US 7,227,196 B2Grant
Group II-VI semiconductor devices
Issue Date:2007-06-05
•41 Claims
•17 Drawing Sheets
Abstract
Semiconductor devices containing group II-VI semiconductor materials are disclosed. The devices may include a p-n junction containing a p-type group II-VI semiconductor material and an n-type semiconductor material. The p-type group II-VI semiconductor includes a single crystal group II-VI semiconductor containing atoms of group II elements, atoms of group VI elements, and one or more p-type dopants. The p-type dopant concentration is greater than about 1016 atoms·cm−3, the semiconductor resistivity is less than about 0.5 ohm·cm, and the carrier mobility is greater than about 0.1 cm2/V·s. The semiconductor devices may include light emitting diodes, laser diodes, field effect transistors, and photodetectors.
Metadata
Inventors
- Robert H. Burgener, II
- Roger L. Felix
- Gary M. Renlund
Application Information
Application Number:US 10/849,348
Filing Date:2004-05-19
Priority Date:2003-05-20
Art Unit:2814
Classifications
IPC:
H01L33/00
Patent Drawings (17 sheets)
Description
CROSS-REFERENCE TO RELATED APPLICATIONS
[0001] This application claims the benefit of U.S. Provisional Application No. 60/471,916, filed May 20, 2003, U.S. Provisional Application No. 60/488,677, filed Jul. 18, 2003, and U.S. Provisional Application No. 60/560,779, filed Apr. 8, 2004, which applications are incorporated by reference.
BACKGROUND OF THE INVENTION
[0002] The present invention provides group II-VI semiconductor devices and methods of fabrication.
[0003] As used herein, the group II-VI semiconductor devices include devices fabricated from group II-VI semiconductor compounds which include group II elements selected from zinc, cadmium, the alkaline earth metals such as beryllium, magnesium calcium, strontium, and barium, and mixtures thereof, and group VI elements selected from oxygen, sulfur, selenium, tellurium, and mixtures thereof. The group II-VI semiconductor compounds may be doped with one or more p-type dopant. Such p-type dopants include, but are not limited to, nitrogen, phosphorus, arsenic, antimony, bismuth, copper, chalcogenides of the foregoing, and mixtures thereof. Zinc oxide and zinc sulfide are two presently preferred group II-VI semiconductor compounds.
[0004] Zinc oxide (ZnO) and zinc sulfide are wide band gap semiconductors with potential for use in electrically excited devices such as light emitting devices (LEDs), laser diodes (LDs), field effect transistors (FETs), photodetectors operating in the ultraviolet and at blue wavelengths of the visible spectrum, and other similar devices. Gallium nitride (GaN) is becoming more commonly used as a semiconductor material for the electronic devices mentioned above.
[0005] Zinc oxide has several advantages over GaN. For instance, ZnO has a significantly larger exciton binding energy than GaN, which suggests that ZnO-based lasers should have more efficient optical emission and detection. Zinc oxide drift mobility saturates at higher fields and higher values than GaN, potentially leading to higher frequency device performance. The cost and ease of manufacture of zinc oxide is attractive when compared to other common semiconductor materials. Zinc oxide has superior radiation-resistance (2 MeV at 1.2×1017 electrons/cm2) compared to GaN, which is desirable for radiation hardened electronics. Zinc oxide has high thermal conductivity (0.54 W/cm·K). Zinc oxide has strong two-photon absorption with high damage thresholds, rendering it ideal for optical power limiting devices. Unlike GaN, zinc oxide does not form polytypes or crystal lattice stacking irregularities.
[0006] N-type zinc oxide semiconductor materials are known and relatively easy to prepare, such as ZnO doped with aluminum, gallium, or other known n-type dopants. P-type zinc oxide semiconductor materials are theoretically possible, but have been difficult to prepare. D.C. Look et al., “The Future of ZnO Light Emitters,” Phys. Stat. Sol., 2004, summarize data on p-type ZnO samples reported in the literature. The best reported ZnO samples have resistivity values of 0.5 ohm·cm (N/Ga dopants) and 0.6 ohm·cm (P dopant). Many of the reported p-type zinc oxide samples tend to be light, heat, oxygen, and moisture sensitive. Some convert to n-type material over time. Their stability has been questioned. Some of the more-stable p-type zinc oxide materials reported in the literature are prepared using complex and expensive fabrication processes, such as molecular beam epitaxy. No commercially viable p-type zinc oxide semiconductor materials are currently known. Therefore, it would be an advancement in the art to provide commercially viable p-type zinc oxide semiconductor materials. More particularly, it would be an advancement in the art to provide commercially viable p-type group II-VI semiconductor materials which may be used to prepare group II-VI semiconductor devices.
