipped with a drainage outlet, for example at the bottom thereof, or with a pump for emptying the metal melt from the container. After the formation of the GaN crystal sheet, the metal melt is drained out of the container using the drainage outlet or the pump. The GaN crystal sheet remains in the container, either supported by the protruding elements, or on the bottom of the container. After draining the metal melt, the GaN crystal sheet can be used. It is noted that procedure 130 is optional, and the method depicted in
In procedure 132, the GaN crystal sheet is post-processed. Post-processing the GaN crystal sheet can include washing the GaN crystal sheet with an acid, for removing excess metal from the GaN crystal sheet, bonding the GaN crystal sheet to a substrate, sintering the GaN crystal sheet to a substrate, growing epitaxial layers on the GaN crystal sheet, doping the GaN crystal sheet, metallizing the GaN crystal sheet, sectioning the GaN crystal sheet, or performing micro-fabrication processes on the GaN crystal sheet (e.g., lithography, etching and deposition). It is noted that procedure 132 is optional, and the method depicted in
It will be appreciated by persons skilled in the art that the disclosed technique is not limited to what has been particularly shown and described hereinabove. Rather the scope of the disclosed technique is defined only by the claims, which follow.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IL06/01319 | 11/15/2006 | WO | 00 | 10/1/2008 |
Number | Date | Country | |
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60737786 | Nov 2005 | US |