Structure and method for fabrication for a solid-state lighting device

Information

  • Patent Grant
  • 6639249
  • Patent Number
    6,639,249
  • Date Filed
    Monday, August 6, 2001
    23 years ago
  • Date Issued
    Tuesday, October 28, 2003
    21 years ago
Abstract
A multi-color, solid-state lighting device includes a stack of two or more panels, each panel having an array of light emitting semiconductor components formed thereon. To form the light emitting components, high quality epitaxial layers of monocrystalline materials can be grown overlying a monocrystalline layer of silicon formed on a low cost substrate, such as glass. The growth of the monocrystalline materials is accomplished by forming a compliant substrate for growing the monocrystalline materials. An accommodating buffer layer comprises a layer of monocrystalline oxide spaced apart from a silicon by an amorphous interface layer of silicon oxide. The amorphous interface layer dissipates strain and permits the growth of a high quality monocrystalline oxide accommodating buffer layer.
Description




FIELD OF THE INVENTION




This invention relates generally to semiconductor structures and devices and to methods for their fabrication, and more specifically to semiconductor structures, devices, and fabrication methods for light emitting semiconductor devices.




BACKGROUND OF THE INVENTION




Solid-state light sources, such as light emitting diodes (LEDs) and laser diodes, can offer significant advantages over other forms of lighting, such as incandescent or fluorescent lighting. For example, when LEDs or laser diodes are placed in arrays of red, green and blue elements, they can act as a source for white light or as a multi-colored display. In such configurations, solid-state light sources are generally more efficient and produce less heat than traditional incandescent or fluorescent lights. Although solid-state lighting offers certain advantages, conventional semiconductor structures and devices used for solid-state lighting are relatively expensive.




Accordingly, a need exists for a semiconductor structure and/or device that provides solid-state lighting at reduced cost.











BRIEF DESCRIPTION OF THE DRAWINGS




The present invention is illustrated by way of example and not limitation in the accompanying figures, in which like references indicate similar elements, and in which:





FIGS. 1

,


2


, and


3


illustrate schematically, in cross section, device structures in suitable for providing light sources in accordance with various embodiments of the invention;





FIG. 4

is a block diagram of irradiation system that can be used to form the crystalline semiconductor layer on the substrate;





FIGS. 5-10

are top views of a sample structure at sequential stages in a first variant of processing the semiconductor layer on the substrate to form single-crystal regions;





FIGS. 11-16

are top views of a sample structure at sequential stages in a second variant of processing the semiconductor layer on the substrate to form single-crystal regions;





FIGS. 17-19

are top views of a sample structure at sequential stages in a third variant of processing the semiconductor layer on the substrate to form single-crystal regions;





FIG. 20

illustrates graphically the relationship between maximum attainable film thickness and lattice mismatch between a host crystal and a grown crystalline overlayer;





FIG. 21

illustrates a high resolution Transmission Electron Micrograph of a structure including a monocrystalline accommodating buffer layer;





FIG. 22

illustrates an x-ray diffraction spectrum of a structure including a monocrystalline accommodating buffer layer;





FIG. 23

illustrates a high resolution Transmission Electron Micrograph of a structure including an amorphous oxide layer;





FIG. 24

illustrates an x-ray diffraction spectrum of a structure including an amorphous oxide layer;





FIGS. 25-28

illustrate schematically, in cross-section, the formation of a device structure suitable for lighting devices in accordance with another embodiment of the invention;





FIGS. 29-32

illustrate a probable molecular bonding structure of the device structures illustrated in

FIGS. 25-28

;





FIGS. 33-36

illustrate schematically, in cross-section, the formation of a device structure suitable for forming lighting sources in accordance with still another embodiment of the invention;





FIGS. 37-39

illustrate schematically, in cross-section, the formation of yet another embodiment of a device structure suitable for lighting sources in accordance with the invention;





FIGS. 40

,


41


illustrate schematically, in cross section, device structures that can be used for light devices in accordance with various embodiments of the invention;





FIGS. 42-46

are illustrations of cross-sectional views of a portion of an integrated circuit that includes a compound semiconductor portion, a bipolar portion, and an MOS portion;





FIGS. 47-53

are illustrations of cross-sectional views of a portion of another integrated circuit that includes a semiconductor laser and a MOS transistor in accordance with various embodiments of the invention;





FIG. 54

illustrates schematically, in cross-section, a portion of a light source device in accordance with an embodiment of the invention; and





FIG. 55

illustrates schematically, in cross-section, a portion of a full-color display device in accordance with a further embodiment of the invention.





FIG. 56

is a flow chart that shows a process for fabricating a structure for producing light.











Skilled artisans will appreciate that elements in the figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale. For example, the dimensions of some of the elements in the figures may be exaggerated relative to other elements to help to improve understanding of embodiments of the present invention.




DETAILED DESCRIPTION OF THE DRAWINGS





FIG. 1

illustrates schematically, in cross section, a portion of a semiconductor structure


20


suitable for providing light sources in accordance with an embodiment of the invention. Semiconductor structure


20


includes a substrate


21


, a thermal oxide layer


23


, a monocrystalline semiconductor layer


22


, accommodating buffer layer


24


comprising a monocrystalline material, and a monocrystalline material layer


26


. In this context, the term “monocrystalline” shall have the meaning commonly used within the semiconductor industry. The term shall refer to materials that are a single crystal or that are substantially a single crystal and shall include those materials having a relatively small number of defects such as dislocations and the like as are commonly found in bulk substrates of silicon or germanium or mixtures of silicon and germanium and epitaxial layers of such materials commonly found in the semiconductor industry.




Structure


20


can also include an amorphous intermediate layer


28


positioned between semiconductor layer


22


and accommodating buffer layer


24


. Structure


20


may also include a template layer


30


between the accommodating buffer layer and monocrystalline material layer


26


. As will be explained more fully below, the template layer helps to initiate the growth of the monocrystalline material layer on the accommodating buffer layer. The amorphous intermediate layer helps to relieve the strain in the accommodating buffer layer and by doing so, aids in the growth of a high crystalline quality accommodating buffer layer.




The substrate


21


can be any suitable material, e.g., silicon, quartz, glass or plastic, or the like, subject to considerations of stability, inertness and heat resistance under processing conditions. Preferably, the substrate


21


is glass.




In the context of this disclosure, the term “substrate” is normally used to indicate either the substrate


21


or the structure including the substrate


21


, the oxide layer


23


, and the semiconductor layer


22


. The substrate


21


is alternatively called a glass substrate, although it can be formed of other materials, as described herein. The structure including the substrate


21


, the oxide layer


23


, and the semiconductor layer


22


is alternatively called a monocrystalline substrate, or a silicon substrate (the silicon substrate being one form of the monocrystalline substrate). In some instances in this disclosure, the term monocrystalline substrate refers to a bulk monocrystalline substrate, and the term silicon substrate means a bulk silicon substrate. The term compliant substrate generally refers to the monocrystilline substrate with the accommodating buffer layer


24


formed thereon.




The thermal oxide layer


23


is preferably a layer of silicon dioxide formed or deposited on the surface of the substrate


21


.




Semiconductor layer


22


can be a monocrystalline semiconductor or compound semiconductor film formed on the thermal oxide layer


23


on the substrate


21


. The film can be, for example, a material from Group IV of the periodic table. Examples of Group IV semiconductor materials include silicon, germanium, mixed silicon and germanium, mixed silicon and carbon, mixed silicon, germanium and carbon, and the like. Preferably, layer


22


is a film of deposited silicon. The process of forming regions of the monocrystalline semiconductor layer


22


on the substrate


21


is described below in connection with

FIGS. 4-19

.




Accommodating buffer layer


24


is preferably a monocrystalline oxide or nitride material epitaxially grown on layer


22


. Amorphous intermediate layer


28


can be grown on layer


22


at the interface between semiconductor layer


22


and the growing accommodating buffer layer by the oxidation of semiconductor layer


22


during the growth of layer


24


. The amorphous intermediate layer serves to relieve strain that might otherwise occur in the monocrystalline accommodating buffer layer as a result of differences in the lattice constants of the material of layer


22


and the buffer layer. As used herein, lattice constant refers to the distance between atoms of a cell measured in the plane of the surface. If such strain is not relieved by the amorphous intermediate layer, the strain may cause defects in the crystalline structure of the accommodating buffer layer. Defects in the crystalline structure of the accommodating buffer layer, in turn, would make it difficult to achieve a high quality crystalline structure in monocrystalline material layer


26


which may comprise a semiconductor material, a compound semiconductor material, or another type of material such as a metal or a non-metal.




Accommodating buffer layer


24


is preferably a monocrystalline oxide or nitride material selected for its crystalline compatibility with the underlying monocrystalline substrate and with the overlying material layer. For example, the material could be an oxide or nitride having a lattice structure closely matched to the monocrystalline layer and to the subsequently applied monocrystalline material layer. Materials that are suitable for the accommodating buffer layer include metal oxides such as the alkaline earth metal titanates, alkaline earth metal zirconates, alkaline earth metal hafnates, alkaline earth metal tantalates, alkaline earth metal ruthenates, alkaline earth metal niobates, alkaline earth metal vanadates, alkaline earth metal tin-based perovskites, lanthanum aluminate, lanthanum scandium oxide, and gadolinium oxide. Additionally, various nitrides such as gallium nitride, aluminum nitride, and boron nitride may also be used for the accommodating buffer layer. Most of these materials are insulators, although strontium ruthenate, for example, is a conductor. Generally, these materials are metal oxides or metal nitrides, and more particularly, these metal oxide or nitrides typically include at least two different metallic elements. In some specific applications, the metal oxides or nitrides may include three or more different metallic elements.




Amorphous interface layer


28


is preferably an oxide formed by the oxidation of the surface of semiconductor layer


22


, and more preferably is composed of a silicon oxide. The thickness of layer


28


is sufficient to relieve strain attributed to mismatches between the lattice constants of semiconductor layer


22


and accommodating buffer layer


24


. Typically, layer


28


has a thickness in the range of approximately 0.5-5 nm.




The material for monocrystalline material layer


26


can be selected, as desired, for a particular structure or application. For example, the monocrystalline material of layer


26


may comprise a compound semiconductor which can be selected, as needed for a particular semiconductor structure, from any of the Group IIIA and VA elements (III-V semiconductor compounds), mixed III-V compounds, Group II(A or B) and VIA elements (II-VI semiconductor compounds), and mixed II-VI compounds. Examples include gallium arsenide (GaAs), gallium indium arsenide (GaInAs), gallium aluminum arsenide (GaAlAs), indium phosphide (InP), cadmium sulfide (CdS), cadmium mercury telluride (CdHgTe), zinc selenide (ZnSe), zinc sulfur selenide (ZnSSe), and the like. However, monocrystalline material layer


26


may also comprise other semiconductor materials, metals, or non-metal materials which are used in the formation of semiconductor structures, devices and/or integrated circuits.




Appropriate materials for template


30


are discussed below. Suitable template materials chemically bond to the surface of the accommodating buffer layer


24


at selected sites and provide sites for the nucleation of the epitaxial growth of monocrystalline material layer


26


. When used, template layer


30


has a thickness ranging from about 1 to about 10 monolayers.





FIG. 2

illustrates, in cross section, a portion of a semiconductor structure


40


suitable for constructing lighting sources in accordance with a further embodiment of the invention. Structure


40


is similar to the previously described semiconductor structure


20


, except that an additional buffer layer


32


is positioned between accommodating buffer layer


24


and monocrystalline material layer


26


. Specifically, the additional buffer layer is positioned between template layer


30


and the overlying layer of monocrystalline material. The additional buffer layer, formed of a semiconductor or compound semiconductor material when the monocrystalline material layer


26


comprises a semiconductor or compound semiconductor material, serves to provide a lattice compensation when the lattice constant of the accommodating buffer layer cannot be adequately matched to the overlying monocrystalline semiconductor or compound semiconductor material layer.





FIG. 3

schematically illustrates, in cross section, a portion of a semiconductor structure


34


suitable for constructing lighting devices in accordance with another exemplary embodiment of the invention. Structure


34


is similar to structure


20


, except that structure


34


includes an amorphous layer


36


, rather than accommodating buffer layer


24


and amorphous interface layer


28


, and an additional monocrystalline layer


38


.




As explained in greater detail below, amorphous layer


36


may be formed by first forming an accommodating buffer layer and an amorphous interface layer in a similar manner to that described above. Monocrystalline layer


38


is then formed (by epitaxial growth) overlying the monocrystalline accommodating buffer layer. The accommodating buffer layer is then exposed to an anneal process to convert the monocrystalline accommodating buffer layer to an amorphous layer. Amorphous layer


36


formed in this manner comprises materials from both the accommodating buffer and interface layers, which amorphous layers may or may not amalgamate. Thus, layer


36


may comprise one or two amorphous layers. Formation of amorphous layer


36


between semiconductor layer


22


and additional monocrystalline layer


26


(subsequent to layer


38


formation) relieves stresses between layers


22


and


38


and provides a true compliant substrate for subsequent processing—e.g., monocrystalline material layer


26


formation.




The processes previously described above in connection with

FIGS. 1 and 2

are adequate for growing monocrystalline material layers over a monocrystalline substrate. However, the process described in connection with

FIG. 3

, which includes transforming a monocrystalline accommodating buffer layer to an amorphous oxide layer, may be better for growing monocrystalline material layers because it allows any strain in layer


26


to relax.




Additional monocrystalline layer


38


may include any of the materials described throughout this application in connection with either of monocrystalline material layer


26


or additional buffer layer


32


. For example, when monocrystalline material layer


26


comprises a semiconductor or compound semiconductor material, layer


38


may include monocrystalline Group IV or monocrystalline compound semiconductor materials.




Additional monocrystalline layer


38


can serve as an anneal cap during layer


36


formation and as a template for subsequent monocrystalline layer


26


formation. Accordingly, layer


38


is preferably thick enough to provide a suitable template for layer


26


growth (at least one monolayer) and thin enough to allow layer


38


to form as a substantially defect free monocrystalline material.




Alternatively, additional monocrystalline layer


38


can comprise monocrystalline material (e.g., a material discussed above in connection with monocrystalline layer


26


) that is thick enough to form devices within layer


38


. In this case, the semiconductor structure does not include monocrystalline material layer


26


. In other words, the semiconductor structure in accordance with this embodiment only includes one monocrystalline layer disposed above amorphous oxide layer


36


.




Turning now to

FIGS. 4-19

, one process by which the monocrystalline semiconductor layer


22


is formed on the substrate


21


is described in further detail.




For forming the monocrystalline semiconductor layer


22


on the substrate


21


, a lateral solidification technique is applied to a semiconductor film on the substrate


21


. The technique involves irradiating a portion of the film with a suitable radiation pulse, e.g., a laser beam pulse, locally, to melt the film completely through its entire thickness. When the molten semiconductor material solidifies, a crystalline structure grows from a pre-selected portion of the film that did not undergo complete melting.




A beam is pulsed repeatedly in forming an extended single-crystal region as a result of laterally stepping a radiation pattern for repeated melting and solidification. The technique described herein for forming layer


22


over substrate


21


is similar to a technique described in International Patent Application number PCT/US96/07730. Any other technique that results in a monocrystalline semiconductor layer over glass can be used to form the semiconductor layer


22


.





FIG. 4

illustrates a block diagram of a projection irradiation system


510


for forming the monocrystalline regions on the glass substrate. The projection irradiation system includes an excimer laser


501


, mirrors


502


, a variable focus field lens


504


, a patterned mask


505


, a two-element imaging lens


506


, a sample stage


507


, and a variable attenuator


508


. A sample


500


is disposed on the sample stage


507


. This system can be used to produce a shaped beam for stepped growth of a single-crystal silicon region in a sequential lateral solidification (SLS) process. Alternatively, a proximity mask or even a contact mask may be used for beam shaping.




In operation of the system


510


, samples are placed onto the stage


507


of the projection irradiation system


510


. The mask can have a pattern of simple stripes of 50 micrometers wide, with various separation distances from 10 to 100 micrometers.




In addition radiation beams other than a laser beam can be used, for example, an electron or ion beam.




The sample structure includes the substrate


21


, a thermal oxide film


23


, and an amorphous silicon film deposited over the thermal oxide film


23


.




Structures in accordance with layers


22


-


23


can prepared by any suitable conventional processing technique, including sequential low-pressure chemical vapor deposition (LPCVD) of SiO


2


and a —Si on a glass or quartz substrate. Other suitable deposition methods, for producing amorphous or microcrystalline deposits, include plasma-enhanced chemical vapor deposition (PECVD), evaporation or sputtering, for example.




The mask pattern is projected onto the samples with different reduction factors in the range from 3 to 6. Samples can be irradiated at room temperature with a 30-nanosecond XeCl excimer laser pulse having a wavelength of 308 nanometers, quartz being transparent at this wavelength. Such a laser is commercially available. For a glass substrate, a longer wavelength can be used, e.g., 348 nanometers.




Irradiation can be with fixed energy density. The energy density can be in the range from 1 to 680 mJ/cm


2


.




In the following, the sequential lateral solidification (SLS) process is described with reference to

FIGS. 5-10

and


11


-


16


showing first and second variants, respectively, of the process, and

FIGS. 17-19

showing a third variant. Starting with the amorphous silicon film


521


, which in this exemplary embodiment is patterned as a rectangle (FIG.


5


), a region


520


, bounded by two broken lines, of the silicon film


521


is irradiated with a pulse, to completely melt the silicon in that region (FIG.


6


), and then resolidify the molten silicon (

FIG. 7

) in the region


520


. Here, the region


520


is in the shape of a stripe, and irradiation of the region


520


may be masked projection or by use of a proximity mask.




Upon re-solidification of the molten silicon in the region


520


, two rows


522


of grains grow explosively from the broken line boundaries of the region


520


towards the center of the region


520


. In the remainder of region


520


, a fine grained polycrystalline region


524


is formed.




Preferably, the width of the stripe is chosen such that, upon resolidification, the two rows of grains approach each other without converging. Smaller widths of the region


520


tend to be undesirable since the subsequent step may have to be reduced in length, and the semiconductor surface may become irregular where grains growing from opposite directions come together during the solidification process. An oxide cap may be formed over the silicon film to retard agglomeration and constrain the surface of the silicon film to be smooth.




A next region


526


to be irradiated is defined by shifting (stepping) the sample with respect to the masked projection or proximity mask in the direction of crystal growth. The shifted (stepped) region


526


is bounded by two broken lines, as shown in FIG.


8


. The distance of the shift is such that the next region


526


to be irradiated overlaps the previously irradiated region


520


so as to completely melt one row of crystals


522


while partially melting the other row of crystals


522


, as shown in FIG.


9


. Upon resolidification, the partially melted row of crystals becomes longer, as shown in FIG.


10


. In this fashion, by repeatedly shifting the irradiated portion, monocrystalline grains of any desired length may be grown.




If the pattern of the irradiated region is not a simple stripe, but is in the shape of a chevron


540


, as shown in

FIG. 11

, the same sequence of shifting the irradiated region shown in

FIGS. 12-16

results in the enlargement of one grain growing from the apex of the trailing edge of the shifting (stepping) chevron pattern. In this manner, a monocrystalline region


571


can be grown with increasing width and length.