BRIEF SUMMARY OF THE INVENTION
[0007] The present invention is drawn to semiconductor devices that contain group II-VI semiconductor materials. The devices may include a p-n junction containing a p-type group II-VI semiconductor material and an n-type semiconductor material. The p-type group II-VI semiconductor includes single crystal group II-VI semiconductors containing atoms of group II elements, atoms of group VI elements, and one or more p-type dopants. The p-type dopant concentration is greater than about 1016 atoms·cm−3, the semiconductor resistivity is less than about 0.5 ohm·cm, and the carrier mobility is greater than about 0.1 cm2/V·s. The semiconductor devices may include light emitting diodes, laser diodes, field effect transistors, and photodetectors.
[0008] The group II elements include, but are not limited to, zinc, cadmium, alkaline earth metals, and mixtures thereof. The group VI elements include, but are not limited to, oxygen, sulfur, selenium, tellurium, and mixtures thereof. The p-type dopant includes, but is not limited to, nitrogen, phosphorus, arsenic, antimony, bismuth, copper, and chalcogenides of the foregoing, and mixtures thereof. Zinc oxide and zinc sulfide are two currently preferred group II-VI semiconductor materials.
[0009] The semiconductor device includes group II-VI semiconductor materials deposited as a thin film onto a self supporting surface. The self supporting surface may be crystalline, polycrystalline, or amorphous. The thin film is preferably deposited by a commercially viable chemical deposition process, such as, but not limited to, RF sputtering, CVD (chemical vapor deposition), MOCVD (metal organic chemical vapor deposition), spin coating, electrophoresis, and hydrothermal growth processes.
[0010] A variety of useful semiconductor devices may be prepared within the scope of the present invention, including but not limited to, light emitting diodes, laser diodes, field effect transistors, and photodetectors. For semiconductor devices designed to emit light, the emitted light may have a wavelength in the range from about 207 nm to about 810 nm. Specific light wavelengths, such as 441.6 nm and 325 nm, may be emitted.
[0011] Advantageously, the n-type semiconductor material is an n-type group II-VI semiconductor compatible with the p-type group II-VI semiconductor material. Typical n-type dopants include, but are not limited to, ions of Al, Ga, B, H, Yb and other rare earth elements, Y, Sc, and mixtures thereof.
[0012] Additional dopants, alloys, or semiconductor layers may be used to optimize the performance of the device. For example, the group II-VI semiconductor material may further include magnesium oxide or cadmium oxide to control the band gap. Multiple Quantum Wells may also but used to optimize or control the device performance.
BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS
[0013] A more particular description of the invention briefly described above will be rendered by reference to specific embodiments thereof which are illustrated in the appended drawings. These drawings depict only typical embodiments of the invention and are not therefore to be considered to be limiting of its scope. The invention will be described and explained with additional specificity and detail through the use of the accompanying drawings in which:
[0014] FIG. 1 is a schematic representation of a sputtering system used in the fabrication of certain p-type group II-VI semiconductor materials.
[0015] FIG. 2 is a graph X-ray Photoelectron Spectroscopy (XPS) of arsenic doped p-type zinc oxide.
[0016] FIG. 3 is a graph of photoluminescence spectra comparing undoped, bulk, n-type zinc oxide with phosphorous doped and arsenic doped p-type zinc oxide.
[0017] FIG. 4 is a graph of the Hall measurements showing sheet resistance and carrier mobility vs. temperature for arsenic doped p-type zinc oxide.
[0018] FIG. 5 is a Secondary Ion Mass Spectroscopy (SIMS) graph of an arsenic doped ZnO film measured against a calibrated standard.
[0019] FIG. 6 is graph of the X-ray diffraction pattern generated by sputtered arsenic doped polycrystalline zinc oxide.
[0020] FIG. 7 is a graph of the X-ray diffraction pattern generated by a zinc oxide thin film within the scope of the present invention showing single crystal (002) plane.
[0021] FIG. 8 is a Secondary Ion Mass Spectroscopy (SIMS) graph of an antimony doped ZnO film.
[0022] FIG. 9 is a schematic diagram of a zinc oxide p-n junction within the scope of the present invention.
[0023] FIG. 10 shows a spectrum of light emitted from a zinc oxide p-n junction within the scope of the present invention.
[0024] FIG. 11 shows a graph of current vs. voltage for a zinc oxide p-n junction within the scope of the present invention showing rectification of the p-n junction.
[0025] FIG. 12 is a schematic diagram of a group II-VI semiconductor heterostructure device containing an active region.
[0026] FIG. 13 is a schematic diagram of a group II-VI semiconductor device of FIG. 10 without an active region.
[0027] FIG. 14A is a schematic diagram of a conventional GaN solid state device fabricated on a sapphire or SiC substrate.
[0028] FIG. 14B is a schematic diagram of a ZnO solid state device fabricated on an alternative self-supporting substrate within the scope of the present invention.