A large area single-crystal region can also be grown by applying sequentially shifted (stepped) irradiation regions to a patterned amorphous silicon film, such as that illustrated in

FIG. 17

, having a tail region


550


, a narrow bottleneck region


552


and a main island region


554


. The region of irradiation


553


defined by masked projection or a proximity mask is illustrated by the regions bounded by broken lines in

FIGS. 17-19

, which also show the sequential lateral shifting (stepping) of the irradiated region


553


to obtain the growth of a single grain from the tail region


550


through the bottleneck region


552


to produce a single crystal island region


554


.




Sequential lateral melting and resolidification in the examples of

FIGS. 5-10

,


11


-


16


and


17


-


19


can be carried out on amorphous silicon films that are deposited by chemical vapor deposition (CVD) on a silicon dioxide coated quartz or glass substrate, with film thicknesses from 100 to 240 nanometers.




The following non-limiting, illustrative examples illustrate various combinations of materials useful in structures


20


,


40


, and


34


. These examples are merely illustrative, and it is not intended that the invention be limited to these illustrative examples.




EXAMPLE 1




In this example, monocrystalline semiconductor layer


22


is a silicon film oriented in the (100) direction. The silicon film can be, for example, a silicon layer as is used in making complementary metal oxide semiconductor (CMOS) integrated circuits. In accordance with this example, accommodating buffer layer


24


is a monocrystalline layer of Sr


2


Ba


l−z


TiO


3


where z ranges from 0 to 1 and the amorphous intermediate layer is a layer of silicon oxide (SiO


x


) formed at the interface between the silicon film and the accommodating buffer layer. The value of z is selected to obtain one or more lattice constants closely matched to corresponding lattice constants of the subsequently formed layer


26


. The accommodating buffer layer can have a thickness of about 2 to about 100 nanometers (nm) and preferably has a thickness of about 5 nm. In general, it is desired to have an accommodating buffer layer thick enough to isolate the monocrystalline material layer


26


from the silicon layer to obtain the desired electrical and optical properties. Layers thicker than 100 nm usually provide little additional benefit while increasing cost unnecessarily; however, thicker layers may be fabricated if needed. The amorphous intermediate layer of silicon oxide can have a thickness of about 0.5-5 nm, and preferably a thickness of about 1 to 2 nm.




Monocrystalline material layer


26


is a compound semiconductor layer of gallium arsenide (GaAs) or aluminum gallium arsenide (AlGaAs) having a thickness of about 1 nm to about 100 micrometers (μm) and preferably a thickness of about 0.5 μm to 10 μm. The thickness generally depends on the application for which the layer is being prepared. To facilitate the epitaxial growth of the gallium arsenide or aluminum gallium arsenide on the monocrystalline oxide, a template layer is formed by capping the oxide layer. The template layer is preferably 1-10 monolayers of Ti—As, Sr—O—As, Sr—Ga—O, or Sr—Al—O. By way of a preferred example, 1-2 monolayers of Ti—As or Sr—Ga—O have been illustrated to successfully grow GaAs layers.




EXAMPLE 2




In accordance with a second exemplary set of semiconductor materials, monocrystalline semiconductor layer


22


is a silicon film as described above. The accommodating buffer layer is a monocrystalline oxide of strontium or barium zirconate or hafnate in a cubic or orthorhombic phase with an amorphous intermediate layer of silicon oxide formed at the interface between the silicon layer and the accommodating buffer layer. The accommodating buffer layer can have a thickness of about 2-100 nm and preferably has a thickness of at least 5 nm to ensure adequate crystalline and surface quality and is formed of a monocrystalline SrZrO


3


, BaZrO


3


, SrHfO


3


, BaSnO


3


or BaHfO


3


. For example, a monocrystalline oxide layer of BaZrO


3


can grow at a temperature of about 700 degrees C. The lattice structure of the resulting crystalline oxide exhibits a 45 degree rotation with respect to the silicon film lattice structure.




An accommodating buffer layer formed of these zirconate or hafnate materials is suitable for the growth of a monocrystalline material layer which comprises compound semiconductor materials in the indium phosphide (InP) system. In this system, the compound semiconductor material can be, for example, indium phosphide (InP), indium gallium arsenide (InGaAs), aluminum indium arsenide, (AlInAs), or aluminum gallium indium arsenic phosphide (AlGaInAsP), having a thickness of about 1.0 nm to 10 μm. A suitable template for this structure is 1-10 monolayers of zirconium-arsenic (Zr—As), zirconium-phosphorus (Zr—P), hafnium-arsenic (Hf—As), hafnium-phosphorus (Hf—P), strontium-oxygen-arsenic (Sr—O—As), strontium-oxygen-phosphorus (Sr—O—P), barium-oxygen-arsenic (Ba—O—As), indium-strontium-oxygen (In—Sr—O), or barium-oxygen-phosphorus (Ba—O—P), and preferably 1-2 monolayers of one of these materials. By way of an example, for a barium zirconate accommodating buffer layer, the surface is terminated with 1-2 monolayers of zirconium followed by deposition of 1-2 monolayers of arsenic to form a Zr—As template. A monocrystalline layer of the compound semiconductor material from the indium phosphide system is then grown on the template layer. The resulting lattice structure of the compound semiconductor material exhibits a 45 degree rotation with respect to the accommodating buffer layer lattice structure and a lattice mismatch to (100) InP of less than 2.5%, and preferably less than about 1.0%.




EXAMPLE 3




In accordance with a third set of exemplary semiconductor materials, a structure is provided that is suitable for the growth of an epitaxial film of a monocrystalline material comprising a II-VI material overlying a silicon film on the glass substrate. A suitable accommodating buffer layer material is Sr


x


Ba


l−x


TiO


3


, where x ranges from 0 to 1, having a thickness of about 2-100 nm and preferably a thickness of about 5-15 nm. Where the monocrystalline layer comprises a compound semiconductor material, the II-VI compound semiconductor material can be, for example, zinc selenide (ZnSe) or zinc sulfur selenide (ZnSSe). A suitable template for this material system includes 1-10 monolayers of zinc-oxygen (Zn—O) followed by 1-2 monolayers of an excess of zinc followed by the selenidation of zinc on the surface. Alternatively, a template can be, for example, 1-10 monolayers of strontium-sulfur (Sr—S) followed by the ZnSeS.




EXAMPLE 4




This embodiment of this example of is shown as structure


40


illustrated in FIG.


2


. Semiconductor layer


22


, accommodating buffer layer


24


, and monocrystalline material layer


26


can be similar to those described in Example 1. In addition, an additional buffer layer


32


serves to alleviate any strains that might result from a mismatch of the crystal lattice of the accommodating buffer layer and the lattice of the monocrystalline material. Buffer layer


32


can be a layer of germanium or a GaAs, an aluminum gallium arsenide (AlGaAs), an indium gallium phosphide (InGaP), an aluminum gallium phosphide (AlGaP), an indium gallium arsenide (InGaAs), an aluminum indium phosphide (AlInP), a gallium arsenide phosphide (GaAsP), or an indium gallium phosphide (InGaP) strain compensated superlattice. In accordance with one aspect of this embodiment, buffer layer


32


includes a GaAs


x


P


l−x


superlattice, wherein the value of x ranges from 0 to 1. In accordance with another aspect, buffer layer


32


includes an In


y


Ga


l−y


P superlattice, wherein the value of y ranges from 0 to 1. By varying the value of x or y, as the case may be, the lattice constant is varied from bottom to top across the superlattice to create a match between lattice constants of the underlying oxide and the overlying monocrystalline material which in this example is a compound semiconductor material. The compositions of other compound semiconductor materials, such as those listed above, may also be similarly varied to manipulate the lattice constant of layer


32


in a like manner. The superlattice can have a thickness of about 50-500 nm and preferably has a thickness of about 100-200 nm. The template for this structure can be the same of that described in Example 1. Alternatively, buffer layer


32


can be a layer of monocrystalline germanium having a thickness of 1-50 nm and preferably having a thickness of about 2-20 nm. In using a germanium buffer layer, a template layer of either germanium-strontium (Ge—Sr) or germanium-titanium (Ge—Ti) having a thickness of about one monolayer can be used as a nucleating site for the subsequent growth of the monocrystalline material layer which in this example is a compound semiconductor material. The formation of the oxide layer is capped with either a monolayer of strontium or a monolayer of titanium to act as a nucleating site for the subsequent deposition of the monocrystalline germanium. The monolayer of strontium or titanium provides a nucleating site to which the first monolayer of germanium can bond.




EXAMPLE 5




This example also illustrates materials useful in a structure


40


as illustrated in FIG.


2


. Semiconductor material


22


, accommodating buffer layer


24


, monocrystallinematerial layer


26


and template layer


30


can be the same as those described above in Example 2. In addition, additional buffer layer


32


is inserted between the accommodating buffer layer and the overlying monocrystalline material layer. The buffer layer, a further monocrystalline material which in this instance comprises a semiconductor material, can be, for example, a graded layer of indium gallium arsenide (InGaAs) or indium aluminum arsenide (InAlAs). In accordance with one aspect of this embodiment, additional buffer layer


32


includes InGaAs, in which the indium composition varies from 0 to about 50%. The additional buffer layer


32


preferably has a thickness of about 10-30 nm. Varying the composition of the buffer layer from GaAs to InGaAs serves to provide a lattice match between the underlying monocrystalline oxide material and the overlying layer of monocrystalline material which in this example is a compound semiconductor material. Such a buffer layer is especially advantageous if there is a lattice mismatch between accommodating buffer layer


24


and monocrystalline material layer


26


.




EXAMPLE 6




This example provides exemplary materials useful in structure


34


, as illustrated in FIG.


3


. Semiconductor material


22


, template layer


30


, and monocrystalline material layer


26


may be the same as those described above in connection with example 1.




Amorphous layer


36


is an amorphous oxide layer which is suitably formed of a combination of amorphous intermediate layer materials (e.g., layer


28


materials as described above) and accommodating buffer layer materials (e.g., layer


24


materials as described above). For example, amorphous layer


36


may include a combination of SiO


x


and Sr


z


Ba


l−z


TiO


3


(where z ranges from 0 to 1),which combine or mix, at least partially, during an anneal process to form amorphous oxide layer


36


.




The thickness of amorphous layer


36


may vary from application to application and may depend on such factors as desired insulating properties of layer


36


, type of monocrystalline material comprising layer


26


, and the like. In accordance with one exemplary aspect of the present embodiment, layer


36


thickness is about 2 nm to about 100 nm, preferably about 2-10 nm, and more preferably about 5-6 nm.




Layer


38


comprises a monocrystalline material that can be grown epitaxially over a monocrystalline oxide material such as material used to form accommodating buffer layer


24


. Layer


38


can include the same materials as those comprising layer


26


. For example, if layer


26


includes GaAs, layer


38


also includes GaAs. However, in accordance with other embodiments, layer


38


may include materials different from those used to form layer


26


. In accordance with one exemplary structure, layer


38


is about 1 monolayer to about 100 nm thick.




Referring again to

FIGS. 1-3

, semiconductor layer


22


is a monocrystalline region of film, such as a monocrystalline silicon. The crystalline structure of the monocrystalline film is characterized by a lattice constant and by a lattice orientation. In similar manner, accommodating buffer layer


24


is also a monocrystalline material and the lattice of that monocrystalline material is characterized by a lattice constant and a crystal orientation. The lattice constants of the accommodating buffer layer and the monocrystalline layer


22


must be closely matched or, alternatively, must be such that upon rotation of one crystal orientation with respect to the other crystal orientation, a substantial match in lattice constants is achieved. In this context the terms “substantially equal” and “substantially matched” mean that there is sufficient similarity between the lattice constants to permit the growth of a high quality crystalline layer on the underlying layer.





FIG. 20

illustrates graphically the relationship of the achievable thickness of a grown crystal layer of high crystalline quality as a function of the mismatch between the lattice constants of the host crystal and the grown crystal. Curve


42


illustrates the boundary of high crystalline quality material. The area to the right of curve


42


represents layers that have a large number of defects. With no lattice mismatch, it is theoretically possible to grow an infinitely thick, high quality epitaxial layer on the host crystal. As the mismatch in lattice constants increases, the thickness of achievable, high quality crystalline layer decreases rapidly. As a reference point, for example, if the lattice constants between the host crystal and the grown layer are mismatched by more than about 2%, monocrystalline epitaxial layers in excess of about 20 nm cannot be achieved. Semiconductor layer


22


can be a (100) or (111) oriented monocrystalline silicon and accommodating buffer layer


24


is a layer of strontium barium titanate. Substantial matching of lattice constants between these two materials is achieved by rotating the crystal orientation of the titanate material by 45° with respect to the crystal orientation of the silicon. The inclusion in the structure of amorphous interface layer


28


, a silicon oxide layer in this example, if it is of sufficient thickness, serves to reduce strain in the titanate monocrystalline layer that might result from any mismatch in the lattice constants of the host silicon and the grown titanate layer. As a result, a high quality, thick, monocrystalline titanate layer is achievable.




Still referring to

FIGS. 1-3

, layer


26


is a layer of epitaxially grown monocrystalline material and that crystalline material is also characterized by a crystal lattice constant and a crystal orientation. The lattice constant of layer


26


can differ from the lattice constant of semiconductor layer


22


. To achieve high crystalline quality in this epitaxially grown monocrystalline layer, the accommodating buffer layer must be of high crystalline quality. In addition, in order to achieve high crystalline quality in layer


26


, substantial matching between the crystal lattice constant of the host crystal, in this case, the monocrystalline accommodating buffer layer, and the grown crystal is desired. With properly selected materials this substantial matching of lattice constants is achieved as a result of rotation of the crystal orientation of the grown crystal with respect to the orientation of the host crystal. For example, if the grown crystal is gallium arsenide, aluminum gallium arsenide, zinc selenide, or zinc sulfur selenide and the accommodating buffer layer is monocrystalline Sr


x


Ba


l−x


TiO


3


, substantial matching of crystal lattice constants of the two materials is achieved, wherein the crystal orientation of the grown layer is rotated by 45° with respect to the orientation of the host monocrystalline oxide. Similarly, if the host material is a strontium or barium zirconate or a strontium or barium hafnate or barium tin oxide and the compound semiconductor layer is indium phosphide or gallium indium arsenide or aluminum indium arsenide, substantial matching of crystal lattice constants can be achieved by rotating the orientation of the grown crystal layer by 45° with respect to the host oxide crystal. In some instances, a crystalline semiconductor buffer layer between the host oxide and the grown monocrystalline material layer can be used to reduce strain in the grown monocrystalline material layer that might result from small differences in lattice constants. Better crystalline quality in the grown monocrystalline material layer can thereby be achieved.




The following example illustrates a process for fabricating a semiconductor structure such as the structures depicted in

FIGS. 1-3

. The process starts by providing a glass substrate having formed thereon regions of single-crystal (monocrystalline) silicon. In accordance with a preferred embodiment of the invention, the monocrystalline silicon regions have a (100) orientation. The silicon regions are preferably oriented on axis or, at most, about 4° off axis. At least a portion of the silicon substrate has a bare surface, although other portions of the silicon substrate, as described below, may encompass other structures. The term “bare” in this context means that the surface in the portions of the silicon substrate has been cleaned to remove any oxides, contaminants, or other foreign material.




In order to epitaxially grow a monocrystalline oxide layer overlying the monocrystalline silicon film, the native oxide layer must first be removed to expose the crystalline structure of the underlying film. The following process is preferably carried out by molecular beam epitaxy (MBE), although other epitaxial processes may also be used in accordance with the present invention. The native oxide can be removed by first thermally depositing a thin layer of strontium, barium, a combination of strontium and barium, or other alkaline earth metals or combinations of alkaline earth metals in an MBE apparatus. In the case where strontium is used, the silicon substrate is then heated to a temperature of about 750° C. to cause the strontium to react with the native silicon oxide layer. The strontium serves to reduce the silicon oxide to leave a silicon oxide-free surface. The resultant surface, which exhibits an ordered 2×1 structure, includes strontium, oxygen, and silicon. The ordered 2×1 structure forms a template for the ordered growth of an overlying layer of a monocrystalline oxide. The template provides the necessary chemical and physical properties to nucleate the crystalline growth of an overlying layer.




The native silicon oxide can be converted and the film surface can be prepared for the growth of a monocrystalline oxide layer by depositing an alkaline earth metal oxide, such as strontium oxide, strontium barium oxide, or barium oxide, onto the silicon substrate surface by MBE at a low temperature and by subsequently heating the structure to a temperature of about 750° C. At this temperature, a solid state reaction takes place between the strontium oxide and the native silicon oxide causing the reduction of the native silicon oxide and leaving an ordered 2×1 structure with strontium, oxygen, and silicon remaining on the silicon substrate surface. Again, this forms a template for the subsequent growth of an ordered monocrystalline oxide layer.




Following the removal of the silicon oxide from the surface of the film, the silicon substrate is cooled to a temperature in the range of about 200-800° C. and a layer of strontium titanate is grown on the template layer by molecular beam epitaxy. The MBE process is initiated by opening shutters in the MBE apparatus to expose strontium, titanium and oxygen sources. The ratio of strontium and titanium is approximately 1:1. The partial pressure of oxygen is initially set at a minimum value to grow stoichiometric strontium titanate at a growth rate of about 0.3-0.5 nm per minute. After initiating growth of the strontium titanate, the partial pressure of oxygen is increased above the initial minimum value. The overpressure of oxygen causes the growth of an amorphous silicon oxide layer at the interface between the underlying monocrystalline layer and the growing strontium titanate layer. The growth of the silicon oxide layer results from the diffusion of oxygen through the growing strontium titanate layer to the interface where the oxygen reacts with silicon at the surface of the underlying silicon substrate. The strontium titanate grows as an ordered (100) monocrystal with the (100) crystalline orientation rotated by 45° with respect to the underlying silicon substrate. Strain that otherwise might exist in the strontium titanate layer because of the small mismatch in lattice constant between the silicon substrate and the growing crystal is relieved in the amorphous silicon oxide intermediate layer.




After the strontium titanate layer has been grown to the desired thickness, the monocrystalline strontium titanate is capped by a template layer that is conducive to the subsequent growth of an epitaxial layer of a desired monocrystalline material. For example, for the subsequent growth of a monocrystalline compound semiconductor material layer of gallium arsenide, the MBE growth of the strontium titanate monocrystalline layer can be capped by terminating the growth with 1-2 monolayers of titanium, 1-2 monolayers of titanium-oxygen or with 1-2 monolayers of strontium-oxygen. Following the formation of this capping layer, arsenic is deposited to form a Ti—As bond, a Ti—O—As bond or a Sr—O—As. Any of these form an appropriate template for deposition and formation of a gallium arsenide monocrystalline layer. Following the formation of the template, gallium is subsequently introduced to the reaction with the arsenic and gallium arsenide forms. Alternatively, gallium can be deposited on the capping layer to form a Sr—O—Ga bond, and arsenic is subsequently introduced with the gallium to form the GaAs.





FIG. 21

is a high resolution Transmission Electron Micrograph (TEM) of semiconductor material using a bulk silicon substrate. Similar results are predicted for material manufactured using a monocrystalline silicon film formed over a glass layer. Single crystal SrTiO


3


accommodating buffer layer


24


was grown epitaxially on silicon semiconductor layer


22


. During this growth process, amorphous interfacial layer


28


is formed which relieves strain due to lattice mismatch. GaAs compound semiconductor layer


26


was then grown epitaxially using template layer


30


.





FIG. 22

illustrates an x-ray diffraction spectrum taken on a structure including GaAs monocrystalline layer


26


comprising GaAs grown on a bulk silicon substrate using accommodating buffer layer


24


. Similar results are predicted for material manufactured using a monocrystalline silicon film formed over a glass layer. The peaks in the spectrum indicate that both the accommodating buffer layer


24


and GaAs compound semiconductor layer


26


are single crystal and (100) orientated.




The structure illustrated in

FIG. 2

can be formed by the process discussed above with the addition of an additional buffer layer deposition step. The additional buffer layer


32


is formed overlying the template layer before the deposition of the monocrystalline material layer. If the buffer layer is a monocrystalline material comprising a compound semiconductor superlattice, such a superlattice can be deposited, by MBE for example, on the template described above. If instead the buffer layer is a monocrystalline material layer comprising a layer of germanium, the process above is modified to cap the strontium titanate monocrystalline layer with a final layer of either strontium or titanium and then by depositing germanium to react with the strontium or titanium. The germanium buffer layer can then be deposited directly on this template. Structure


34


, illustrated in

FIG. 3

, may be formed by growing an accommodating buffer layer, forming an amorphous oxide layer over semiconductor layer


22


, and growing semiconductor layer


38


over the accommodating buffer layer, as described above. The accommodating buffer layer and the amorphous oxide layer are then exposed to an anneal process sufficient to change the crystalline structure of the accommodating buffer layer from monocrystalline to amorphous, thereby forming an amorphous layer such that the combination of the amorphous oxide layer and the now amorphous accommodating buffer layer form a single amorphous oxide layer


36


. Layer


26


is then subsequently grown over layer


38


. Alternatively, the anneal process may be carried out subsequent to growth of layer


26


.




In accordance with one aspect of this embodiment, layer


36


is formed by exposing semiconductor layer


22


, the accommodating buffer layer, the amorphous oxide layer, and monocrystalline layer


38


to a rapid thermal anneal process with a peak temperature of about 700° C. to about 1000° C. and a process time of about 5 seconds to about 10 minutes. However, other suitable anneal processes may be employed to convert the accommodating buffer layer to an amorphous. For example, laser annealing, electron beam annealing, or “conventional” thermal annealing processes (in the proper environment) may be used to form layer


36


. When conventional thermal annealing is employed to form layer


36


, an overpressure of one or more constituents of layer


30


may be required to prevent degradation of layer


38


during the anneal process. For example, when layer


38


includes GaAs, the anneal environment preferably includes an overpressure of arsenic to mitigate degradation of layer


38


.




As noted above, layer


38


of structure


34


may include any materials suitable for either of layers


32


or


26


. Accordingly, any deposition or growth methods described in connection with either layer


32


or


26


, may be employed to deposit layer


38


.





FIG. 23

is a high resolution TEM of semiconductor material manufactured in accordance with the structure illustrated in

FIG. 3

, but using a bulk substrate. Similar results are predicted for material manufactured using a monocrystalline silicon film formed over a glass layer. In accordance with this structure, a single crystal SrTiO


3


accommodating buffer layer was grown epitaxially on the bulk substrate. During this growth process, an amorphous interfacial layer forms as described above. Next, additional monocrystalline layer


38


comprising a compound semiconductor layer of GaAs is formed above the accommodating buffer layer and the accommodating buffer layer is exposed to an anneal process to form amorphous oxide layer


36


.





FIG. 24

illustrates an x-ray diffraction spectrum taken on a structure including additional monocrystalline layer


38


comprising a GaAs compound semiconductor layer and amorphous oxide layer


36


formed on a bulk substrate. Similar results are predicted for material manufactured using a monocrystalline silicon film formed over a glass layer. The peaks in the spectrum indicate that GaAs compound semiconductor layer


38


is single crystal and (100) orientated and the lack of peaks around 40 to 50 degrees indicates that layer


36


is amorphous.




The process described above illustrates a process for forming a semiconductor structure including a silicon substrate, an overlying oxide layer, and a monocrystalline material layer comprising a gallium arsenide compound semiconductor layer by the process of molecular beam epitaxy. The process can also be carried out by the process of chemical vapor deposition (CVD), metal organic chemical vapor deposition (MOCVD), migration enhanced epitaxy (MEE), atomic layer epitaxy (ALE), physical vapor deposition (PVD), chemical solution deposition (CSD), pulsed laser deposition (PLD), or the like. Further, by a similar process, other monocrystalline accommodating buffer layers such as alkaline earth metal titanates, zirconates, hafnates, tantalates, vanadates, ruthenates, and niobates, alkaline earth metal tin-based perovskites, lanthanum aluminate, lanthanum scandium oxide, and gadolinium oxide can also be grown. Further, by a similar process such as MBE, other monocrystalline material layers comprising other III-V and II-VI monocrystalline compound semiconductors, semiconductors, metals and non-metals can be deposited overlying the monocrystalline oxide accommodating buffer layer.




Each of the variations of monocrystalline material layer and monocrystalline oxide accommodating buffer layer uses an appropriate template for initiating the growth of the monocrystalline material layer. For example, if the accommodating buffer layer is an alkaline earth metal zirconate, the oxide can be capped by a thin layer of zirconium. The deposition of zirconium can be followed by the deposition of arsenic or phosphorus to react with the zirconium as a precursor to depositing indium gallium arsenide, indium aluminum arsenide, or indium phosphide respectively. Similarly, if the monocrystalline oxide accommodating buffer layer is an alkaline earth metal hafnate, the oxide layer can be capped by a thin layer of hafnium. The deposition of hafnium is followed by the deposition of arsenic or phosphorous to react with the hafnium as a precursor to the growth of an indium gallium arsenide, indium aluminum arsenide, or indium phosphide layer, respectively. In a similar manner, strontium titanate can be capped with a layer of strontium or strontium and oxygen and barium titanate can be capped with a layer of barium or barium and oxygen. Each of these depositions can be followed by the deposition of arsenic or phosphorus to react with the capping material to form a template for the deposition of a monocrystalline material layer comprising compound semiconductors such as indium gallium arsenide, indium aluminum arsenide, or indium phosphide.




The formation of a device structure suitable for constructing lighting sources in accordance with another embodiment of the invention is illustrated schematically in cross-section in

FIGS. 25-28

. Like the previously described structures referred to in

FIGS. 1-3

, this structure involves the process of forming a compliant substrate utilizing the epitaxial growth of single crystal oxides, such as the formation of accommodating buffer layer


24


previously described with reference to

FIGS. 1 and 2

and amorphous layer


36


previously described with reference to

FIG. 3

, and the formation of a template layer


30


. However, the embodiment illustrated in

FIGS. 25-28

utilizes a template that includes a surfactant to facilitate layer-by-layer monocrystalline material growth.




Turning now to

FIG. 25

, a glass substrate


51


having a thermal oxide layer


69


and a semiconductor film


52


, formed as described above in connection with FIGS.


4


-


19


,is provided. An amorphous intermediate layer


58


is grown on semiconductor film


52


at the interface between the film


52


and a growing accommodating buffer layer


54


, which is preferably a monocrystalline crystal oxide layer, by the oxidation of film


52


during the growth of layer


54


. Layer


54


is preferably a monocrystalline oxide material such as a monocrystalline layer of Sr


z


Ba


l−z


TiO


3


where z ranges from 0 to 1. However, layer


54


may also comprise any of those compounds previously described with reference layer


24


in

FIGS. 1-2

and any of those compounds previously described with reference to layer


36


in

FIG. 3

which is formed from layers


24


and


28


referenced in

FIGS. 1 and 2

.




Layer


54


is grown with a strontium (Sr) terminated surface represented in

FIG. 25

by hatched line


55


which is followed by the addition of a template layer


60


which includes a surfactant layer


61


and capping layer


63


as illustrated in

FIGS. 26 and 27

. Surfactant layer


61


may comprise, but is not limited to, elements such as Al, In and Ga, but will be dependent upon the composition of layer


54


and the overlying layer of monocrystalline material for optimal results. In one exemplary embodiment, aluminum (Al) is used for surfactant layer


61


and functions to modify the surface and surface energy of layer


54


. Preferably, surfactant layer


61


is epitaxially grown, to a thickness of one to two monolayers, over layer


54


as illustrated in

FIG. 26

by way of molecular beam epitaxy (MBE), although other epitaxial processes may also be performed including chemical vapor deposition (CVD), metal organic chemical vapor deposition (MOCVD), migration enhanced epitaxy (MEE), atomic layer epitaxy (ALE), physical vapor deposition (PVD), chemical solution deposition (CSD), pulsed laser deposition (PLD), or the like.




Surfactant layer


61


is then exposed to a Group V element such as arsenic, for example, to form capping layer


63


as illustrated in FIG.


27


. Surfactant layer


61


may be exposed to a number of materials to create capping layer


63


such as elements which include, but are not limited to, As, P, Sb and N. Surfactant layer


61


and capping layer


63


combine to form template layer


60


.




Monocrystalline material layer


66


, which in this example is a compound semiconductor such as GaAs, is then deposited via MBE, CVD, MOCVD, MEE, ALE, PVD, CSD, PLD, and the like to form the final structure illustrated in FIG.


28


.





FIGS. 29-32

illustrate possible molecular bond structures for a specific example of a compound semiconductor structure formed in accordance with the structure illustrated in

FIGS. 25-28

. More specifically,

FIGS. 29-32

illustrate the growth of GaAs (layer


66


) on the strontium terminated surface of a strontium titanate monocrystalline oxide (layer


54


) using a surfactant containing template (layer


60


).




The growth of a monocrystalline material layer


66


such as GaAs on an accommodating buffer layer


54


such as a strontium titanium oxide over amorphous interface layer


58


and monocrystalline layer


52


, both of which may comprise materials previously described with reference to layers


28


and


22


, respectively in

FIGS. 1 and 2

, illustrates a critical thickness of about 1000 Angstroms where the two-dimensional (2D) and three-dimensional (3D) growth shifts because of the surface energies involved. In order to maintain a true layer by layer growth (Frank Van der Mere growth), the following relationship must be satisfied:






δ


STO


>(δ


INT





GaAs


)






where the surface energy of the monocrystalline oxide layer


54


must be greater than the surface energy of the amorphous interface layer


58


added to the surface energy of the GaAs layer


66


. Since it is impracticable to satisfy this equation, a surfactant containing template was used, as described above with reference to

FIGS. 26-28

, to increase the surface energy of the monocrystalline oxide layer


54


and also to shift the crystalline structure of the template to a diamond-like structure that is in compliance with the original GaAs layer.





FIG. 29

illustrates the molecular bond structure of a strontium terminated surface of a strontium titanate monocrystalline oxide layer. An aluminum surfactant layer is deposited on top of the strontium terminated surface and bonds with that surface as illustrated in

FIG. 30

, which reacts to form a capping layer comprising a monolayer of Al


2


Sr having the molecular bond structure illustrated in

FIG. 30

which forms a diamond-like structure with an sp


3


hybrid terminated surface that is compliant with compound semiconductors such as GaAs. The structure is then exposed to As to form a layer of AlAs as shown in FIG.


31


. GaAs is then deposited to complete the molecular bond structure illustrated in

FIG. 32

which has been obtained by 2D growth. The GaAs can be grown to any thickness for forming other semiconductor structures, devices, or integrated circuits. Alkaline earth metals such as those in Group IIA are those elements preferably used to form the capping surface of the monocrystalline oxide layer


54


because they are capable of forming a desired molecular structure with aluminum.




In this embodiment, a surfactant containing template layer aids in the formation of a compliant substrate for the monolithic integration of various material layers including those comprised of Group III-V compounds to form high quality semiconductor structures, devices and integrated circuits. For example, a surfactant containing template may be used for the monolithic integration of a monocrystalline material layer such as a layer comprising Germanium (Ge), for example, to form high efficiency photocells.




Turning now to

FIGS. 33-36

, the formation of a device structure is illustrated in cross-section. This structure utilizes the formation of a compliant substrate which relies on the epitaxial growth of single crystal oxides on silicon followed by the epitaxial growth of single crystal silicon onto the oxide.




A glass substrate


97


having a layer of thermal oxide deposited


77


thereon, and a region of monocrystalline layer


72


formed thereon as described above in connection with

FIGS. 4-19

is provided. An accommodating buffer layer


74


such as a monocrystalline oxide layer is grown on the monocrystalline layer layer


72


with an amorphous interface layer


78


as illustrated in FIG.


33


. Monocrystalline oxide layer


74


may be comprised of any of those materials previously discussed with reference to layer


24


in

FIGS. 1 and 2

, while amorphous interface layer


78


is preferably comprised of any of those materials previously described with reference to the layer


28


illustrated in

FIGS. 1 and 2

. Layer


72


, although preferably silicon, may also comprise any of those materials previously described with reference to semiconductor layer


22


in

FIGS. 1-3

.




Next, a silicon layer


81


is deposited over monocrystalline oxide layer


74


via MBE, CVD, MOCVD, MEE, ALE, PVD, CSD, PLD, and the like as illustrated in

FIG. 34

with a thickness of a few hundred Angstroms but preferably with a thickness of about 50 Angstroms. Monocrystalline oxide layer


74


preferably has a thickness of about 20 to 100 Angstroms.




Rapid thermal annealing is then conducted in the presence of a carbon source such as acetylene or methane, for example at a temperature within a range of about 800° C. to 1000° C. to form capping layer


82


and silicate amorphous layer


86


. However, other suitable carbon sources may be used as long as the rapid thermal annealing step functions to amorphize the monocrystalline oxide layer


74


into a silicate amorphous layer


86


and carbonize the top silicon layer


81


to form capping layer


82


which in this example would be a silicon carbide (SiC) layer as illustrated in FIG.


35


. The formation of amorphous layer


86


is similar to the formation of layer


36


illustrated in FIG.


3


and may comprise any of those materials described with reference to layer


36


in

FIG. 3

but the preferable material will be dependent upon the capping layer


82


used for silicon layer


81


.




Finally, a compound semiconductor layer


96


, such as gallium nitride (GaN) is grown over the SiC surface by way of MBE, CVD, MOCVD, MEE, ALE, PVD, CSD, PLD, or the like to form a high quality compound semicondcutor material for device formation. More specifically, the deposition of GaN and GaN based systems such as GaInN and AlGaN will result in the formation of dislocation nets confined at the silicon/amorphous region. The resulting nitride containing compound semiconductor material may comprise elements from groups III, IV and V of the periodic table and is defect free.




Although GaN has been grown on SiC bulk substrate in the past, this process possesses a one step formation of the compliant substrate containing a SiC top surface and an amorphous layer on a Si surface. More specifically, this structure uses an intermediate single crystal oxide layer that is amorphosized to form a silicate layer which adsorbs the strain between the layers. Moreover, unlike past use of a SiC bulk substrate, this structure is not limited by wafer size which is usually less than 50 mm in diameter for prior art SiC bulk substrates.




The monolithic integration of nitride containing semiconductor compounds containing group III-V nitrides and silicon devices can be used for high temperature RF applications and optoelectronics. GaN systems have particular use in the photonic industry for the blue/green and UV light sources and detection. High brightness light emitting diodes (LEDs) and lasers may also be formed within the GaN system.





FIGS. 37-39

schematically illustrate, in cross-section, the formation of another embodiment of a device structure. This embodiment includes a compliant layer that functions as a transition layer that uses clathrate or Zintl type bonding. More specifically, this arrangement utilizes an intermetallic template layer to reduce the surface energy of the interface between material layers thereby allowing for two dimensional layer by layer growth.




The structure illustrated in

FIG. 37

includes substrate


101


, such as glass or quartz, a thermal oxide layer


103


, a monocrystalline film


102


, an amorphous interface layer


108


and an accommodating buffer layer


104


. Amorphous interface layer


108


is formed on the monocrystalline film


102


at the interface between monocrystalline film


102


and accommodating buffer layer


104


as previously described with reference to

FIGS. 1 and 2

. Amorphous interface layer


108


may comprise any of those materials previously described with reference to amorphous interface layer


28


in

FIGS. 1 and 2

. The monocrystalline film


102


is preferably silicon but may also comprise any of those materials previously described with reference to semiconductor layer


22


in

FIGS. 1-3

.




A template layer


130


is deposited over accommodating buffer layer


104


as illustrated in FIG.


38


and preferably comprises a thin layer of Zintl type phase material composed of metals and metalloids having a great deal of ionic character. As in previously described embodiments, template layer


130


is deposited by way of MBE, CVD, MOCVD, MEE, ALE, PVD, CSD, PLD, or the like to achieve a thickness of one monolayer. Template layer


130


functions as a “soft” layer with non-directional bonding but high crystallinity which absorbs stress build up between layers having lattice mismatch. Materials for template


130


may include, but are not limited to, materials containing Si, Ga, In, and Sb such as, for example, AlSr


2


, (MgCaYb)Ga


2


, (Ca,Sr,Eu,Yb)In


2


, BaGe


2


As, and SrSn


2


As


2






A monocrystalline material layer


126


is epitaxially grown over template layer


130


to achieve the final structure illustrated in FIG.


39


. As a specific example, an SrAl


2


layer may be used as template layer


130


and an appropriate monocrystalline material layer


126


such as a compound semiconductor material GaAs is grown over the SrAl


2


. The Al—Ti (from the accommodating buffer layer of layer of Sr


z


Ba


l−z


TiO


3


where z ranges from 0 to 1) bond is mostly metallic while the Al—As (from the GaAs layer) bond is weakly covalent. The Sr participates in two distinct types of bonding with part of its electric charge going to the oxygen atoms in the lower accommodating buffer layer


104


comprising Sr


z


Ba


l−z


TiO


3


to participate in ionic bonding and the other part of its valence charge being donated to Al in a way that is typically carried out with Zintl phase materials. The amount of the charge transfer depends on the relative electronegativity of elements comprising the template layer


130


as well as on the interatomic distance. In this example, Al assumes an sp


3


hybridization and can readily form bonds with monocrystalline material layer


126


, which in this example, comprises compound semiconductor material GaAs.




The compliant substrate produced by use of the Zintl type template layer used in this embodiment can absorb a large strain without a significant energy cost. In the above example, the bond strength of the Al is adjusted by changing the volume of the SrAl


2


layer thereby making the device tunable for specific applications which include the monolithic integration of III-V and Si devices and the monolithic integration of high-k dielectric materials for CMOS technology.




Clearly, those embodiments specifically describing structures having compound semiconductor portions and Group IV semiconductor portions, are meant to illustrate embodiments of the present invention and not limit the present invention. There are a multiplicity of other combinations and other embodiments of the present invention. For example, the present invention includes structures and methods for fabricating material layers which form semiconductor structures, devices and integrated circuits including other layers such as metal and non-metal layers. More specifically, the invention includes structures and methods for forming a compliant substrate that is used in the fabrication of semiconductor structures, devices and integrated circuits and the material layers suitable for fabricating those structures, devices, and integrated circuits. By using embodiments of the present invention, it is now simpler to integrate devices that include monocrystalline layers comprising semiconductor and compound semiconductor materials as well as other material layers that are used to form those devices with other components that work better or are easily and/or inexpensively formed within semiconductor or compound semiconductor materials. This allows a device to be shrunk, the manufacturing costs to decrease, and yield and reliability to increase.