[0029] FIGS. 15A-15B are schematic representations of group II-VI semiconductor devices fabricated with multiple quantum wells.
[0030] FIGS. 16A-16B are schematic representations of group II-VI semiconductor devices fabricated with a single quantum well.
[0031] FIG. 17 is a zinc-oxygen-arsenic ternary diagram.
DETAILED DESCRIPTION OF THE INVENTION
[0032] The present invention is drawn to methods for group II-VI semiconductor devices. These devices are preferably fabricated using group II-VI semiconductor materials. In particular, the present invention is drawn to methods that are commercially viable such that the semiconductor materials can be fabricated economically and efficiently. Some chemical fabrication processes, such as molecular beam epitaxy and laser ablation epitaxy, require complicated and expensive equipment to produce small compound samples. Such processes, while useful for research purposes, are not commercially viable.
[0033] In accordance with one aspect within the scope of the present invention, p-type group II-VI semiconductor devices may be fabricated using commercially viable processes in which the partial pressures of the semiconductor constituents are controlled.
[0034] In one method within the scope of the present invention, a p-type group II-VI semiconductor material is fabricated by obtaining a self supporting substrate surface and depositing a thin film of group II-VI semiconductor doped with one or more p-type dopants on the substrate surface. The deposition conditions are controlled such that the group II, group VI, and p-type dopant atoms are in a gaseous phase prior to combining as the thin film of group II-VI semiconductor.
[0035] The resulting thin film of group II-VI semiconductor is a persistent p-type semiconductor. As used herein a persistent p-type semiconductor is not substantially degraded by UV or visible light exposure, exists at substantially room temperature and pressure, and retains its p-type semiconductor characteristic for an extended period of time, greater than one year. Depending upon the choice of group II-VI elements, the semiconductor material may also exhibit high temperature stability and radiation resistance. This is particularly relevant to zinc oxide semiconductors.
[0036] The p-type dopant may be selected from known p-type dopant materials. Typical p-type dopants include, but are not limited to, nitrogen, phosphorus, arsenic, antimony, bismuth, copper, chalcogenides of the foregoing, and mixtures thereof.
[0037] The band gap of the group II-VI semiconductor may be controlled by including additional dopant or alloy compounds including, but not limited to, cadmium oxide and magnesium oxide, which are themselves group II-VI compounds. As an example, zinc oxide host has a band gap of about 3.2 eV. The zinc oxide band gap may be modified using known band gap engineering techniques. By varying the host material, the light emission wavelength may be adjusted. Zinc oxide alloyed with magnesium oxide may increase the band gap to about 4.0 eV which will result in a light emission of about 310 nm. Similarly, cadmium oxide alloyed with zinc oxide, alone or in combination with other cadmium chalcogenides, may decrease the band gap which will result in a light emission in the visible region up to about 660 nm. The amount of magnesium oxide or cadmium oxide will typically range up to about 20 mole % to achieve a desired band gap or other electronic properties.
[0038] The p-type dopant concentration in the group II-VI semiconductor is preferably greater than about 1016 atoms·cm−3, and typically in the range from about 1016 to about 1022 atoms·cm−3. More preferably, the p-type dopant concentration is in the range from about 1017 to 1019 atoms·cm−3. The dopant content in the resulting group II-VI material may be varied and controlled. High dopant content is possible using techniques within the scope of the present invention.
[0039] The semiconductor resistivity is preferably less than about 0.5 ohm·cm. More preferably the resistivity is less than about 0.1 ohm·cm, more preferably the resistivity is less than about 0.01 ohm·cm, and more preferably the resistivity is less than about 0.001 ohm·cm.
[0040] The carrier mobility is preferably greater than about 0.1 cm2/V·s. More preferably, the carrier mobility is greater than 0.5 cm2/V·s, and more preferably the carrier mobility is greater than 4 cm2/V·s. Carrier mobilities greater than 100 cm2/V·s have been observed.
[0041] The group II-VI semiconductor may be deposited as a thin film on self supporting substrates known in the art such as sapphire and silicon carbide. However, the semiconductor materials need not be deposited on expensive crystal growth substrates. Instead, they may advantageously be deposited on lower cost crystalline, polycrystalline, and amorphous substrates. Such substrates may include, but are not limited to, silicon wafers, amorphous self supporting substrate surfaces like fused silica and glasses such as borosilicate glass and soda lime glass, and polycrystalline substrate surfaces such as alumina. The group II-VI semiconductor materials may be deposited on many other substrates. The choice of substrate may be affected by the desired application of the semiconductor, including transparency, electronic properties, and cost.