A glass or quartz substrate can be used in forming a monocrystalline material layer of a compound semiconductor or a non-compound semiconductor over the glass substrate, thereby forming a “handle” wafer having an essentially transparent nature. This type of wafer overcomes the fragile nature of compound semiconductor or other monocrystalline material wafers by placing semiconductor devices over a relatively more durable base material and allows for uses in which transparency is advantageous. When the wafer comprises monocrystalline silicon over glass, the unique techniques described herein also allow the formation of monocrystalline compound semiconductor materials over the silicon layer, allowing economical combinations of all electrical components, and particularly all active electronic devices, to be formed within or using the monocrystalline material layers even though the substrate itself may include a non-semiconductor material. Fabrication costs for compound semiconductor devices and other devices employing monocrystalline materials should decrease because larger substrates can be processed more economically and more readily compared to the relatively smaller and more fragile substrates (e.g. conventional compound semiconductor wafers).





FIG. 40

illustrates schematically, in cross section, a device structure


50


in accordance with a further embodiment. Device structure


50


includes glass or quartz substrate


51


, a thermal oxide layer


69


, such as silicon dioxide, and a monocrystalline semiconductor layer


52


, preferably a monocrystalline silicon region formed as described above in connection with

FIGS. 4-19

. Monocrystalline semiconductor layer


52


includes two regions,


53


and


57


. An electrical semiconductor component generally indicated by the dashed line


56


is formed, at least partially, in region


53


. Electrical component


56


can be a resistor, a capacitor, an active semiconductor component such as a diode or a transistor or an integrated circuit such as a CMOS integrated circuit. For example, electrical semiconductor component


56


can be a CMOS integrated circuit configured to perform digital signal processing or another function for which silicon integrated circuits are well suited. The electrical semiconductor component in region


53


can be formed by conventional semiconductor processing as well known and widely practiced in the semiconductor industry. A layer of insulating material


59


such as a layer of silicon dioxide or the like may overlie electrical semiconductor component


56


.




Insulating material


59


and any other layers that may have been formed or deposited during the processing of semiconductor component


56


in region


53


are removed from the surface of region


57


to provide a bare silicon surface in that region. As is well known, bare silicon surfaces are highly reactive and a native silicon oxide layer can quickly form on the bare surface. A layer of barium or barium and oxygen is deposited onto the native oxide layer on the surface of region


57


and is reacted with the oxidized surface to form a first template layer (not shown). In accordance with one embodiment, a monocrystalline oxide layer is formed overlying the template layer by a process of molecular beam epitaxy. Reactants including barium, titanium and oxygen are deposited onto the template layer to form the monocrystalline oxide layer. Initially during the deposition the partial pressure of oxygen is kept near the minimum necessary to fully react with the barium and titanium to form monocrystalline barium titanate layer. The partial pressure of oxygen is then increased to provide an overpressure of oxygen and to allow oxygen to diffuse through the growing monocrystalline oxide layer. The oxygen diffusing through the barium titanate reacts with silicon at the surface of region


57


to form an amorphous layer of silicon oxide


62


on second region


57


and at the interface between silicon layer


52


and the monocrystalline oxide layer


65


. Layers


65


and


62


may be subject to an annealing process as described above in connection with

FIG. 3

to form a single amorphous accommodating layer.




In accordance with an embodiment, the step of depositing the monocrystalline oxide layer


65


is terminated by depositing a second template layer


64


, which can be 1-10 monolayers of titanium, barium, barium and oxygen, or titanium and oxygen. A layer


66


of a monocrystalline compound semiconductor material is then deposited overlying second template layer


64


by a process of molecular beam epitaxy. The deposition of layer


66


is initiated by depositing a layer of arsenic onto template


64


. This initial step is followed by depositing gallium and arsenic to form monocrystalline gallium arsenide


66


. Alternatively, strontium can be substituted for barium in the above example.




In accordance with a further embodiment, a semiconductor component, generally indicated by a dashed line


68


is formed in compound semiconductor layer


66


. Semiconductor component


68


can be formed by processing steps conventionally used in the fabrication of gallium arsenide or other III-V compound semiconductor material devices. Semiconductor component


68


can be any active or passive component, and preferably is a semiconductor laser, light emitting diode, photodetector, heterojunction bipolar transistor (HBT), high frequency MESFET, or other component that utilizes and takes advantage of the physical properties of compound semiconductor materials. A metallic conductor schematically indicated by the line


70


can be formed to electrically couple device


68


and device


56


, thus implementing an integrated device that includes at least one component formed in silicon layer


52


and one device formed in monocrystalline compound semiconductor material layer


66


. Although illustrative structure


50


has been described as a structure formed on a silicon


52


and having a barium (or strontium) titanate layer


65


and a gallium arsenide layer


66


, similar devices can be fabricated using other monocrystalline substrates, monocrystalline oxide layers and other compound semiconductor layers as described elsewhere in this disclosure.





FIG. 41

illustrates a semiconductor structure


71


in accordance with a further embodiment. Structure


71


includes glass or quartz substrate


97


, a thermal oxide layer


77


, a monocrystalline semiconductor layer


73


such as a monocrystalline silicon film formed on the substrate


97


as described above in connection with

FIGS. 4-19

that includes a region


75


and a region


76


.




An electrical component schematically illustrated by the dashed line


79


is formed in region


75


using conventional silicon device processing techniques commonly used in the semiconductor industry. Using process steps similar to those described above, a monocrystalline oxide layer


80


and an intermediate amorphous silicon oxide layer


83


are formed overlying region


76


of layer


73


. A template layer


84


and subsequently a monocrystalline semiconductor layer


87


are formed overlying monocrystalline oxide layer


80


. In accordance with a further embodiment, an additional monocrystalline oxide layer


88


is formed overlying layer


87


by process steps similar to those used to form layer


80


, and an additional monocrystalline semiconductor layer


90


is formed overlying monocrystalline oxide layer


88


by process steps similar to those used to form layer


87


. In accordance with one embodiment, at least one of layers


87


and


90


are formed from a compound semiconductor material. Layers


80


and


83


may be subject to an annealing process as described above in connection with

FIG. 3

to form a single amorphous accommodating layer.




A semiconductor component generally indicated by a dashed line


92


is formed at least partially in monocrystalline semiconductor layer


87


. In accordance with one embodiment, semiconductor component


92


may include a field effect transistor having a gate dielectric formed, in part, by monocrystalline oxide layer


88


. In addition, monocrystalline semiconductor layer


90


can be used to implement the gate electrode of that field effect transistor. In accordance with one embodiment, monocrystalline semiconductor layer


87


is formed from a group III-V compound and semiconductor component


92


is a radio frequency amplifier that takes advantage of the high mobility characteristic of group III-V component materials. In accordance with yet a further embodiment, an electrical interconnection schematically illustrated by the line


94


electrically interconnects component


79


and component


92


. Structure


71


thus integrates components that take advantage of the unique properties of the two monocrystalline semiconductor materials.




Attention is now directed to a method for forming exemplary portions of illustrative composite semiconductor structures or composite integrated circuits like


50


or


71


. In particular, the illustrative composite semiconductor structure or integrated circuit


103


shown in

FIGS. 42-46

includes a compound semiconductor portion


1022


, a bipolar portion


1024


, and a MOS portion


1026


. In

FIG. 42

, a p-type doped, monocrystalline silicon layer


110


is provided over a thermal oxide layer


109


and a glass or quartz substrate


107


, formed according to the process described above in connection with

FIGS. 4-19

. The layer


110


has a compound semiconductor portion


1022


, a bipolar portion


1024


, and an MOS portion


1026


. Within bipolar portion


1024


, the monocrystalline silicon layer


110


is doped to form an N


+


buried region


1102


. A lightly p-type doped epitaxial monocrystalline silicon layer


1104


is then formed over the buried region


1102


and the substrate


110


. A doping step is then performed to create a lightly n-type doped drift region


1117


above the N


+


buried region


1102


. The doping step converts the dopant type of the lightly p-type epitaxial layer within a section of the bipolar region


1024


to a lightly n-type monocrystalline silicon region. A field isolation region


1106


is then formed between and around the bipolar portion


1024


and the MOS portion


1026


. A gate dielectric layer


1110


is formed over a portion of the epitaxial layer


1104


within MOS portion


1026


, and the gate electrode


1112


is then formed over the gate dielectric layer


1110


. Sidewall spacers


1115


are formed along vertical sides of the gate electrode


1112


and gate dielectric layer


1110


.




A p-type dopant is introduced into the drift region


1117


to form an active or intrinsic base region


1114


. An n-type, deep collector region


1108


is then formed within the bipolar portion


1024


to allow electrical connection to the buried region


1102


. Selective n-type doping is performed to form N


+


doped regions


1116


and the emitter region


1120


. N


+


doped regions


1116


are formed within layer


1104


along adjacent sides of the gate electrode


1112


and are source, drain, or source/drain regions for the MOS transistor. The N


+


doped regions


1116


and emitter region


1120


have a doping concentration of at least 1E19 atoms per cubic centimeter to allow ohmic contacts to be formed. A p-type doped region is formed to create the inactive or extrinsic base region


1118


which is a P


+


doped region (doping concentration of at least 1E19 atoms per cubic centimeter).




In the embodiment described, several processing steps have been performed but are not illustrated or further described, such as the formation of well regions, threshold adjusting implants, channel punch through prevention implants, field punch through prevention implants, as well as a variety of masking layers. The formation of the device up to this point in the process is performed using conventional steps. As illustrated, a standard N-channel MOS transistor has been formed within the MOS region


1026


, and a vertical NPN bipolar transistor has been formed within the bipolar portion


1024


. Although illustrated with a NPN bipolar transistor and a N-channel MOS transistor, device structures and circuits in accordance with various embodiments may additionally or alternatively include other electronic devices formed using the silicon substrate. As of this point, no circuitry has been formed within the compound semiconductor portion


1022


.




After the silicon devices are formed in regions


1024


and


1026


, a protective layer


1122


is formed overlying devices in regions


1024


and


1026


to protect devices in regions


1024


and


1026


from potential damage resulting from device formation in region


1022


. Layer


1122


may be formed of, for example, an insulating material such as silicon oxide or silicon nitride.




All of the layers that have been formed during the processing of the bipolar and MOS portions of the integrated circuit, except for epitaxial layer


1104


but including protective layer


1122


, are now removed from the surface of compound semiconductor portion


1022


. A bare silicon surface is thus provided for the subsequent processing of this portion, for example in the manner set forth above.




An accommodating buffer layer


124


is then formed over the layer


110


as illustrated in FIG.


43


. The accommodating buffer layer will form as a monocrystalline layer over the properly prepared (i.e., having the appropriate template layer) bare silicon surface in portion


1022


. The portion of layer


124


that forms over portions


1024


and


1026


, however, may be polycrystalline or amorphous because it is formed over a material that is not monocrystalline, and therefore, does not nucleate monocrystalline growth. The accommodating buffer layer


124


typically is a monocrystalline metal oxide or nitride layer and typically has a thickness in a range of approximately 2-100 nanometers. In one particular embodiment, the accommodating buffer layer is approximately 5-15 nm thick. During the formation of the accommodating buffer layer, an amorphous intermediate layer


122


is formed along the uppermost silicon surfaces of the integrated circuit


103


. This amorphous intermediate layer


122


typically includes an oxide of silicon and has a thickness and range of approximately 1-5 nm. In one particular embodiment, the thickness is approximately 2 nm. Following the formation of the accommodating buffer layer


124


and the amorphous intermediate layer


122


, a template layer


125


is then formed and has a thickness in a range of approximately one to ten monolayers of a material. In one particular embodiment, the material includes titanium-arsenic, strontium-oxygen-arsenic, or other similar materials as previously described with respect to

FIGS. 1-3

and


36


-


37


. A monocrystalline compound semiconductor layer


132


is then epitaxially grown overlying the monocrystalline portion of accommodating buffer layer


124


as shown in FIG.


44


. The portion of layer


132


that is grown over portions of layer


124


that are not monocrystalline may be polycrystalline or amorphous. The compound semiconductor layer can be formed by a number of methods and typically includes a material such as gallium arsenide, aluminum gallium arsenide, indium phosphide, or other compound semiconductor materials as previously mentioned. The thickness of the layer is in a range of approximately 1-5,000 nm, and more preferably 100-2000 nm. Furthermore, additional monocrystalline layers may be formed above layer


132


, as discussed in more detail below in connection with

FIGS. 31-32

.




In this particular embodiment, each of the elements within the template layer are also present in the accommodating buffer layer


124


, the monocrystalline compound semiconductor material


132


, or both. Therefore, the delineation between the template layer


125


and its two immediately adjacent layers disappears during processing. Therefore, when a transmission electron microscopy (TEM) photograph is taken, an interface between the accommodating buffer layer


124


and the monocrystalline compound semiconductor layer


132


is seen.




After at least a portion of layer


132


is formed in region


1022


, layers


122


, and


124


may be subject to an annealing process as described above in connection with

FIG. 3

to form a single amorphous accommodating layer. If only a portion of layer


132


is formed prior to the anneal process, the remaining portion may be deposited onto structure


103


prior to further processing.




At this point in time, sections of the compound semiconductor layer


132


and the accommodating buffer layer


124


(or of the amorphous accommodating layer if the annealing process described above has been carried out) are removed from portions overlying the bipolar portion


1024


and the MOS portion


1026


as shown in FIG.


45


. After the section of the compound semiconductor layer and the accommodating buffer layer


124


are removed, an insulating layer


142


is formed over protective layer


1122


. The insulating layer


142


can include a number of materials such as oxides, nitrides, oxynitrides, low-k dielectrics, or the like. As used herein, low-k is a material having a dielectric constant no higher than approximately 3.5. After the insulating layer


142


has been deposited, it is then polishedor etched to remove portions of the insulating layer


142


that overlie monocrystalline compound semiconductor layer


132


.




A transistor


144


is then formed within the monocrystalline compound semiconductor portion


1022


. A gate electrode


148


is then formed on the monocrystalline compound semiconductor layer


132


. Doped regions


146


are then formed within the monocrystalline compound semiconductor layer


132


. In this embodiment, the transistor


144


is a metal-semiconductor field-effect transistor (MESFET). If the MESFET is an n-type MESFET, the doped regions


146


and at least a portion of monocrystalline compound semiconductor layer


132


are also n-type doped. If a p-type MESFET were to be formed, then the doped regions


146


and at least a portion of monocrystalline compound semiconductor layer


132


would have just the opposite doping type. The heavier doped (N


+


) regions


146


allow ohmic contacts to be made to the monocrystalline compound semiconductor layer


132


. At this point in time, the active devices within the integrated circuit have been formed. Although not illustrated in the drawing figures, additional processing steps such as formation of well regions, threshold adjusting implants, channel punchthrough prevention implants, field punchthrough prevention implants, and the like may be performed in accordance with the present invention. This particular embodiment includes an n-type MESFET, a vertical NPN bipolar transistor, and a planar n-channel MOS transistor. Many other types of transistors, including P-channel MOS transistors, p-type vertical bipolar transistors, p-type MESFETs, and combinations of vertical and planar transistors, can be used. Also, other electrical components, such as resistors, capacitors, diodes, and the like, may be formed in one or more of the portions


1022


,


1024


, and


1026


.




Processing continues to form a substantially completed integrated circuit


103


as illustrated in FIG.


46


. An insulating layer


152


is formed over the layer


110


. The insulating layer


152


may include an etch-stop or polish-stop region that is not illustrated in

FIG. 46. A

second insulating layer


154


is then formed over the first insulating layer


152


. Portions of layers


154


,


152


,


142


,


124


, and


1122


are removed to define contact openings where the devices are to be interconnected. Interconnect trenches are formed within insulating layer


154


to provide the lateral connections between the contacts. As illustrated in

FIG. 46

, interconnect


1562


connects a source or drain region of the n-type MESFET within portion


1022


to the deep collector region


1108


of the NPN transistor within the bipolar portion


1024


. The emitter region


1120


of the NPN transistor is connected to one of the doped regions


1116


of the n-channel MOS transistor within the MOS portion


1026


. The other doped region


1116


is electrically connected to other portions of the integrated circuit that are not shown. Similar electrical connections are also formed to couple regions


1118


and


1112


to other regions of the integrated circuit.




A passivation layer


156


is formed over the interconnects


1562


,


1564


, and


1566


and insulating layer


154


. Other electrical connections are made to the transistors as illustrated as well as to other electrical or electronic components within the integrated circuit


103


but are not illustrated in the FIGS. Further, additional insulating layers and interconnects may be formed as necessary to form the proper interconnections between the various components within the integrated circuit


103


.




As can be seen from the previous embodiment, active devices for both compound semiconductor and Group IV semiconductor materials can be integrated into a single integrated circuit. Because there is some difficulty in incorporating both bipolar transistors and MOS transistors within a same integrated circuit, it may be possible to move some of the components within bipolar portion


1024


into the compound semiconductor portion


1022


or the MOS portion


1026


. Therefore, the requirement of special fabricating steps solely used for making a bipolar transistor can be eliminated. Therefore, there would only be a compound semiconductor portion and a MOS portion to the integrated circuit.




In still another embodiment, an integrated circuit can be formed such that it includes an optical laser in a compound semiconductor portion and an optical interconnect (waveguide) to a MOS transistor within a Group IV semiconductor region of the same integrated circuit.

FIG. 47-53

include illustrations of one embodiment.





FIG. 47

includes an illustration of a cross-section view of a portion of an integrated circuit


160


that includes a glass or quartz substrate


163


, a thermal oxide layer


165


, and a monocrystalline silicon layer


161


formed on the substrate


163


as described above in connection with

FIGS. 4-19

. An amorphous intermediate layer


162


and an accommodating buffer layer


164


, similar to those previously described, have been formed over layer


161


. Layers


162


and


164


may be subject to an annealing process as described above in connection with

FIG. 3

to form a single amorphous accommodating layer. In this specific embodiment, the layers needed to form the optical laser will be formed first, followed by the layers needed for the MOS transistor. In

FIG. 47

, the lower mirror layer


166


includes alternating layers of compound semiconductor materials. For example, the first, third, and fifth films within the optical laser may include a material such as gallium arsenide, and the second, fourth, and sixth films within the lower mirror layer


166


may include aluminum gallium arsenide or vice versa. Layer


168


includes the active region that will be used for photon generation. Upper mirror layer


170


is formed in a similar manner to the lower mirror layer


166


and includes alternating films of compound semiconductor materials. In one particular embodiment, the upper mirror layer


170


may be p-type doped compound semiconductor materials, and the lower mirror layer


166


may be n-type doped compound semiconductor materials.




Another accommodating buffer layer


172


, similar to the accommodating buffer layer


164


, is formed over the upper mirror layer


170


. In an alternative embodiment, the accommodating buffer layers


164


and


172


may include different materials. However, their function is essentially the same in that each is used for making a transition between a compound semiconductor layer and a monocrystalline Group IV semiconductor layer. Layer


172


may be subject to an annealing process as described above in connection with

FIG. 3

to form an amorphous accommodating layer. A monocrystalline Group IV semiconductor layer


174


is formed over the accommodating buffer layer


172


. In one particular embodiment, the monocrystalline Group IV semiconductor layer


174


includes germanium, silicon germanium, silicon germanium carbide, or the like.




In

FIG. 48

, the MOS portion is processed to form electrical components within this upper monocrystalline Group IV semiconductor layer


174


. As illustrated in

FIG. 48

, a field isolation region


171


is formed from a portion of layer


174


. A gate dielectric layer


173


is formed over the layer


174


, and a gate electrode


175


is formed over the gate dielectric layer


173


. Doped regions


177


are source, drain, or source/drain regions for the transistor


181


, as shown. Sidewall spacers


179


are formed adjacent to the vertical sides of the gate electrode


175


. Other components can be made within at least a part of layer


174


. These other components include other transistors (n-channel or p-channel), capacitors, transistors, diodes, and the like.




A monocrystalline Group IV semiconductor layer is epitaxially grown over one of the doped regions


177


. An upper portion


184


is P+ doped, and a lower portion


182


remains substantially intrinsic (undoped) as illustrated in FIG.


48


. The layer can be formed using a selective epitaxial process. In one embodiment, an insulating layer (not shown) is formed over the transistor


181


and the field isolation region


171


. The insulating layer is patterned to define an opening that exposes one of the doped regions


177


. At least initially, the selective epitaxial layer is formed without dopants. The entire selective epitaxial layer may be intrinsic, or a p-type dopant can be added near the end of the formation of the selective epitaxial layer. If the selective epitaxial layer is intrinsic, as formed, a doping step may be formed by implantation or by furnace doping. Regardless how the P+ upper portion


184


is formed, the insulating layer is then removed to form the resulting structure shown in FIG.


48


.




The next set of steps is performed to define the optical laser


180


as illustrated in FIG.


49


. The field isolation region


171


and the accommodating buffer layer


172


are removed over the compound semiconductor portion of the integrated circuit. Additional steps are performed to define the upper mirror layer


170


and active layer


168


of the optical laser


180


. The sides of the upper mirror layer


170


and active layer


168


are substantially coterminous.




Contacts


186


and


188


are formed for making electrical contact to the upper mirror layer


170


and the lower mirror layer


166


, respectively, as shown in FIG.


49


. Contact


186


has an annular shape to allow light (photons) to pass out of the upper mirror layer


170


into a subsequently formed optical waveguide.




An insulating layer


190


is then formed and patterned to define optical openings extending to the contact layer


186


and one of the doped regions


177


as shown in FIG.


50


. The insulating material can be any number of different materials, including an oxide, nitride, oxynitride, low-k dielectric, or any combination thereof. After defining the openings


192


, a higher refractive index material


202


is then formed within the openings to fill them and to deposit the layer over the insulating layer


190


as illustrated in FIG.


51


. With respect to the higher refractive index material


202


, “higher” is in relation to the material of the insulating layer


190


(i.e., material


202


has a higher refractive index compared to the insulating layer


190


). Optionally, a relatively thin lower refractive index film (not shown) could be formed before forming the higher refractive index material


202


. A hard mask layer


204


is then formed over the high refractive index layer


202


. Portions of the hard mask layer


204


, and high refractive index layer


202


are removed from portions overlying the opening and to areas closer to the sides of FIG.


51


.




The balance of the formation of the optical waveguide, which is an optical interconnect, is completed as illustrated in

FIG. 52. A

deposition procedure (possibly a dep-etch process) is performed to effectively create sidewalls sections


212


. In this embodiment, the sidewall sections


212


are made of the same material as material


202


. The hard mask layer


204


is then removed, and a low refractive index layer


214


(low relative to material


202


and layer


212


) is formed over the higher refractive index material


212


and


202


and exposed portions of the insulating layer


190


. The dash lines in

FIG. 52

illustrate the border between the high refractive index materials


202


and


212


. This designation is used to identify that both are made of the same material but are formed at different times.




Processing is continued to form a substantially completed integrated circuit as illustrated in

FIG. 53. A

passivation layer


220


is then formed over the optical laser


180


and MOSFET transistor


181


. Although not shown, other electrical or optical connections are made to the components within the integrated circuit but are not illustrated in FIG.


53


. These interconnects can include other optical waveguides or may include metallic interconnects.




In other embodiments, other types of lasers can be formed. For example, another type of laser can emit light (photons) horizontally instead of vertically. If light is emitted horizontally, the MOSFET transistor could be formed within the monocrystalline layer


161


, and the optical waveguide would be reconfigured, so that the laser is properly coupled (optically connected) to the transistor. In one specific embodiment, the optical waveguide can include at least a portion of the accommodating buffer layer. Other configurations are possible.




Clearly, these embodiments of integrated circuits having compound semiconductor portions and Group IV semiconductor portions, are meant to illustrate what can be done and are not intended to be exhaustive of all possibilities or to limit what can be done. There is a multiplicity of other possible combinations and embodiments. For example, the compound semiconductor portion may include light emitting diodes, photodetectors, diodes, or the like, and the Group IV semiconductor can include digital logic, memory arrays, and most structures that can be formed in conventional MOS integrated circuits. By using what is shown and described herein, it is now simpler to integrate devices that work better in compound semiconductor materials with other components that work better in Group IV semiconductor materials. This allows a device to be shrunk, the manufacturing costs to decrease, and yield and reliability to increase.




A composite integrated circuit may include components that provide electrical isolation when electrical signals are applied to the composite integrated circuit. The composite integrated circuit may include a pair of optical components, such as an optical source component and an optical detector component. An optical source component may be a light generating semiconductor device, such as an optical laser (e.g., the optical laser illustrated in FIG.


45


), a photo emitter, a diode, etc. An optical detector component may be a light-sensitive semiconductor junction device, such as a photodetector, a photodiode, a bipolar junction, a transistor, etc.




A composite integrated circuit may include processing circuitry that is formed at least partly in the Group IV semiconductor portion of the composite integrated circuit. The processing circuitry is configured to communicate with circuitry external to the composite integrated circuit. The processing circuitry may be electronic circuitry, such as a microprocessor, RAM, logic device, decoder, etc.




For the processing circuitry to communicate with external electronic circuitry, the composite integrated circuit may be provided with electrical signal connections with the external electronic circuitry. The composite integrated circuit may have internal optical communications connections for connecting the processing circuitry in the composite integrated circuit to the electrical connections with the external circuitry. Optical components in the composite integrated circuit may provide the optical communications connections which may electrically isolate the electrical signals in the communications connections from the processing circuitry. Together, the electrical and optical communications connections may be for communicating information, such as data, control, timing, etc.




A pair of optical components (an optical source component and an optical detector component) in the composite integrated circuit may be configured to pass information. Information that is received or transmitted between the optical pair may be from or for the electrical communications connection between the external circuitry and the composite integrated circuit. The optical components and the electrical communications connection may form a communications connection between the processing circuitry and the external circuitry while providing electrical isolation for the processing circuitry. If desired, a plurality of optical component pairs may be included in the composite integrated circuit for providing a plurality of communications connections and for providing isolation. For example, a composite integrated circuit receiving a plurality of data bits may include a pair of optical components for communication of each data bit.




In operation, for example, an optical source component in a pair of components may be configured to generate light (e.g., photons) based on receiving electrical signals from an electrical signal connection with the external circuitry. An optical detector component in the pair of components may be optically connected to the source component to generate electrical signals based on detecting light generated by the optical source component. Information that is communicated between the source and detector components may be digital or analog.




If desired the reverse of this configuration may be used. An optical source component that is responsive to the on-board processing circuitry may be coupled to an optical detector component to have the optical source component generate an electrical signal for use in communications with external circuitry. A plurality of such optical component pair structures may be used for providing two-way connections. In some applications where synchronization is desired, a first pair of optical components may be coupled to provide data communications and a second pair may be coupled for communicating synchronization information.




For clarity and brevity, optical detector components that are discussed below are discussed primarily in the context of optical detector components that have been formed in a compound semiconductor portion of a composite integrated circuit. In application, the optical detector component may be formed in many suitable ways (e.g., formed from silicon, etc.).




A composite integrated circuit will typically have an electric connection for a power supply and a ground connection. The power and ground connections are in addition to the communications connections that are discussed above. Processing circuitry in a composite integrated circuit may include electrically isolated communications connections and include electrical connections for power and ground. In most known applications, power supply and ground connections are usually well-protected by circuitry to prevent harmful external signals from reaching the composite integrated circuit. A communications ground may be isolated from the ground signal in communications connections that use a ground communications signal.





FIG. 54

illustrates schematically, in cross-section, a portion of a white light source device


600


in accordance with an embodiment of the invention. The white light source


600


includes a red panel


604


, a blue panel


606


, a green panel


608


, and an optional diffuser


602


. Each panel


604


-


608


includes a multitude of uniformly colored light-emitting semiconductor components, such as LEDs


610


-


614


. The panels


604


-


608


are stacked vertically in close proximity to one another so that they form a full color light source.




By placing arrays of single colored LEDs on separate panels, the manufacturing processes for the semiconductor panels can be simplified and optimized, thus reducing the overall cost of the full-color light source.




In the exemplary arrangement shown, the LEDs


610


-


614


are arranged in arrays on the panels, with the LED array of each panel horizontally offset from arrays of the other panels so that light emitted from the lower panels


606


-


608


is not blocked by the LEDs


610


-


612


of the upper panels


604


-


606


. The layers


161


,


162


,


164


, and


165


can be formed as described with reference to

FIGS. 47-51

and thin enough so that they do not significantly effect the passage of light therethrough. Alternatively, the layers


161


,


162


,


164


, and


165


can have cavities etched or formed therein to facilitate the transmission of light emitted from lower panels, as shown in FIG.


55


.




The diffuser


602


can be any suitable diffuser, such as a holographic diffuser, frosted glass, fresnel diffuser, or the like, or material for scattering the light emitted by the LEDs


610


-


614


so as to create white light.




For each panel


604


,


606


,


608


, plural LEDs


610


,


612


, or


614


are formed on a solid-state structure


169


. Other semiconductor structures, such as those shown in

FIGS. 1-3

,


25


-


28


, and


33


-


39


can alternatively be used in the panels


604


-


608


.




The structure


169


includes a glass or quartz substrate


163


, a thermal oxide layer


165


, and a monocrystalline silicon layer


161


formed on the substrate


163


as described above in connection with

FIGS. 4-19

. An amorphous intermediate layer


162


and an accommodating buffer layer


164


, similar to those previously described, have been formed over layer


161


. Layers


162


and


164


may be subject to an annealing process as described above in connection with

FIG. 3

to form a single amorphous accommodating layer.




By including panels of red, green, and blue LEDs formed using a low cost substrate having a large surface area, such as glass, the light source


600


can provide a solid-state white light source suitable for many conventional applications, such as room and display lighting. The solid-state light source


600


has significant advantages over conventional light sources, such as incandescent and fluorescent lighting, in that is more compact and rugged and, in some cases, more energy efficient.




The LEDs


610


-


614


can include conventional LED structures. The wavelength, and thus the color of light emitted by an LED or laser diode, depends on the bandgap energy E


g


. LEDs or laser diodes that emit light in the red-to-yellow spectrum have been available since the


1970


's. The red LEDs


610


consists of a conventional AlGaAs surface-emitting LED having an n type GaAs layer


620


, a n-AlGaAs layer


622


, a p-GaAs layer


624


, a p-AlGaAs layer


626


, and a p-GaAs layer


628


, and conductors


630


,


632


for providing current to the LEDs


610


.





FIG. 54

shows an LED structure for green LEDs


612


and blue LEDs


614


in which an InGaN active layer


642


,


662


is formed over a group III-V nitride layer


640


,


660


. The group III-V nitride layer


640


,


660


is formed on the buffer layer


164


. The group III-V nitride layer


640


,


660


is typically GaN. A second group III-V nitride layer


644


,


664


, such as AlGaN, is then formed on the InGaN active layer


642


,


662


. A third group III-V nitride layer


646


,


666


, such as an InGaN layer, is formed on the second group III-V layer


644


,


664


. The first group III-V nitride layer


640


,


660


is n-type doped. The second and third group III-V nitride layers


644


,


664


and


646


,


666


are p-type doped. P-electrodes


650


,


670


are formed on the third group III-V nitride layer


646


,


666


. N-electrodes


652


,


672


are formed on the first group III-V nitride layer


640


,


660


.





FIG. 55

illustrates schematically, in cross-section, a portion of a full-color display


703


in accordance with a further embodiment of the invention. The full-color display


703


can be used in display devices for presenting full-color images. A LED driver control (not shown), electrically connected to the LED electrodes


630


,


632


,


650


,


652


,


670


,


672


, can be included to individually activate various LEDs in the panels


604


-


608


to generate color images. The driver control circuitry and pixel transistors can be fabricated in the silicon layer


161


near the light-emitting components.




The diffuser


702


can be any suitable diffuser, such as a holographic diffuser, for providing a controlled viewing cone.




As shown in

FIG. 55

, cavities


701


can be etched or otherwise formed in the layers


161


,


162


, and


164


to facilitate the transmission of light emitted in LEDs from the lower panels


606


-


608


with reduced scattering and absorption.




Although three panels of LEDs are illustrated in

FIGS. 54-55

, a lighting source contemplated by the present invention is not so limited and can include two or more panels LEDs. Further, the wavelengths of the LEDs are not limited to red, green, and blue, and may be any color suitable for the application of the lighting device. In addition, other light emitting semiconductor components, such as laser diodes or VCSELs can be used instead of or in combination with LEDs.




Referring now to

FIG. 56

, a flow chart shows a process for fabricating a structure for producing light. The flow chart includes some of the steps used in the process. The details of how these steps are performed are described herein above. Other steps of the process are described herein above, or would be obvious to one of ordinary skill in the art. At step


5600


, a first glass substrate is provided, meaning it is prepared for use in equipment that can perform the next step of the process. At step


5605


, a first monocrystalline silicon layer is formed on the first glass. At step


5610


, a first monocrystalline perovskite oxide film is deposited overlying the first monocrystalline silicon layer, the film having a thickness less than a thickness of the material that would result in strain-induced defects. A first amorphous oxide interface layer containing at least silicon and oxygen is formed at step


5615


at an interface between the first monocrystalline perovskite oxide film and the first monocrystalline silicon layer. A first monocrystalline compound semiconductor layer is epitaxially formed at step


5620


, overlying the first monocrystalline perovskite oxide film. At step


5625


, a first light-emitting semiconductor component for emitting light at a first wavelength is formed, using the first monocrystalline compound semiconductor layer.




A second glass substrate is provided at step


5630


a for overlying the first glass substrate At step


5635


, a second monocrystalline silicon layer is formed on the second glass substrate. A second monocrystalline perovskite oxide film is deposited at step


5640


, overlying the second monocrystalline silicon layer, the film having a thickness less than a thickness of the material that would result in strain-induced defects. A second amorphous oxide interface layer containing at least silicon and oxygen is formed at an interface between the second monocrystalline perovskite oxide film and the second monocrystalline silicon layer at step


5645


. A second monocrystalline compound semiconductor layer is epitaxially formed at step


5650


, overlying the second monocrystalline perovskite oxide film. At step


5655


, a second light-emitting semiconductor component is formed a for emitting light at a second wavelength, using the second monocrystalline compound semiconductor layer. A third glass substrate is provided at step


5660


for overlying the second glass substrate. A third monocrystalline silicon layer is formed on the third glass substrate at step


5665


. A third monocrystalline perovskite oxide film is deposited at step


5670


, overlying the third monocrystalline silicon layer, the film having a thickness less than a thickness of the material that would result in strain-induced defects. At step


5675


, a third amorphous oxide interface layer is formed, containing at least silicon and oxygen at an interface between the third monocrystalline perovskite oxide film and the third monocrystalline silicon layer. At step


5680


, a third monocrystalline compound semiconductor layer is epitaxially forming overlying the third monocrystalline perovskite oxide film. A third light-emitting semiconductor component is formed at step


5685


, for emitting light at a third wavelength, using the third monocrystalline compound semiconductor layer.




In the foregoing specification, the invention has been described with reference to specific embodiments. However, one of ordinary skill in the art appreciates that various modifications and changes can be made without departing from the scope of the present invention as set forth in the claims below. Accordingly, the specification and figures are to be regarded in an illustrative rather than a restrictive sense, and all such modifications are intended to be included within the scope of present invention.




Benefits, other advantages, and solutions to problems have been described above with regard to specific embodiments. However, the benefits, advantages, solutions to problems, and any element(s) that may cause any benefit, advantage, or solution to occur or become more pronounced are not to be construed as a critical, required, or essential features or elements of any or all the claims. As used herein, the terms “comprises,” “comprising,” or any other variation thereof, are intended to cover a non-exclusive inclusion, such that a process, method, article, or apparatus that comprises a list of elements does not include only those elements but may include other elements not expressly listed or inherent to such process, method, article, or apparatus.