[0042] The group II-VI semiconductor material is preferably deposited as a single crystal. As used herein, a single crystal group II-VI semiconductor material possesses a single predominant reflection on an X-ray diffraction pattern. Polycrystalline materials will possess multiple reflection peaks on an X-ray diffraction pattern. Persons skilled in the art will appreciate that a perfect single crystal, defect free, does not exist. There will always be some minor crystal defects present. As used herein, a single predominant reflection peak will possess at least 95% of the integrated area of the X-ray diffraction pattern, and more preferably greater than 99%.
[0043] Zinc oxide doped with arsenic is one presently preferred group II-VI semiconductor. Several possible fabrication methods may be used to prepare p-type zinc oxide doped with arsenic. For example, in one fabrication method within the scope of the present invention, a thin film of zinc arsenide (Zn3As2, ZnAs2, or a mixture thereof) is deposited onto a self supporting substrate, such as fused silica or silicon wafer. The zinc arsenide may be deposited by thermal evaporation, sputtering, a combination of thermal evaporation and sputtering, or other known deposition techniques such as MOCVD, CVD, spin coating, etc.
[0044] Zinc oxide doped with arsenic may be sputtered onto the substrate at a temperature at which a portion of the arsenic is in the gas phase. Without being bound by theory, it is presently believed that a portion of the arsenic from the zinc arsenide layer evaporates by heating the substrate during the sputtering process such that the sputtering atmosphere contains identifiable partial pressures of arsenic, zinc, and oxygen. The partial pressures may be determined by a mass spectrometer. These gaseous species are present at appropriate ratios such that when they are forced onto the substrate by action of the magnetic field, they form the desired arsenic doped zinc oxide. The partial pressures of the group II-VI semiconductor compounds is preferably controlled during the fabrication process.
[0045] Some useful results have been obtained when the thin film of zinc oxide was sputtered in a sputtering atmosphere comprising hydrogen gas. Without being bound by theory, it is possible the hydrogen in the sputtering atmosphere helps limit the oxygen available to oxidize the zinc and arsenic and form undesired oxides. From a review of the Zn—O—As ternary diagram shown in FIG. 17 , too much oxygen present may encourage the formation of undesirable ternary compounds, such as Zn4O9As2, Zn3O8As2, Zn3O6As2, and ZnO4As2. Hence, it is desirable to limit the oxygen partial pressure during the deposition process. Because hydrogen is known to act as an n-type dopant, it is possible that some hydrogen is incorporated into the semiconductor material and may counteract the activity of the p-type dopant. Therefore, other means for controlling the oxygen content in the sputtering atmosphere may be used.
[0046] Effective p-type zinc oxide may be prepared in a manner similar to the method described above, except that it is not necessary to first deposit a zinc arsenide layer onto the substrate. The zinc oxide may be directly sputtered onto the substrate under conditions in which gaseous arsenic is available. This may be accomplished through the use of a heated basket containing arsenic, zinc arsenide, or an arsenic compound. It may also be accomplished through the use of gaseous arsenic compounds, such as arsenic ethoxide (As(OC2H5)3).
[0047] In the RF magnetron sputtering process, a substrate is placed in a low-pressure chamber. The magnetron sputtering head is driven by an RF power source which generates a plasma and ionization of the gas or gases (e.g., argon and selected dopants). For RF sputtering, a high-frequency generator is used generating electromagnetic power in the MHz-Region (typically about 13.56 MHz). Argon ions bombard the target releasing ions from the target which are liberated and accelerated towards the substrate. Additional atoms in the plasma may also be deposited onto the substrate.
[0048] The sputtering process conditions may vary. For example, sputtering system may have a target comprising from about 0.99 to about 0.95 mole % zinc oxide and about 0.01 to about 0.05 mole % arsenic. Alternatively, the sputtering system may have a target comprising from about 0.99 to about 0.95 mole % zinc and about 0.01 to about 0.05 mole % arsenic oxide (As2O3). Similarly, the sputtering system may have a target comprising zinc metal and arsenic metal or a target comprising zinc oxide and arsenic oxide or a target comprising zinc metal or zinc oxide and a source of gaseous arsenic. Other similar variations in the sputtering process conditions are within the level of skill in the art.
[0049] The system may operate at a power in the range from about 20 to about 120 watts. Persons skilled in the art will appreciate that the power may be varied to control deposition time and film thickness, as well as the quality of the resulting film.
[0050] Good results have been obtained when the inert sputtering gas is present in the sputtering atmosphere at a pressure in the range from about 4 to 20 mtorr. The inert sputtering gas is preferably selected from argon, krypton, xenon, neon, and helium. Argon is a presently preferred inert sputtering gas. Small amounts of oxygen may be included in the sputtering gas, usually at a pressure in the range from about 1 to 4 mtorr. In some embodiments, beneficial results have been obtained when the thin film is annealed at a temperature in the range from about 300 to about 450° C. for a time period in the range from about 1 to about 15 minutes.