Claims
  • 1. A device for providing light, comprising:a first panel including: a first glass substrate; a first monocrystalline silicon layer formed on the first glass substrate; a first amorphous oxide material layer overlying the first monocrystalline silicon layer; a first monocrystalline perovskite oxide material layer overlying the first amorphous oxide matrial layer; a first monocrystalline compound semiconductor material layer overlying the first monocrystalline perovskite oxide material layer; and a first light-emitting semiconductor component, formed using the first monocrystalline compound semiconductor material layer, for emitting light at a first wavelength; and a second panel overlying the first panel, including: a second glass substrate; a second monocrystalline silicon layer formed on the second glass substrate; a second amorphous oxide material layer overlying the second monocrystalline silicon layer; a second monocrystalline perovskite oxide material layer overlying the second amorphous oxide material layer; a second monocrystalline compound semiconductor material layer overlying the second monocrystalline perovskite oxide material layer; and a second light-emitting semiconductor component, formed using the second monocrystalline compound semiconductor material layer, for emitting light at a second wavelength.
  • 2. The device of claim 1, further comprising:a third panel overlying the second panel, including: a third glass substrate; a third monocrystalline silicon layer formed on the third glass substrate; a third amorphous oxide material layer overlying the third monocrystalline silicon layer; a third monocrystalline perovskite oxide material layer overlying the third amorphous oxide material layer; a third monocrystalline compound semiconductor material layer overlying the third monocrystalline perovskite oxide material layer; and a third light-emitting semiconductor component, formed using the third monocrystalline compound semiconductor material layer, for emitting light at a third wavelength.
  • 3. The device of claim 2, wherein the first wavelength, the second wavelength, and the third wavelength have values selected so that white light is produced when emissions of the first light-emitting semiconductor component, the second light-emitting semiconductor component, and the third light-emitting semiconductor component are combined.
  • 4. The device of claim 1, further comprising:a diffuser overlying the third panel.
  • 5. The device of claim 1, wherein the first monocrystalline silicon layer and second monocrystalline silicon layer are formed on the first glass substrate and the second glass substrate, respectively, using a lateral solidification technique.
  • 6. A process for fabricating a structure for producing light, comprising:providing a first glass substrate; forming a first monocrystalline silicon layer on the first glass substrate; depositing a first monocrystalline perovskite oxide film overlying the first monocrystalline silicon layer, the film having a thickness less than a thickness of the material that would result in strain-induced defects; forming a first amorphous oxide interface layer containing at least silicon and oxygen at an interface between the first monocrystalline perovskite oxide film and the first monocrystalline silicon layer; epitaxially forming a first monocrystalline compound semiconductor layer overlying the first monocrystalline perovskite oxide film; forming a first light-emitting semiconductor component for emitting light at a first wavelength, using the first monocrystalline compound semiconductor layer; providing a second glass substrate for overlying the first glass substrate; forming a second monocrystalline silicon layer on the second glass substrate; depositing a second monocrystalline perovskite oxide film overlying the second monocrystalline silicon layer, the film having a thickness less than a thickness of the material that would result in strain-induced defects; forming a second amorphous oxide interface layer containing at least silicon and oxygen at an interface between the second monocrystalline perovskite oxide film and the second monocrystalline silicon layer; epitaxially forming a second monocrystalline compound semiconductor layer overlying the second monocrystalline perovskite oxide film; and forming a second light-emitting semiconductor component for emitting light at a second wavelength, using the second monocrystalline compound semiconductor layer.
  • 7. The process of claim 6, further comprising:providing a third glass substrate for overlying the second glass substrate; forming a third monocrystalline silicon layer on the third glass substrate; and depositing a third monocrystalline perovskite oxide film overlying the third monocrystalline silicon layer, the film having a thickness less than a thickness of the material that would result in strain-induced defects; forming a third amorphous oxide interface layer containing at least silicon and oxygen at an interface between the third monocrystalline perovskite oxide film and the third monocrystalline silicon layer; epitaxially forming a third monocrystalline compound semiconductor layer overlying the third monocrystalline perovskite oxide film; and forming a third light-emitting semiconductor component for emitting light at a third wavelength, using the third monocrystalline compound semiconductor layer.
  • 8. The process of claim 7, wherein the first wavelength, the second wavelength, and the third wavelength have values selected so that white light is produced when emissions of the first light-emitting semiconductor component, the second light-emitting semiconductor component, and the third light-emitting semiconductor component are combined.
  • 9. The process of claim 6, further comprising: providing a diffuser for overlying the third glass substrate.
  • 10. The process of claim 6, wherein the steps of forming first monocrystalline silicon layer and second monocrystalline silicon layer include applying a lateral solidification technique.
  • 11. The process of claim 6, wherein the steps of forming the first monocrystalline silicon layer includes:depositing a silicon film on the first glass substrate; irradiating a first portion of the silicon film so as to melt the silicon film in the first portion; permitting the melted silicon film in the first portion to solidify to form at least one silicon crystal; irradiating a second portion of the silicon film that at least partially overlaps the at least one silicon crystal so as to melt the silicon film in the second portion; and permitting the melted silicon film in the second portion to solidify to enlarge the at least one silicon crystal.
US Referenced Citations (447)
Number Name Date Kind
3670213 Nakawaga et al. Jun 1972 A
3766370 Walther Oct 1973 A
3802967 Ladany et al. Apr 1974 A
3914137 Huffman et al. Oct 1975 A
3935031 Adler Jan 1976 A
4006989 Andringa Feb 1977 A
4084130 Holton Apr 1978 A
4120588 Chaum Oct 1978 A
4146297 Alferness et al. Mar 1979 A
4174422 Matthews et al. Nov 1979 A
4242595 Lehovec Dec 1980 A
4284329 Smith et al. Aug 1981 A
4289920 Hovel Sep 1981 A
4297656 Pan Oct 1981 A
4392297 Little Jul 1983 A
4398342 Pitt et al. Aug 1983 A
4404265 Manasevit Sep 1983 A
4424589 Thomas et al. Jan 1984 A
4439014 Stacy et al. Mar 1984 A
4442590 Stockton et al. Apr 1984 A
4452720 Harada et al. Jun 1984 A
4459325 Nozawa et al. Jul 1984 A
4482422 McGinn et al. Nov 1984 A
4482906 Hovel et al. Nov 1984 A
4484332 Hawrylo Nov 1984 A
4503540 Nakashima et al. Mar 1985 A
4523211 Morimoto et al. Jun 1985 A
4594000 Falk et al. Jun 1986 A
4629821 Bronstein-Bonte et al. Dec 1986 A
4661176 Manasevit Apr 1987 A
4667088 Kramer May 1987 A
4667212 Nakamura May 1987 A
4681982 Yoshida Jul 1987 A
4748485 Vasudev May 1988 A
4756007 Qureshi et al. Jul 1988 A
4772929 Manchester et al. Sep 1988 A
4773063 Hunsperger et al. Sep 1988 A
4774205 Choi et al. Sep 1988 A
4777613 Shahan et al. Oct 1988 A
4793872 Meunier et al. Dec 1988 A
4802182 Thornton et al. Jan 1989 A
4815084 Scifres et al. Mar 1989 A
4841775 Ikeda et al. Jun 1989 A
4845044 Ariyoshi et al. Jul 1989 A
4846926 Kay et al. Jul 1989 A
4855249 Akasaki et al. Aug 1989 A
4868376 Lessin et al. Sep 1989 A
4872046 Morkoc et al. Oct 1989 A
4876208 Gustafson et al. Oct 1989 A
4876219 Eshita et al. Oct 1989 A
4882300 Inoue et al. Nov 1989 A
4885376 Verkade Dec 1989 A
4888202 Murakami et al. Dec 1989 A
4889402 Reinhart Dec 1989 A
4891091 Shastry Jan 1990 A
4896194 Suzuki Jan 1990 A
4901133 Curran et al. Feb 1990 A
4910164 Shichijo Mar 1990 A
4912087 Aslam et al. Mar 1990 A
4928154 Umeno et al. May 1990 A
4934777 Jou et al. Jun 1990 A
4952420 Walters Aug 1990 A
4959702 Moyer et al. Sep 1990 A
4963508 Umeno et al. Oct 1990 A
4963949 Wanlass et al. Oct 1990 A
4965649 Zanio et al. Oct 1990 A
4981714 Ohno et al. Jan 1991 A
4984043 Vinal Jan 1991 A
4999842 Huang et al. Mar 1991 A
5018816 Murray et al. May 1991 A
5028976 Ozaki et al. Jul 1991 A
5051790 Hammer Sep 1991 A
5053835 Horikawa et al. Oct 1991 A
5055445 Belt et al. Oct 1991 A
5055835 Sutton Oct 1991 A
5060031 Abrokwah et al. Oct 1991 A
5063081 Cozzette et al. Nov 1991 A
5063166 Mooney et al. Nov 1991 A
5067809 Tsubota Nov 1991 A
5073981 Giles et al. Dec 1991 A
5075743 Behfar-Rad Dec 1991 A
5081062 Vasudev et al. Jan 1992 A
5081519 Nishimura et al. Jan 1992 A
5103494 Mozer Apr 1992 A
5116461 Lebby et al. May 1992 A
5119448 Schaefer et al. Jun 1992 A
5122852 Chang et al. Jun 1992 A
5127067 Delcoco et al. Jun 1992 A
5130762 Kulick Jul 1992 A
5132648 Trinh et al. Jul 1992 A
5140651 Soref et al. Aug 1992 A
5141894 Bisaro et al. Aug 1992 A
5143854 Pirrung et al. Sep 1992 A
5144409 Ma Sep 1992 A
5155658 Inam et al. Oct 1992 A
5159413 Calviello et al. Oct 1992 A
5163118 Lorenzo et al. Nov 1992 A
5173474 Connell et al. Dec 1992 A
5173835 Cornett et al. Dec 1992 A
5181085 Moon et al. Jan 1993 A
5185589 Krishnaswamy et al. Feb 1993 A
5191625 Gustavsson Mar 1993 A
5194397 Cook et al. Mar 1993 A
5194917 Regener Mar 1993 A
5198269 Swartz et al. Mar 1993 A
5208182 Narayan et al. May 1993 A
5210763 Lewis et al. May 1993 A
5216729 Berger et al. Jun 1993 A
5221367 Chisholm et al. Jun 1993 A
5225031 McKee et al. Jul 1993 A
5227196 Itoh Jul 1993 A
5244818 Jokers et al. Sep 1993 A
5248564 Ramesh Sep 1993 A
5260394 Tazaki et al. Nov 1993 A
5266355 Wernberg et al. Nov 1993 A
5270298 Ramesh Dec 1993 A
5280013 Newman et al. Jan 1994 A
5281834 Cambou et al. Jan 1994 A
5283462 Stengel Feb 1994 A
5286985 Taddiken Feb 1994 A
5293050 Chapple-Sokol et al. Mar 1994 A
5306649 Hebert Apr 1994 A
5310707 Oishi et al. May 1994 A
5312765 Kanber May 1994 A
5314547 Heremans et al. May 1994 A
5323023 Fork Jun 1994 A
5326721 Summerfelt Jul 1994 A
5334556 Guldi Aug 1994 A
5352926 Andrews Oct 1994 A
5356509 Terranova et al. Oct 1994 A
5356831 Calviello et al. Oct 1994 A
5357122 Okubora et al. Oct 1994 A
5358925 Neville Connell et al. Oct 1994 A
5371734 Fischer Dec 1994 A
5372992 Itozaki et al. Dec 1994 A
5373166 Buchan et al. Dec 1994 A
5391515 Kao et al. Feb 1995 A
5393352 Summerfelt Feb 1995 A
5394489 Koch Feb 1995 A
5395663 Tabata et al. Mar 1995 A
5397428 Stoner et al. Mar 1995 A
5399898 Rostoker Mar 1995 A
5404581 Honjo Apr 1995 A
5405802 Yamagata et al. Apr 1995 A
5406202 Mehrgardt et al. Apr 1995 A
5418216 Fork May 1995 A
5418389 Watanabe May 1995 A
5420102 Harshavardhan et al. May 1995 A
5427988 Sengupta et al. Jun 1995 A
5436759 Dijaii et al. Jul 1995 A
5438584 Paoli et al. Aug 1995 A
5441577 Sasaki et al. Aug 1995 A
5442191 Ma Aug 1995 A
5442561 Yoshizawa et al. Aug 1995 A
5444016 Abrokwah et al. Aug 1995 A
5450812 McKee et al. Sep 1995 A
5452118 Maruska Sep 1995 A
5453727 Shibasaki et al. Sep 1995 A
5466631 Ichikawa et al. Nov 1995 A
5473047 Shi Dec 1995 A
5473171 Summerfelt Dec 1995 A
5478653 Guenzer Dec 1995 A
5479033 Baca et al. Dec 1995 A
5479317 Ramesh Dec 1995 A
5480829 Abrokwah et al. Jan 1996 A
5481102 Hazelrigg, Jr. Jan 1996 A
5482003 McKee et al. Jan 1996 A
5484664 Kitahara et al. Jan 1996 A
5486406 Shi Jan 1996 A
5491461 Partin et al. Feb 1996 A
5492859 Sakaguchi et al. Feb 1996 A
5494711 Takeda et al. Feb 1996 A
5504035 Rostoker et al. Apr 1996 A
5504183 Shi Apr 1996 A
5511238 Bayraktaroglu Apr 1996 A
5512773 Wolf et al. Apr 1996 A
5514484 Nashimoto May 1996 A
5514904 Onga et al. May 1996 A
5515047 Yamakido et al. May 1996 A
5515810 Yamashita et al. May 1996 A
5516725 Chang et al. May 1996 A
5519235 Ramesh May 1996 A
5528057 Yanagase et al. Jun 1996 A
5528067 Farb et al. Jun 1996 A
5528414 Oakley Jun 1996 A
5530235 Stefik et al. Jun 1996 A
5538941 Findikoglu et al. Jul 1996 A
5541422 Wolf et al. Jul 1996 A
5549977 Jin et al. Aug 1996 A
5551238 Prueitt Sep 1996 A
5552547 Shi Sep 1996 A
5553089 Seki et al. Sep 1996 A
5556463 Guenzer Sep 1996 A
5561305 Smith Oct 1996 A
5569953 Kikkawa et al. Oct 1996 A
5572052 Kashihara et al. Nov 1996 A
5576879 Nashimoto Nov 1996 A
5588995 Sheldon Dec 1996 A
5589284 Summerfelt et al. Dec 1996 A
5596205 Reedy et al. Jan 1997 A
5596214 Endo Jan 1997 A
5602418 Imai et al. Feb 1997 A
5603764 Matsuda et al. Feb 1997 A
5606184 Abrokwah et al. Feb 1997 A
5608046 Cook et al. Mar 1997 A
5610744 Ho et al. Mar 1997 A
5614739 Abrokwah et al. Mar 1997 A
5619051 Endo Apr 1997 A
5621227 Joshi Apr 1997 A
5623439 Gotoh et al. Apr 1997 A
5623552 Lane Apr 1997 A
5629534 Inuzuka et al. May 1997 A
5633724 King et al. May 1997 A
5635433 Sengupta Jun 1997 A
5640267 May et al. Jun 1997 A
5650646 Summerfelt Jul 1997 A
5656382 Nashimoto Aug 1997 A
5659180 Shen et al. Aug 1997 A
5661112 Hatta et al. Aug 1997 A
5668048 Kondo et al. Sep 1997 A
5670798 Schetzina Sep 1997 A
5670800 Nakao et al. Sep 1997 A
5674366 Hayashi et al. Oct 1997 A
5679965 Schetzina Oct 1997 A
5682046 Takahashi et al. Oct 1997 A
5686741 Ohori et al. Nov 1997 A
5689123 Major et al. Nov 1997 A
5725641 MacLeod Mar 1998 A
5729394 Sevier et al. Mar 1998 A
5729641 Chandonnet et al. Mar 1998 A
5731220 Tsu et al. Mar 1998 A
5733641 Fork et al. Mar 1998 A
5734672 McMinn et al. Mar 1998 A
5735949 Mantl et al. Apr 1998 A
5739552 Kimura et al. Apr 1998 A
5741724 Ramdani et al. Apr 1998 A
5745631 Reinker Apr 1998 A
5753300 Wessels et al. May 1998 A
5753928 Krause May 1998 A
5754319 Van De Voorde et al. May 1998 A
5760426 Marx et al. Jun 1998 A
5760427 Onda Jun 1998 A
5764676 Paoli et al. Jun 1998 A
5767543 Ooms et al. Jun 1998 A
5770887 Tadatomo et al. Jun 1998 A
5776359 Schultz et al. Jul 1998 A
5776621 Nashimoto Jul 1998 A
5777350 Nakamura et al. Jul 1998 A
5777762 Yamamoto Jul 1998 A
5778018 Yoshikawa et al. Jul 1998 A
5778116 Tomich Jul 1998 A
5780311 Beasom et al. Jul 1998 A
5789733 Jachimowicz et al. Aug 1998 A
5789845 Wadaka et al. Aug 1998 A
5790583 Ho Aug 1998 A
5792569 Sun et al. Aug 1998 A
5792679 Nakato Aug 1998 A
5796648 Kawakubo et al. Aug 1998 A
5801072 Barber Sep 1998 A
5801105 Yano et al. Sep 1998 A
5807440 Kubota et al. Sep 1998 A
5810923 Yano et al. Sep 1998 A
5812272 King et al. Sep 1998 A
5814583 Itozaki et al. Sep 1998 A
5825055 Summerfelt Oct 1998 A
5825799 Ho et al. Oct 1998 A
5827755 Yonchara et al. Oct 1998 A
5828080 Yano et al. Oct 1998 A
5830270 McKee et al. Nov 1998 A
5833603 Kovacs et al. Nov 1998 A
5834362 Miyagaki et al. Nov 1998 A
5838035 Ramesh Nov 1998 A
5844260 Ohori Dec 1998 A
5846846 Suh et al. Dec 1998 A
5852687 Wickham Dec 1998 A
5857049 Beranek et al. Jan 1999 A
5858814 Goossen et al. Jan 1999 A
5861966 Ortel Jan 1999 A
5863326 Nause et al. Jan 1999 A
5869845 Vander Wagt et al. Feb 1999 A
5872493 Ella Feb 1999 A
5873977 Desu et al. Feb 1999 A
5874860 Brunel et al. Feb 1999 A
5879956 Seon et al. Mar 1999 A
5880452 Plesko Mar 1999 A
5883564 Partin Mar 1999 A
5883996 Knapp et al. Mar 1999 A
5886867 Chivukula et al. Mar 1999 A
5888296 Ooms et al. Mar 1999 A
5889296 Imamura et al. Mar 1999 A
5896476 Wisseman et al. Apr 1999 A
5907792 Droopad et al. May 1999 A
5912068 Jia Jun 1999 A
5926493 O'Brien et al. Jul 1999 A
5926496 Ho et al. Jul 1999 A
5937274 Kondow et al. Aug 1999 A
5937285 Abrokwah et al. Aug 1999 A
5948161 Kizuki Sep 1999 A
5953468 Finnila et al. Sep 1999 A
5955591 Imbach et al. Sep 1999 A
5959879 Koo Sep 1999 A
5962069 Schindler et al. Oct 1999 A
5963291 Wu et al. Oct 1999 A
5966323 Chen et al. Oct 1999 A
5977567 Verdiell Nov 1999 A
5981400 Lo Nov 1999 A
5981976 Murasato Nov 1999 A
5981980 Miyajima et al. Nov 1999 A
5984190 Nevill Nov 1999 A
5987011 Toh Nov 1999 A
5990495 Ohba Nov 1999 A
5995359 Klee et al. Nov 1999 A
5995528 Fukunaga et al. Nov 1999 A
6002375 Corman et al. Dec 1999 A
6008762 Nghiem Dec 1999 A
6011641 Shin et al. Jan 2000 A
6011646 Mirkarimi et al. Jan 2000 A
6013553 Wallace et al. Jan 2000 A
6020222 Wollesen Feb 2000 A
6022140 Fraden et al. Feb 2000 A
6022410 Yu et al. Feb 2000 A
6022963 McGall et al. Feb 2000 A
6023082 McKee et al. Feb 2000 A
6028853 Haartsen Feb 2000 A
6039803 Fitzgerald et al. Mar 2000 A
6045626 Yano et al. Apr 2000 A
6046464 Schetzina Apr 2000 A
6048751 D'Asaro et al. Apr 2000 A
6049702 Tham et al. Apr 2000 A
6051858 Uchida et al. Apr 2000 A
6055179 Koganei et al. Apr 2000 A
6058131 Pan May 2000 A
6064078 Northrup et al. May 2000 A
6064092 Park May 2000 A
6078717 Nashimoto et al. Jun 2000 A
6083697 Beecher et al. Jul 2000 A
6087681 Shakuda Jul 2000 A
6088216 Laibowitz et al. Jul 2000 A
6090659 Laibowitz et al. Jul 2000 A
6093302 Montgomery Jul 2000 A
6096584 Ellis-Monaghan et al. Aug 2000 A
6100578 Suzuki Aug 2000 A
6103008 McKee et al. Aug 2000 A
6103403 Grigorian et al. Aug 2000 A
6107653 Fitzgerald Aug 2000 A
6107721 Lakin Aug 2000 A
6108125 Yano Aug 2000 A
6113690 Yu et al. Sep 2000 A
6114996 Nghiem Sep 2000 A
6121642 Newns Sep 2000 A
6121647 Yano et al. Sep 2000 A
6128178 Newns Oct 2000 A
6134114 Ungermann et al. Oct 2000 A
6136666 So Oct 2000 A
6137603 Henmi Oct 2000 A
6139483 Seabaugh et al. Oct 2000 A
6143072 McKee et al. Nov 2000 A
6143366 Lu Nov 2000 A
6146906 Inoue et al. Nov 2000 A
6150239 Goesele et al. Nov 2000 A
6153010 Kiyoku et al. Nov 2000 A
6153454 Krivokapic Nov 2000 A
6156581 Vaudo et al. Dec 2000 A
6173474 Conrad Jan 2001 B1
6174755 Manning Jan 2001 B1
6175497 Tseng et al. Jan 2001 B1
6175555 Hoole Jan 2001 B1
6180252 Farrell et al. Jan 2001 B1
6180486 Leobandung et al. Jan 2001 B1
6184044 Sone et al. Feb 2001 B1
6184144 Lo Feb 2001 B1
6191011 Gilboa et al. Feb 2001 B1
6194753 Seon et al. Feb 2001 B1
6197503 Vo-Dinh et al. Mar 2001 B1
6204737 Ella Mar 2001 B1
6208453 Wessels et al. Mar 2001 B1
6210988 Howe et al. Apr 2001 B1
6211096 Allman et al. Apr 2001 B1
6222654 Frigo Apr 2001 B1
6224669 Yi et al. May 2001 B1
6225051 Sugiyama et al. May 2001 B1
6229159 Suzuki May 2001 B1
6232910 Bell et al. May 2001 B1
6235145 Li et al. May 2001 B1
6238946 Ziegler May 2001 B1
6239449 Fafard et al. May 2001 B1
6253649 Kawahara et al. May 2001 B1
6241821 Yu et al. Jun 2001 B1
6242686 Kishimoto et al. Jun 2001 B1
6248459 Wang et al. Jun 2001 B1
6248621 Wilk et al. Jun 2001 B1
6252261 Usui et al. Jun 2001 B1
6255198 Linthicum et al. Jul 2001 B1
6256426 Duchet Jul 2001 B1
6265749 Gardner et al. Jul 2001 B1
6268269 Lee et al. Jul 2001 B1
6271619 Yamada et al. Aug 2001 B1
6275122 Speidell et al. Aug 2001 B1
6277436 Stauf et al. Aug 2001 B1
6278137 Shimoyama et al. Aug 2001 B1
6278138 Suzuki Aug 2001 B1
6278523 Gorecki Aug 2001 B1
6291319 Yu et al. Sep 2001 B1
6297842 Koizumi et al. Oct 2001 B1
6300615 Shinohara et al. Oct 2001 B1
6306668 McKee et al. Oct 2001 B1
6312819 Jia et al. Nov 2001 B1
6313486 Kencke et al. Nov 2001 B1
6316785 Nunoue et al. Nov 2001 B1
6316832 Tsuzuki et al. Nov 2001 B1
6319730 Ramdani et al. Nov 2001 B1
6320238 Kizilyalli et al. Nov 2001 B1
6326637 Parkin et al. Dec 2001 B1
6326645 Kadota Dec 2001 B1
6338756 Dietze Jan 2002 B2
6339664 Farjady et al. Jan 2002 B1
6340788 King et al. Jan 2002 B1
6343171 Yoshimura et al. Jan 2002 B1
6345424 Hasegawa et al. Feb 2002 B1
6348373 Ma et al. Feb 2002 B1
6359330 Goudard Mar 2002 B1
6362017 Manabe et al. Mar 2002 B1
6367699 Ackley Apr 2002 B2
6372356 Thornton et al. Apr 2002 B1
6372813 Johnson et al. Apr 2002 B1
6389209 Suhir May 2002 B1
6391674 Ziegler May 2002 B2
6392257 Ramdani et al. May 2002 B1
6393167 Davis et al. May 2002 B1
6404027 Hong et al. Jun 2002 B1
6410941 Taylor et al. Jun 2002 B1
6410947 Wada Jun 2002 B1
6411756 Sadot et al. Jun 2002 B2
6417059 Huang Jul 2002 B2
6427066 Grube Jul 2002 B1
6432546 Ramesh et al. Aug 2002 B1
6438281 Tsukamoto et al. Aug 2002 B1
6461927 Mochizuki et al. Oct 2002 B1
6462360 Higgins, Jr. et al. Oct 2002 B1
20010013313 Droopad et al. Aug 2001 A1
20020006245 Kubota et al. Jan 2002 A1
20020008234 Emrick Jan 2002 A1
20020030246 Eisenbeiser et al. Mar 2002 A1
20020047123 Ramdani et al. Apr 2002 A1
20020047143 Ramdani et al. Apr 2002 A1
20020072245 Ooms et al. Jun 2002 A1
20020131675 Litvin Sep 2002 A1
Foreign Referenced Citations (114)
Number Date Country
196 07 107 Aug 1997 DE
197 12 496 Oct 1997 DE
100 17 137 Oct 2000 DE
0 250 171 Dec 1987 EP
0 300 499 Jan 1989 EP
0 309 270 Mar 1989 EP
0 331 467 Sep 1989 EP
0 342 937 Nov 1989 EP
0 455 526 Jun 1991 EP
0 483 993 May 1992 EP
0 514 018 Nov 1992 EP
0 538 611 Apr 1993 EP
0 581 239 Feb 1994 EP
0 602 568 Jun 1994 EP
0 607 435 Jul 1994 EP
0 630 057 Dec 1994 EP
0 682 266 Nov 1995 EP
0 711 853 May 1996 EP
0 777 379 Jun 1997 EP
0 810 666 Dec 1997 EP
0 875 922 Nov 1998 EP
0 881 669 Dec 1998 EP
0 884 767 Dec 1998 EP
0 926 739 Jun 1999 EP
0 957 522 Nov 1999 EP
0 964 259 Dec 1999 EP
0 964 453 Dec 1999 EP
0 993 027 Apr 2000 EP
0 999 600 May 2000 EP
1 001 468 May 2000 EP
1 043 426 Oct 2000 EP
1 043 765 Oct 2000 EP
1 069 606 Jan 2001 EP
1 085 319 Mar 2001 EP
1 109 212 Jun 2001 EP
2 779 843 Dec 1999 FR
1 319 311 Jun 1970 GB
2 335 792 Sep 1999 GB
52-88354 Jul 1977 JP
52-89070 Jul 1977 JP
52-135684 Nov 1977 JP
54-134554 Oct 1979 JP
55-87424 Jul 1980 JP
58-075868 May 1983 JP
58-213412 Dec 1983 JP
60-210018 Oct 1985 JP
60-212018 Oct 1985 JP
61-36981 Feb 1986 JP
61-63015 Apr 1986 JP
61-108187 May 1986 JP
63-34994 Feb 1988 JP
63-131104 Jun 1988 JP
63-198365 Aug 1988 JP
63-289812 Nov 1988 JP
64-50575 Feb 1989 JP
64-52329 Feb 1989 JP
1-102435 Apr 1989 JP
1-179411 Jul 1989 JP
HEI 2-391 Jan 1990 JP
02051220 Feb 1990 JP
3-41783 Feb 1991 JP
03-188619 Aug 1991 JP
5-48072 Feb 1993 JP
5-086477 Apr 1993 JP
05150143 Jun 1993 JP
5-152529 Jun 1993 JP
5-291299 Nov 1993 JP
06-069490 Mar 1994 JP
6-232126 Aug 1994 JP
6-291299 Oct 1994 JP
6-334168 Dec 1994 JP
0812494 Jan 1996 JP
9-67193 Mar 1997 JP
9-82913 Mar 1997 JP
10-256154 Sep 1998 JP
10-303396 Nov 1998 JP
10-321943 Dec 1998 JP
11135614 May 1999 JP
11-238683 Aug 1999 JP
11-260835 Sep 1999 JP
11340542 Dec 1999 JP
2000-068466 Mar 2000 JP
2 000 1645 Jun 2000 JP
2000-351692 Dec 2000 JP
2002-9366 Jan 2002 JP
WO 9210875 Jun 1992 WO
WO 9307647 Apr 1993 WO
WO 9403908 Feb 1994 WO
WO 9745827 Dec 1997 WO
WO 9805807 Jan 1998 WO
WO 9820606 May 1998 WO
WO 9914797 Mar 1999 WO
WO 9914804 Mar 1999 WO
WO 9919546 Apr 1999 WO
WO 9963580 Dec 1999 WO
WO 0006812 Feb 2000 WO
WO 0016378 Mar 2000 WO
WO 0033363 Jun 2000 WO
WO 0048239 Aug 2000 WO
WO 0104943 Jan 2001 WO
WO 0116395 Mar 2001 WO
WO 0133585 May 2001 WO
WO 0137330 May 2001 WO
WO 0159814 Aug 2001 WO
WO 0159820 Aug 2001 WO
WO 0159821 Aug 2001 WO
WO 02 01648 Jan 2002 WO
WO 0203113 Jan 2002 WO
WO 0203467 Jan 2002 WO
WO 0203480 Jan 2002 WO
WO 0209160 Jan 2002 WO
WO 0233385 Apr 2002 WO
WO 0247127 Jun 2002 WO
WO 0250879 Jun 2002 WO
Non-Patent Literature Citations (150)
Entry
Nakagawara et al., Effects of Buffer Layers in Epitaxial Growth of SrTiO3 Thin Film on Si(100), J. Appl. Phys., 78(12), Dec. 15, 1995, pp. 7226-7230.
Suzuki et al., “A Proposal of Epitaxial Oxide Thin Film Structures For Future Oxide Electronics,” Materials Science and Engineering B41, (1996), pp. 166-173.
W. F. Egelhoff et al., “Optimizing GMR Spin Valves: The Outlook for Improved Properties”, 1998 Int'l Non Volatile Memory Technology Conference, pp. 34-37.
Wang et al., “Processing and Performance of Piezoelectric Films”, Univ. Of MD, Wilcoxon Research Col, and Motorola Labs, May 11, 2000.
M. Rotter et al., “Nonlinear Acoustoelectric Interactions in GaAs/LiNbO3 Structures”, Applied Physics Letters, vol. 75(7), Aug. 16, 1999, pp. 965-967.
K. Sreenivas et al., “Surface Acoustic Wave Propagation on Lead Zirconate Titanate Thin Films,” Appl. Phys. Lett. 52(9), Feb. 29, 1998, pp. 709-711.
M. Rotter et al., “Single Chip Fused Hybrids for Acousto-Electric and Acousto-Optic Applications,” 1997 Applied Physics Letters, vol. 70(16), Apr. 21, 1997, pp. 2097-2099.
A. Mansingh et al., “Surface Acoustic Wave Propagation in PZT/YBCO/SrTiO3 and PbTiO3/YBCO/SrTiO3 Epitaxial Heterostructures,” Ferroelectric, vol. 224, pp. 275-282, 1999.
S. Mathews et al., “Ferroelectric Field Effect Transistor based on Epitaxial Perovskite Heterostructures”, Science, vol. 276, Apr. 11, 1997, pp. 238-240.
R. Houdre et al., “Properties of GaAs on Si Grown by Molecular Beam Epitaxy,” Solid State and Materials Sciences, vol. 16, Issue 2, 1990, pp. 91-114.
S. F. Fang et al., “Gallium Arsenide and Other Compound Semiconductors on Silicon,” J. Appl Phys., 68(7), Oct. 1, 1990, pp. R31-R58.
Carlin et al., Impact of GaAs Buffer Thickness on Electronic Quality of GaAs Grown on Graded Ge/GeSi/Si Substrates, Appl. Phys. Letter, vol. 76, No. 14, Apr. 2000, pp. 1884-1886.
Ringel et al., “Epitaxial Integration of III-V materials and Devices with Si Using Graded GeSi Buffers,” 27th International Symposium on Compound Semiconductors, Oct. 2000.
Zogg et al., “Progress in Compound-Semiconductor-on-Silicon-Heteroepitaxy with Fluroide Buffer Layers,” J. Electrochem Soc., vol. 136, No. 3, Mar. 1998, pp. 775-779.
Xiong et al., “Oxide Defined GaAs Vertical-Cavity Surface-Emitting Lasers on Substrates,” IEEE Photonics Technology Letters, vol. 12, No. 2, Feb. 2000, pp. 110-112.
Clem et al., “Investigation of PZT//LSCO//Pt//Aerogel Thin Film Composites for Uncooled Pyroelectric IR Detectors,” Mat. Res. Soc. Symp. Proc., vol. 541, pp. 661-666, 1999.
Gunapala et al., “Bound-To-Quasi-Bound Qauntum-Well Infrared Photodetectors,” NASA Tech Brief, vol. 22, No. 9, Sep. 1998.
Abhay M. Joshi et al., “Monolithic InGaAs-on-silicon Wave Infrared Detector Arrays,” Intn. Society for Optical Engineering, vol. 2999, pp. 211-224.
Bruley et al., “Nanostructure and Chemistry of a (100)MgO/(100) GaAs Interface,” Appl. Phys Lett, 65(5), Aug. 1994, pp. 564-566.
Fork et al., “Epitaxial MgO On Si(001) for Y-Ba-Cu-O Thin Film Growth by Pulsed Laser Deposition,” Appl. Phys Lett., 58(20), May 20, 1991, pp. 2294-2296.
Himpsel et al., “Dialectrics on Semiconductors,” Materials Science and Engineering, B1(1998), pp. 9-13.
Li et al., “Epitaxial La 0.67Sr0.33 Mno3 Magnetic Tunnel Junctions,” J. Appl. Phys. 81(8), Apr. 15, 1997, pp. 5509-5511.
O'Donnell et al., “Clossal Magnetoresistance Magnetic Tunnel Junctions Grown by Molecular-Beam Epitaxy,” Appl. Physics Letters, vol. 76, No. 14, Apr. 3, 2000, pp. 1914-1916.
Mikami et al., “Formation of Si Epi/MgO-Al2O3Eip./SiO3/Si and Its Epitaxial Film Quality,” Fundamental Research Laboratories and Microelectronics Laboratories, pp. 31-34, 1983.
T. Asano et al., “An Epitaxial Si/Insulator/Si Structure Prepared by Vacuum Deposition of CaF2 and Silicon,” Thin Solid Films, vol. 93 (1982), pp. 143-150.
T. Chikyow et al., “Reaction and Regrowth Control of CeO2 on Si(111) Surface for the Silicon-On-Insulator Structure,” Appl. Phys. Lett., vol. 65, No. 8, Aug. 22, 1994, pp. 1030-1032.
J.F. Kang, et al., “Epitaxial Growth of CeO2(100) Films on Si(100) Substrates by Dual Ion Beams Reactive Sputtering,” Solid State Communications, vol. 108, No. 4, pp. 225-227, 1998.
R.A. Morgan et al., “Vertical-Cavity Surface-Emitting Lasers Come of Age,” SPIE, vol. 2683, pp. 18-29.
“Technical Analysis of Qualcomm QCP-800 Portable Cellular Phone (Transmitter Circuitry),” Talus Corporation, Qualcomm QCP-800 Technical Analysis Report, Dec. 10, 1996, pp. 5-8.
Jo-Ey Wong, et al.; “An Electrostatically-Actuated Mems Switch for Power Applications”; IEEE, 2000, pp. 633-638.
T. Mizuno, et al.; “Electron and Hole Mobility Enhancement in Strained-Si MOSFET's on SiGe-on-Insulator Substrates Fabricated by SIMOX Technology”; IEEE Electron Device Letters, vol. 21. No. 5, May 2000; pp. 230-232.
F.M. Buffer, et al.; “Strain-dependence of electron transport in bulk Si and deep-submicron MOSFET's” Computatural Electronics, 2000, Book of Abstracts, IWCE Glasgow 2000, 7th Int'l Workshop on, 2000; pp. 64-65.
S.S. Lu, et al.; “Piezoelectric field effect transistor (PEFET) using In0.2Ga0.8As/Al0.35Ga0.65As/In0.2Ga0.8As/GaAs Strained layer structure on (111)B GaAs substrate”; Electronics Letters, 12th Ma 1994, vol. 30, No. 10; pp. 823-825.
Kihong Kim, et al. “On-Chip Wireless Interconnection with Integrated Antennas”; 2000 IEEE; pp. 20.2.1-20.3.4.
C. Passiopoulos, et al.; “V-Band Single Chip, Direct Carrier BPSK Modulation Transmitter with Integrated Patch Antenna”; 1998 IEEE MTT-S Digest; pp. 305-308.
Mau-Chung Frank Chang, et al.; “RF/Wireless Interconnect for Inter- and Intra-Chip Communications”; Proceedings of the IEEE, vol. 89, No. 4, Apr. 2001; pp. 456-466.
The Electronics Industry Report; Prismark; 2001; pp. 111-120.
J.K. Abrokwah, et al.; “A Manufacturable Complementary GaAs Process”; GaAs IC Symposium, IEEE, 1993, pp. 127-130.
H. Nagata, “A Preliminary Consideration of the Growth Behaviour of CeO2, SrTiO3 and SrVO3 Films on Si Substrate,” Thin Solid Films, 224, 1993, pp. 1-3.
Nagata et al., “Heteroepitaxial Growth of CeO2(001) Films on Si(001) Substrates by Pulsed Laser Deposition in Ultrahigh Vacuum,” Jpn. Journ. Appl. Phys., vol. 30, No. 6B, Jun. 1001, pp. L1136-L1138.
Kado et al., “Heteroepitaxial Growth of SrO Films on Si Substrates,” J. Appl. Phys., 61(6), Mar. 15, 1987, pp. 2398-2400.
H. Ishiwara et al., “Epitaxial Growth of Perovskite Type Oxide Films on Substrates”; Materials Research Symposium Proceedings, vol. 220, pp. 595-600, Apr. 29, May 3, 1991.
J.K. Abrakwah, et al.; “A Manufacturable High-Speed Low-Power Complementary GaAs Process”; Extended Abstracts of the 1994 International Conference on Solid State Devices and Materials, Yokohama, 1994, pp. 592-594.
C.J. Palmstrom et al.; “Stable and Epitaxial Contacts to III-V Compound Semiconductors”; Contacts to Semiconductors Fundamentals and Technology; Noyles Publications, 1993; pp. 67-150.
Jayshri Sabarinathat, et al.; “Submicron three-dimensional infrared GaAs/AlxOy-based photonic crystal using single-step epitaxial growth”; Applied Physics Letters, vol. 78, No. 20, May 14, 2001; pp. 3024-3026.
Philip Ball; “The Next Generation of Optical Fibers”; Technology Review, May 2001; pp. 55-61.
John D. Joannopoulos, et al.; “Molding the Flow of Light”; Photonic Crystals; Princeton University Press, 1995.
Thomas F. Krauss, et al.; “Photonic crystals in the optical regime—past, present and future”; Progress in Quantum Electronics 23 (1999) 51-96.
G. H. Jin, et al.; “PLZT Film Waveguide Mach-Zehnder Electrooptic Modulator”; Journal of Lightwave Technology, vol. 18, No. 6, Jun. 2000; pp. 807-812.
D.E. Aspnes, et al.; “Steps on (001) silicon surfaces”; J. Vac. Sci. Technol. B, vol. 5, No. 4, Jul./Aug. 1987; pp. 939-944.
D.M. Newns, et al.; “Mott transition field effect transistor”; Applied Physics Letters, vol. 73, No. 6, 10 Aug. 1998; pp. 780-782.