[0051] It will be appreciated that alternative p-type dopants may be used in the foregoing methods. For example, antimony has been used to prepare p-type zinc oxide by using antimony or antimony oxide (Sb2O3) instead of arsenic or arsenic oxide in several of the foregoing sputtering methods. Similarly, the methods may be adapted for use with other group II elements besides zinc, such as cadmium and alkaline earth metals. Likewise, the methods may be adapted for use with other group VI elements besides oxygen, such as sulfur, selenium, tellurium, and mixtures thereof.
[0052] There are many potential applications and uses of the p-type group II-VI semiconductor materials, and in particular zinc oxide and zinc sulfide semiconductor materials. For example, it may be combined with a suitable n-type semiconductor material to form a p-n junction used in various electrical components. The n-type semiconductor is preferably compatible with the p-type group II-VI semiconductor and preferably contains an n-type dopant selected from known dopant materials. Typical n-type dopants include, but are not limited to, ions of Al, Ga, B, H, Yb and other rare earth elements, Y, Sc, and mixtures thereof. It may be used to prepare light emitting devices that produce light ranging from the ultraviolet to the red region under an electric potential. Band gap engineering principles can be used to control the light emitted. Ultraviolet light can be used to photopump phosphors and produce visible white light. The low activation energy would permit the light emitting devices to operate at low voltage. The p-type group II-VI semiconductor materials may be used to prepare ultraviolet laser diodes. Just as the thin film may be configured to generate light under an electric potential, the devices may be used as a photovoltaic solar cell to generate electricity when exposed to light or a photodetector device.
[0053] The electrical conductivity of the thin films renders them useful in flat-panel display devices. The zinc oxide thin films may be used in electrochromic devices, such as automatically dimming rear-view mirrors for automobiles and electrically controlled “smart” windows. Electric current may be passed through the thin films coated on vehicle windows and freezer display cases to render them frost-free. The thin film conductivity may be exploited to dissipate static electricity from windows on photocopy machines, to form transparent electromagnetic shields, invisible security circuits on windows, and transparent radio antennas built into automobile windows. The high thermal and chemical stability of zinc oxide may render radiation hardened electrical components.
[0054] While some of the discussion herein mentions zinc oxide specifically, it will be appreciated that the processes, compositions, and applications thereof, have broad application to group II-VI semiconductor devices and are not limited solely to zinc oxide based semiconductor devices.
EXAMPLES
[0055] The following examples are given to illustrate various embodiments within the scope of the present invention. These are given by way of example only, and it is to be understood that the following examples are not comprehensive or exhaustive of the many embodiments within the scope of the present invention.
[0056] Many of the following Examples involve sputtering. FIG. 1 illustrates a schematic representation of a sputtering system 10 used in some of the following examples. In RF sputtering, a substrate 12 is placed in a low-pressure chamber 14. The magnetron sputtering head 16 is driven by an RF power source (not shown) which generates a plasma and ionization of the sputtering gas or gases between the electrodes. The sputtering gas typically includes an inert sputtering gas, which may include, but is not limited to, argon, krypton, xenon, neon, and helium. The sputtering gas may optionally include one or more selected dopants. A plurality of gas sources 18, 20, 22, and 24 may provide N2, H2, Ar, O2, or other desired gases. For RF sputtering, a high-frequency generator is used generating electromagnetic power in the MHz-Region. Argon ions bombard the target 26, releasing ions from the target which are accelerated towards the substrate. Additional atoms in the plasma may also be deposited onto the substrate, such as dopant atoms.
[0057] In the sputtering system of FIG. 1 , the substrate 12 is secured in place by a heated substrate fixture 28. The temperature of the heated substrate fixture 28 was measured and reported as the substrate temperature. The sputtering chamber 14 is constantly evacuated with a vacuum pump system 30. The sputtering atmosphere includes an inert sputtering gas mentioned above, and may optionally include other gases which are provided by the respective gas source 18, 20, 22, and 24. The gas pressures reported below, such as 10 mtorr, represent the gas pressure of the respective gas as it is introduced into the sputtering chamber 14. In some embodiments, volatile materials 32, such as arsenic for example, are evaporated in a heated basket, illustrated as the heated evaporator 34. The system includes online pressure measurement 36. It also includes thickness measurement capability 38. The system optionally includes an online mass spectrometer 40 which may measure the gas content and accurately determine the partial pressure of the sputtering atmosphere.
[0058] Unless specifically noted, the following are common conditions for the sputtering described in the Examples:
[0059] 1. The distance between the sputtering target and the deposition substrate was about 1.5 inches.
[0060] 2. Radio Frequency was 13.56 MHz. It will be appreciated by those skilled in the art that much lower and much higher frequencies may be used in RF sputtering systems. However, for practical considerations and FCC regulations, the radio frequency used was 13.56 MHz.