Lucent Technologies, Inc. “Arrayed Waveguide Grating Multiplexer/Demultiplexer”; Jan. 2000; 4 pages.
Hisashi Schichijo, et al.; “Co-Integration of GaAs MESFET and Si CMOS Circuits”; IEEE Electron Device Letters, vol. 9, No. 9, Sep. 1988; pp. 444-446.
H. Shichijo, et al.; “GaAs MESFET and Si CMOS Cointegration and Circuit Techniques”; 1988 IEEE: GaAs IC Symposium 239-242.
H. Shichijo, et al.; “Monolithic Process for Co-Integration of GaAs and Silicon Circuits”; 1988 IEEE; pp. 778-781.
Z.H. Zhu, et al. “Growth of InGaAs multi-quantum wells at 1.3 m wavelength on GaAs compliant substrates”; Applied Physics Letters, vol. 72, No. 20, May 18, 1998; pp. 2598-2600.
Kurt Eisenbeiser, et al.; “Metamorphic InAIA/InGaAs Enhancement Mode HEMT's on GaAs Substrates”; IEEE Electron Device Letters, vol. 20, No. 10, Oct. 1999; pp. 507-509.
Tomonori Nagashima, et al.; “Three-Terminal Tandem Solar Cells With a Back-Contact Type Bottom Cell” Higashifuji Technical Center, Toyota Motor Corporation; 4 pages.
James Schellenberg, et al.; “Low-Loss, Planar Monolithic Baluns for K/Ka-Band Applications”; 1999 IEEE MTT-S Digest; pp. 1733-1736.
Arnold Leitner et al; “Pulsed Laser Deposition of Superconducting Strontium Titanate Thin-Films”; Session K11-Thin Films and Borocarbides; Mixed Session, Wednesday Afternoon; Mar. 19, 1997; Room 1202 B, Conv. Center (Abstract).
R.D. Vispute; “High quality optoelectronic grade epitaxial AIN films on -Al203, Si and 6H-SIC by pulsed laser deposition”; Thin Solid Films 299 (1997), pp. 94-103.
T. Warren Weeks, et al.; “GaN thin films deposited via organometallic vapor phase epitaxy on (6H)-SiC(0001) using high-temperature monocrystalline AIN buffer layers” 320 Applied Physics Letters, vol. 67, No. 3, Jul. 17, 1995, pp. 1401-403.
Z. Yu, et al.; “Epitaxial oxide thin films on SI(001)*”; J. Vac. Sci. Technol. B. vol. 18, No. 4, Jul./Aug. 2000; pp. 2139-2145.
Gentex Corporate Website; Photoelectric Smoke Detectors—How They Work; 2001.
Jeffrey B. Casady, et al.; “A Hybrid 6H-SiC Temperature Sensor Operational from 25 C to 500 C”; IEEE Transactions on Components, Packaging, and Manufacturing Technology—Part A, vol. 19, No. 3, Sep. 1996; pp. 416-422.
Ronald W. Waynant, et al.; “Optoelectronic Integrated Circuits”; Electro-Optics Handbook, McGraw-Hill, Inc., 1994; Chapter Twenty Seven.
Antonio Mecozzi, et al.; “The Roles of Semiconductor Optical Amplifiers in Optical Networks”; Optics & Photonics News; Mar. 2001; pp. 37-42.
D.A. Francis, et al.; “A single-chip linear optical amplifier”; OFC, 2001; Mar. 17-22, 2001.
G. Vogg et al.; “Epitaxial alloy films of zintl-phase Ca9Si1-xGex)2”; Journal of Crystal Growth 223 (2001); pp. 573-576.
Peter S. Guilfoyle, et al.; “Optoelectronic Architecture for High-Speed Switching and Processing Applications”; 1998 The Photonics Design and Applications Handbook; pp. H-399-H-406.
Gerald B. Stringfellow; “Organometallic Vapor-Phase Epitaxy: Theory and Practice”; Departments of Materials Science and Engineering and Electrical Engineering, University of Utah; Academic Press, 1989.
M.A. Herman, et al.; “Molecular Beam Epitaxy Fundamentals and Current Status”; Springer-Verlag Berlin Heidelberg, 1989, 1996.
“Integration of GaAs on Si Using a Spinel Buffer Layer”, IBM Technical Bulletin, vol. 30, No. 6, Nov. 1987, p. 365.
“GaInAs Superconducting FET,” IBM Technical Bulletin, vol. 36, No. 8, Aug. 1993, pp. 655-656.
“Epitaxial 3d Structure Using Mixed Spinels,” IBM Technical Bulletin, vol. 30, No. 3, Aug. 1987, p. 1271.
Moon et al., “Roles of Buffer Layers in Epitaxial Growth of SrTiO3 Films on Silicon Substrates,” Japan J of Appl. Phys., vol. 33, Mar. 1994, pp. 1472-1477.
Yodo et al., GaAs Heteroepitaxial Growth on Si Substrates with Thin Si Interlayers in situ Annealed at High Temperatures, 8257b Journal of Vacuum Science & Technology, 1995 May/Jun., vol. 13, No. 3, pp. 1000-1005.
Cuomo et al., “Substrate Effect on the Superconductivity of YBa2Cu3O7 Thin Films,” AIP Conference 1988, pp. 141-148.
McKee et al., “Crystalline Oxides on Silicon: The First Five Monolayers,” Physical Review Letters, vol. 81, No. 14, Oct. 1998, pp. 3014-3017.
McKee et al., “Molecular Beam Epitaxy Growth of Epitaxial Barium Silicide, Barium Oxide, and Barium Titanate on Silicon,” 1991 American Institute of Physics, pp. 782-784, Aug. 13, 1991.
Tambo et al., Molecular Beam Epitaxy Growth of SrTiO3 Films on Si(100)-2x1 with SrO Buffer Layer, Jpn. J. Appl. Phys., vol. 37, 1998, pp. 4454-4459.
McKee et al., “The MBE Growth and Optical Quality of BaTiO3 and SrTiO3 Thin Films on MgO,” Mat. Res. Soc. Symp. Proc., vol. 341, Apr. 1994, pp. 309-314.
McKee et al., “BaSi2 and Thin Film Alkaline Earth Silicides on Silicon,” Appl Phys. Lett., 63(20), Nov. 1993, pp. 2818-2820.
McKee et al., “Surface Structures and the Orthorhombic Transformation of Thin Film BaSi2 on Silicon,” Mat. Res. Soc. Symp. Proc., vol. 221, pp. 131-136.
Brian A. Floyd, et al.; “The projected Power Consumption of a Wireless Clock Distribution System and Comparison to Conventional Distribution Systems”; IEEE, 1999; pp. IITC99-249-IITC99-250.
Mori et al., “Epitaxial Growth of SrTiO3 Films on Si(100) Substrates Using a Focused Electron Beam Evaporation Method,” Jpn. J. of Apl. Phys., vol. 30, No. 8A, Aug. 1991, pp. L1415-L1417.
Moon et al., “Growth of Crystalline SrTiO3 Films on Si Substrates Using Thin Fluoride Buffer Layers and Their Electrical Properties,” Jpn. J. of Appl. Phys., vol. 33, (1994), pp. 5911-5916.
Farrow et al., “Heteroepitaxy of Dissimilar Materials,” Mat. Res. Soc. Symposium Proceedings, vol. 221, pp. 29-34, Apr. 29-May 2, 1991.
Ishiwara et al., “Heteroepitaxy on Silicon: Fundamentals, Structure, and Devices,” Mat. Res. Soc., Symposium Proceedings, vol. 116, pp. 369-374, Apr. 5-8, 1988.
Douglas B. Chrisey, et al; Pulsed Laser Deposition of Thin Films; pp. 273-285.
B.A. Block, et al; “Photoluminescence properties of Er3-doped BaTiO3 thin films”; Appl. Phys. Lett. 65 (1), Jul. 4, 1994, pp. 25-27.
Kevin J. Chen et al; “A Novel Ultrafast Functional Device: Resonant Tunneling High Electron Mobility Transistor”; Electron Devices Meetingk 1996; IEEE Hong Kong; Jun. 29, 1996; pp. 60-63, XP010210167.
Wenhua Zhu et al.; “Molecular Beam Epitaxy of GaAs on Si-on-Insulator”; 320 Applied Physics Letters 59(1991) Jul. 8, No. 2; pp. 210-212.
Umesh K. Mishra et al; “Oxide Based Compound Semiconductor Electronics”; Electron Devices Meeting; 1997; Technical Digest, International; Washington, D.C.; Dec. 7-10, 1997; pp. 545-548.
J.M. Daughton et al.; “Applications of Spin Dependent Transport Materials”; J. Phys. D. Appl Phys. 32(1999) R169-R177.
Wei Zhang et al.; “Stress Effect and Enhanced Magnetoresistance in La0.67Ca0.33MnO3-δ Films”; Physical Review, B. Condensed Matter; American Institute of Physics; vol. 58, No. 21, Part 1; Dec. 1, 1998; pp. 14143-14146.
Q.-Y. Tong et al.; “IOS-a new type of materials combination for system-on-a chip preparation”; 1999 IEEE International SOI Conference, Oct. 1999; pp. 104-105.
T. Kanniainen et al.; “Growth of Dielectric 1hfo2/Ta205 Thin Film Nanolaminate Capacitors By Atomic Layer Epitaxy”; Electrochemical Society Proceedings, U.S. Electrochemical Society; Pennington, N.J.; Aug. 31, 1997; pp. 36-46.
Myung Bok Lee; “Heteroepitaxial Growth of BaTiO3 Films on Si by Pulsed Laser Deposition”; Applied Physics Letters; Mar. 13, 1995; pp. 1331-1333.
Myung Bok Lee; “Formation and Characterization of Eptiaxial TiO2 and BaTiO3/TiO2 Films on Si Substrate”; Japan Journal Applied Physics Letters; vol. 34; 1995; pp. 808-811.
Gilbert Lecarpentier et al.; “High Accuracy Machine Automated Assembly for Opto Electronics”; 2000 Electronic Components and Technology Conference; pp. 1-4.
R. Ramesh; “Ferroelectric La-Sr-Co-O/Pb-Zr-Ti-O/La-Sr-Co-O Heterostructures on Silicon via Template Growth”; 320 Applied Physics Letters; 63(1993); Dec. 27,; No. 26; pp. 3592-3594.
K. Eisengbeiser; “Field Effect Transistors with SrTiO3 Gate Dielectric on Si”; Applied Physics Letters; vol. 76, vol. 76, No. 10; Mar. 6, 2000; pp. 1324-1326.
Stephen A. Mass; “Microwave Mixers”; Second Edition; 2pp.
Douglas J. Hamilton et al.; “Basic Integrated Circuit Engineering”; pp. 2; 1975.
Takeshi Obata; “Tunneling Magnetoresistance at Up to 270 K in La0.8Sr0.2MnO3/SrTiO3/La0.8Sr0.2MnO3 Junctions with 1.6-nm-Thick Barriers”; Applied Physics Letters; vol. 74, No. 2; Jan. 11, 1999; pp. 290-292.
Wei Zhang et al.; “Enhanced Magnetoresistance in La-Ca-Mn-O Films on Si Substrates Using YbaCuO/CeO2 Heterostructures”; Physica C; vol. 282-287, No. 2003; Aug. 1, 1997; pp. 1231-1232.
Shogo Imada et al; “Epitaxial Growth of Ferroelectric YmnO3 Thin Films on Si (111) Substrates by Molecular Beam Epitaxy”; Jpn. J. Appl. Phys. vol. 37 (1998); pp. 6497-6501; Part 1, No. 12A, Dec. 1998.
Ladislav Pust et al; “Temperature Dependence of the Magnetization Reversal in Co(fcc)-BN-Co(poly hcp) Structures”Journal of Applied Physics; vol. 85, No. 8; Apr. 15, 1999; pp. 5765-5767.
C. Martinez; “Epitaxial Metallic Nanostructures on GaAs”; Surface Science; vol. 482-485; pp. 910-915; 2001.
Wen-Ching Shih et al; “Theoretical Investigation of the SAW Properties of Ferroelectric Film Composite Structures”; IEEE Transactions of Ultrasonics, Ferroelectrics, and Frequency Control; vol. 45, No. 2; Mar. 1998; pp. 305-316.
Zhu Dazhong et al.; “Design of ZnO/SiO2/Si Monolithic Integrated Progrmmable SAW Filter”; Proceedings of Fifth International Conference on Solid-State and Integrated Circuit Technology; 21-23; Oct. 1998; pp. 826-829.
Kirk-Othmer Encyclopedia of Chemical Technology; Fourth Edition, vol. 12; Fuel Resources to Heat Stabilizers; A Wiley-Interscience Publication: John Wiley & Sons.
Joseph W. Goodman et al; “Optical Interconnectiosn For VLSI Systems”; Proceedings of the IEEE, vol. 72, No. 7 Jul. 1984.
Fathimulla et al.; “Monolithic Integration of InGaAs/InAIAs MODFETs and RTDs on InP-bonded-to-Si Substrate”, Fourth International Conference on Indium Phosphide and Related Materials, Newport, RI, USA; Apr. 21-24, 1992; pp. 167-170; XP000341253; IEEE, New York, NY, USA; ISBN:0-7803-0522-1.
H. Takahashi et al.; “Arraryed-Waveguide Grating For Wavelength Division Multi/Demultiplexer With Nanometre Resolution”; Electronics Letters; vol. 26, No. 2, 18th Jan. 1990.
Pierret R.F.; “1/J-FET and MESFET”; Field Effect Devices; MA, Addison-Wesley; 1990; pp. 9-22.
M. Schreiter, et al.; “Sputtering of Self-Polarized PXT Films for IR-Detector Arrays”; 1998 IEEE; pp. 181-185.
Hideaki Adachi et al.; “Sputtering Preparation of Ferroelectric PLZT Thin Films and Their Optical Applications”; IEEE Transactions of Ultrasonics, Ferroelectrics and Frequencey Control, vol. 38, No. 6, Nov. 1991.
A.J. Moulson et al.; “Electroceramics Materials Properties Applications”; Chapman & Hall; pp. 366-369.
P.A. Langjahr et al; “Epitaxial Growth and Structure of Cubic and Pseudocubic Perovskite Films on Perovskite Substrates”; Mat. Res. Soc. Symp. Proc., vol. 401; 1995 Materials Research Society; pp. 109-114.
Wang et al.; “Depletion-Mode GaAs MOSFETs with Negligible Drain Current Drift and Hysteresis”; Electron Devices Meeting, 1998, IEDM ′98 Technical Digest; pp. 67-70.
Ben G. Streetman; “Solid State Electronic Devices”; 1990, Prentice Hall; Third Edition; pp. 320-322.
A.Y Wu et al.; “Highly Oriented (Pb,La)(Zr,Ti)O3 Thin Films on Amorphous Substrates”; IEEE, 1992; pp. 301-304.
Timothy E. Glassman et al.; “Evidence for Cooperative Oxidation of MoCVD Precursors Used in BaxSr1-xTiO3 Film Growth”; Mat. Res. Soc. Symp. Proc. vol. 446, 1997 Materials Research Society; pp. 321-326.
S.N. Subbarao et al.; “Monolithic PIN Photodetector and FET Amplifier on GaAs-os-Si”; IEEE, GaAs IC Symposium-163-166; 1989.
T.A. Langdo et al.; “High Quality Ge on Si by Epitaxial Necking”; Applied Physics Letters; vol. 76, No. 25: pp. 3700-3702; Jun. 19, 2000.
Chenning Hu et al.; Solar Cells From Basics to Advanced Systems; McGraw-Hill Book Company; 1983.
O.J. Painter et al; “Room Temperature Photonic Crystal Defect Lasers at Near-Infrared Wavelengths in InGaAsp”; Journal of Lightwave Technology, vol. 17, No. 11; Nov. 1999.
C. Donn et al.; “A 16-Element, K-Band Monolithic Active Receive Phased Array Antenna”; Antennas and Propagation Society International Symposium, 1988; pp. 188-191, vol. 1; Jun. 6-10, 1988.
Don W. Shaw; “Epitaxial GaAs on Si: Progress and Potential Applications”; Mat. Res. Soc. Symp. Proc.; pp. 15-30; 1987.
G.J.M. Dormans, et al.; “PbTiO/3/Thin Films Grown by Organometallic Chemical Vapour Deposition”; Third International Symposium on Integrated Ferroelectrics; Apr. 3-5, 1991 (Abstract).
P.J. Borrelli et al.; “Compositional and Structural Properties of Sputtered PLZT Thin Films”; Ferroelectric Thin Films II Symposium; Dec. 2-4, 1991 (Abstract).
Ranu Nayak et al; “Enhanced acousto-optic diffraction efficiency in a symmetric SrRiO3/BaTiO3/SrTiO3 thin-film heterostructure”; Nov. 1, 2000; vol. 39, No. 31; Applied Optics; pp. 5847-5853.
Ranu Nayak et al; “Studies on acousto-optical interaction in SrTiO3/BaTiO3/SrTiO3 epitaxial thin film heterostructures”; J. Phys. D: Appl. Phys. 32 (1999) 380-387.
S.K. Tweksbury et al.; “Cointegration of Optoelectronics and Submicron CMOS”; Wafer Scale Integration; 1993; Proceedings, Fifth Annual IEEE; Jan. 20, 1993; pp. 358-367.
V. Kaushik et al.; “Device Characteristics of Crystalline Epitaxial Oxides on Silicon”; Device Research Conference, 2000; Conference Digest 58th DRC; pp. 17-20; Jun. 19-21, 2000.
Katherine Derbyshire; “Prospects Bright for Optoelectronics Volume, Cost Drive Manufacturing for Optical Applications”; Semiconductor Magazine; vol. 3, No. 3; Mar. 2002.
Alex Chediak et al; “Integration of GaAs/Si with Buffer Layer and Its Impact on Device Integration”; TICS 4, Prof. Sands. MSE 225, Apr. 12, 2002; pp. 1-5.
S.A. Chambers et al; “Band Discontinuities at Epitaxial SrTiO3/Si(001) Heterojunctions”; Applied Physics Letters; vol. 77, No. 11; Sep. 11, 2000; pp. 1662-1664.
H. Wang et al.; “GaAs/GaAIAs Power HBTs for Mobile Communications”; Microwave Symposium Digest; 1993 IEEE; vol. 2; pp. 549-552.
Y. Ota et al.; “Application of Heterojunction FET to Power Amplifier for Cellular Telephone”; Electronics Letters; 26th May 1994; vol. 30, No. 11; pp. 906-907.
Keiichi Sakuno et al; “A 3.5W HBT MMIC Power Amplifier Module for Mobile Communications”; IEEE 1994; Microwave and Millimeter-Wave Monolithic Circuits Symposium; pp. 63-66.
Mitsubishi Semiconductors Press Release (GaAs FET's) Nov. 8, 1999 pp. 1-2.
R.J. Matyi et al; “Selected Area Heteroepitaxial Growth of GaAs on Silicon for Advanced Device Structures”; 2194 Thin Solid Films; 181 (1989) Dec. 10; No.1; pp. 213-225.
K. Nashimoto et al; “Patterning of Nb, LaOnZr, TiO3 Waveguides for Fabricating Micro-Optics Using Wet Etching and Solid-Phase Epitaxy”; Applied Physics Letters; vol. 75, No. 8; Aug. 23, 1999; pp. 1054-1056.
Bang-Hung Tsao et al; “Sputtered Barium Titanate and Barium Strontium Titanate Films for Capacitor Applications”; Applications of Ferroelectrics, 2000; Proceedings of the 2000 12th International Symposium on vol. 2; pp. 837-840.
Man Fai Ng et al; “Heteroepitaxial growth of lanthanum aluminate films derived from mixed metal nitrates”; Journal of Materials Research; vol. 12, No. 5; pp. 1306.
Yuji Matsumoto et al.; “Room-Temperature Ferromagnetism in Transparent Transition Metal-Doped Titanium Dioxide”; Science; Feb. 2, 2001; vol. 291; pp. 854-856.
S.A. Chambers et al.; “Epitaxial Growth and Properties of Ferromagnetic Co-Doped TiO2 Anatase”; Applied Physics Letters; vol. 79, No. 21; Nov. 19, 2001; pp. 3467-3469.