[0061] 3. The atmosphere was maintained by using a continuous vacuum, and pressures were controlled by addition of indicated gases. Some residual atmospheric oxygen or moisture adsorbs on the metal surfaces within the sputtering chamber. Therefore, oxygen out-gases during the sputtering process at the operating temperature and pressure.
[0062] 4. The sputtering time was typically about 10 minutes, but some samples were sputtered for longer time periods, such as an hour, and some samples were sputtered for shorter periods, such as one minute. The sputtering time was selected to produce a film thickness of about one micron. It will be appreciated that several factors affect the film thickness, including, but not limited to, sputtering time, power, temperature, concentration of dopants, and evaporation of constituents of the sputtered thin film.
[0063] 5. One inch RF magnetron sputtering head was used with water cooling.
[0064] 6. All samples were tested for semiconductor type by Seebeck and Hall measurement.
[0065] 7. All chemicals were high purity from Alfa Aesar.
[0066] 8. In most cases, the operating condition ranges and experimental result ranges are drawn from multiple experiments. Thus, the reported examples and results may represent a composite of several actual experiments.
Example 1
Sputtering of ZnO with Arsenic as a Dopant
[0067] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was ZnO (0.99-0.95 moles)+As (0.01-0.05 moles). The preferred target composition was ZnO (0.98 moles)+As (0.02 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 60 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr and O2 at a gas pressure of about 1 to 4 mtorr. The preferred sputtering atmosphere pressures were about 9 mtorr argon and about 1 mtorr O2.
[0068] The resulting transparent p-type zinc oxide layer had a resistance of about 10,000 ohms/square. After annealing at 440° C. in air, the resistance dropped to about 1,000 ohms/square. In another composition prepared in accordance with the procedure of this Example, the transparent p-type zinc oxide layer had a resistance ranging from 200,000 ohms/square to 10,000,000 ohms/square. This composition was not subsequently annealed.
Example 2
Sputtering of ZnO with Arsenic as a Dopant
[0069] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was ZnO (0.99-0.95 moles)+As (0.01-0.05 moles). The preferred target composition was ZnO (0.98 moles)+As (0.02 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 60 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr and H2 at a gas pressure of about 1 to 4 mtorr. The preferred sputtering atmosphere pressures were about 9 mtorr argon and about 1 mtorr H2.
[0070] The resulting transparent p-type zinc oxide layer had a resistance of about 500 ohms/square. Without being bound by theory, it is believed that the hydrogen gas may be moderating the concentration of oxygen in the sputtering atmosphere.
Example 3
Sputtering of ZnO with Arsenic as a Dopant
[0071] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was ZnO (0.99-0.95 moles)+As (0.01-0.05 moles). The preferred target composition was ZnO (0.975 moles)+As (0.025 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 60 to 90 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. The preferred sputtering atmosphere pressure was about 9 mtorr argon.
[0072] The resulting transparent p-type zinc oxide layer had a resistance of about 1000 ohms/square. The resulting p-type zinc oxide was analyzed by X-ray Photoelectron Spectroscopy (XPS). A graph of the XPS data is shown in FIG. 2 . The data from FIG. 2 show arsenic in zinc oxide with a concentration of about 0.25 mole percent.
Example 4
Sputtering of ZnO with Arsenic as a Dopant
[0073] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. A First Composition Layer comprising zinc and arsenic was deposited onto the self supporting substrate.
[0074] In one example, the First Composition Layer was deposited by thermal evaporation of zinc arsenide (Zn3As2 or ZnAs2) for a period of about 2-60 seconds, with a preferred period of about 14 seconds. The substrate temperature was about 360° C. Thermal evaporation is a well known technique for depositing thin films, particularly metal and metal alloys. Subsequent analysis of the First Composition Layer indicated that it contained zinc and arsenic in approximately equal atomic amounts. This suggests that the stoichiometry of the zinc arsenide had changed during thermal evaporation or that it contained a mixture of zinc arsenide molecules.
[0075] The following sequential basic steps take place: (i) a vapor is generated by boiling or subliming a source material, (ii) the vapor is transported from the source to the substrate, and (iii) the vapor is condensed to a solid film on the substrate surface. In the evaporative deposition process, a substrate is placed in a low-pressure chamber. A tungsten crucible is disposed below the substrate. The desired source material or mixture of source materials is placed in the crucible and heated to a temperature sufficiently high to evaporate the source material. The source material vapor condenses on the substrate, which may or may not be heated. Heating the substrate may enhance the bond between the deposited source material film and the substrate. The evaporative deposition process may be completed in less than a minute, and usually a few seconds.
[0076] In another example, the First Composition Layer was deposited by RF sputtering. In yet another example, the First Composition Layer was deposited by the combination of thermal evaporation and RF sputtering. It will be appreciated that the First Composition Layer may be deposited using other known, conventional, or novel deposition techniques, including, but not limited to, RF sputtering and evaporative deposition techniques described above, as well as chemical vapor deposition (CVD), metal organic chemical vapor deposition (MOCVD), other evaporation and sputtering techniques, and combinations of these and other thin film deposition technologies.
[0077] Preparing a thin film by evaporation alone is a very quick process that is completed in a matter of seconds, but it is difficult to properly control the resulting thin film. In contrast, sputtering alone is a slow process that requires many minutes to complete. The combination of sputtering and thermal evaporation includes heat to facilitate evaporation of the source material and a RF field to induce sputtering. Alternatively, the RF field can be used to heat the source material disposed close to the RF magnetron head sufficiently to evaporate the source material for deposition by thermal evaporation. In this case, a small amount of sputtering will also occur. The resulting thin film is of good quality and quickly prepared. In this case, the combination of sputtering and evaporation was used to deposit Zn3As2 onto a fused silica substrate at 350° C. for about 50 seconds.
[0078] A Second Composition Layer comprising zinc oxide was deposited onto the First Composition Layer by RF sputtering. The sputtering target composition was ZnO. The substrate temperature was between 400 and 550° C. The preferred temperature was about 450° C. The RF power was between 20 and 120 watts. The preferred power was about 100 watts. The sputtering time was between 10 and 40 minutes, and preferably about 20 minutes. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. The preferred sputtering atmosphere pressure was about 10 mtorr argon.
[0079] The resulting p-type zinc oxide layer had a resistance of about 2,000 to 50,000 ohms/square and a resistivity of about 1.4 ohm·cm. The variable resistance may be attributed to variable thickness of the p-type zinc oxide layer. The concentration of arsenic was about 1.74×1018 per cm3 and was measured by the Hall effect technique. Without being bound by theory, it is believed that a quantity of arsenic may be evaporated during the sputtering step and become part of the sputtering plasma such that ZnO doped with arsenic was deposited onto substrate.
[0080] The photoluminescence of arsenic doped p-type zinc oxide was measured and compared against undoped, bulk, n-type zinc oxide and phosphorus doped p-type zinc oxide. This comparison is shown in FIG. 3 . The distinctly different photoluminescence between n-type and p-type zinc oxide is apparent. Moreover, the arsenic doped zinc oxide shows photoluminescence consistent with the phosphorus doped zinc oxide. A noticeable luminescent peak at about 3.3568 eV was observed with both phosphorus doped and arsenic doped p-type zinc oxide compositions.
[0081] The resistance and mobility of the p-type zinc oxide were measured and are shown graphically in FIG. 4 . The slope of the mobility curve provides an indication of how deep the centers are located. A sample of the arsenic doped p-type zinc oxide film was analyzed by Secondary Ion Mass Spectroscopy (SIMS) and measured against a calibrated standard. The results, shown graphically in FIG. 5 , indicate stable and consistent arsenic doping at a concentration of about 1020 atoms/cm3 to a depth of about 60 nm. Based upon the SIMS data, the composition of the arsenic doped p-type zinc oxide is labeled on the Zn—O-As ternary diagram of FIG. 17 . Another p-type zinc oxide sample prepared according to the procedure of this Example. It had a composition of Zn0.41O0.59As9.43×10−4 . It had an arsenic content of about 4.3×1019 arsenic atoms/cm3 to a depth of about 450 nm.
[0082] A region of the arsenic doped p-type zinc oxide that was sputtered directly onto a fused silica substrate was analyzed by X-ray diffraction. A graph of the X-ray diffraction pattern is shown in FIG. 7 illustrating a single dominant peak representing the (002) plane. This indicates that single crystal p-type zinc oxide was deposited directly onto the amorphous fused silica substrate. By way of comparison, an X-ray diffraction pattern of polycrystalline zinc oxide is shown in FIG. 6 .
Example 5
Sputtering of ZnO with Arsenic as a Dopant
[0083] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was Zn (0.99-0.95 moles)+As2O3 (0.01-0.05 moles). The preferred target composition was about Zn (0.99 moles)+As2O3 (0.01 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 15 and 40 watts. The preferred power was about 30 watts. A lower power was used in this example to keep the powdered zinc metal in the target from being quickly vaporized and dispersed during the sputtering processing. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr and O2 at a gas pressure of about 1 to 4 mtorr. The preferred sputtering atmosphere pressures were about 10 mtorr argon and about 1 mtorr O2.
[0084] The resulting transparent p-type zinc oxide layer had a resistance of about 100,000 ohms/square.
Example 6
Sputtering of ZnO with Arsenic as a Dopant
[0085] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was ZnO (0.99-0.95 moles)+As2O3 (0.01-0.05 moles). The preferred target composition was ZnO (0.99 moles)+As2O3 (0.01 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 60 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. The preferred sputtering atmosphere pressure was about 10 mtorr argon.
[0086] The resulting transparent p-type zinc oxide layer had a resistance of about 100,000 ohms/square.
Example 7
Sputtering of ZnO with Antimony as a Dopant
[0087] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was Zn (0.99-0.95 moles)+Sb (0.01-0.05 moles). The preferred target composition was Zn (0.98 moles)+Sb (0.02 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 90 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. The preferred sputtering atmosphere pressure was about 10 mtorr argon.
[0088] The resulting transparent p-type zinc oxide layer had a resistance of about 600,000 ohms/square. Without being bound by theory, it is believed that the oxygen needed to form the zinc oxide crystal lattice was obtained from residual oxygen in the sputtering system atmosphere.
[0089] The target composition is not limited to metallic zinc and antimony. The target may comprise zinc oxide and antimony metal, zinc metal and antimony oxide, and zinc oxide and antimony oxide. The sputtering atmosphere may optionally include either hydrogen gas or oxygen gas at a gas pressure of about 0.1 to 4 mtorr in addition to the inert sputtering gas.
Example 8
Sputtering of ZnO with Antimony as a Dopant
[0090] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was ZnO (0.99-0.95 moles)+Sb (0.01-0.05 moles). The preferred target composition was ZnO (0.98 moles)+Sb (0.02 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 90 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. The preferred sputtering atmosphere pressure was about 10 mtorr argon.
[0091] The resulting transparent p-type zinc oxide layer had a sheet resistivity of about 6.8×10−5 ohm·cm and a mobility of about 169 cm2/V·sec. The concentration of antimony was about 1.3×1021 atoms per cm3 measured by the Hall effect technique. A sample of the antimony doped p-type zinc oxide film was analyzed by Secondary Ion Mass Spectroscopy (SIMS) and measured against an antimony doped silica standard. The results were valid within a factor of 2. The results, shown graphically in FIG. 8 , indicate stable and consistent arsenic doping at a concentration of about 1020 atoms/cm3 to a depth of about 270 nm. The antimony concentration increased to about 1021 close to the fused silica substrate. Portions of the sample were visually transparent. Another sample of the antimony doped p-type zinc oxide layer prepared in the same manner had a sheet resistivity of about 9.4×10−5 ohm·cm and a mobility of about 108 cm2/V·sec. The concentration of antimony was about 6.34×1020 atoms per cm3 measured by the Hall effect technique.
Example 9
Sputtering of ZnO with Antimony as a Dopant
[0092] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. The sputtering target composition was ZnO (0.99-0.95 moles)+Sb (0.01-0.05 moles). The preferred target composition was ZnO (0.98 moles)+Sb (0.02 moles). The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 90 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr and oxygen gas at a pressure of about 1 mtorr. The preferred sputtering atmosphere pressure was about 10 mtorr argon and 1 mtorr oxygen.
[0093] The resulting transparent p-type zinc oxide layer had better crystallinity and mobility compared to the other antimony-doped zinc oxide thin films prepared above.
Example 10
Sputtering of ZnO with Copper as a Dopant
[0094] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. A First Composition Layer comprising copper was deposited onto the self supporting substrate by RF sputtering for a period of from 5 to 40 minutes, with a preferred period of about 10 minutes at room temperature.
[0095] A Second Composition Layer comprising zinc oxide was deposited onto the First Composition Layer by RF sputtering. The sputtering target composition was ZnO. The substrate temperature was between 400 and 550° C. The preferred temperature was about 450° C. The RF power was between 20 and 120 watts. The preferred power was about 100 watts. The sputtering time was between 10 and 40 minutes, and preferably about 20 minutes. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. The preferred sputtering atmosphere pressure was about 10 mtorr argon.
[0096] At low concentration, copper may counteract the natural n-type property of ZnO resulting in a neutral or p-type semiconductor with low resistance. Without being bound by theory, it is believed that a quantity of copper may be evaporated during the sputtering step and become part of the sputtering plasma such that ZnO doped with copper was deposited onto substrate.
Example 11
Sputtering of ZnO with Arsenic as a Dopant
[0097] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Both fused silica and silicon wafers were used as the self supporting substrate. A First Composition Layer comprising zinc and arsenic was deposited onto the self supporting substrate. The First Composition Layer included Zn3As2, ZnAs2, or a mixture thereof. In one example, the zinc/arsenic layer was deposited by thermal evaporation for a period of about 2-60 seconds, with a preferred period of about 14 seconds. The temperature was about 360° C. The First Composition Layer may also be deposited by RF sputtering.
[0098] A Second Composition Layer comprising zinc oxide was deposited onto the First Composition Layer by RF sputtering. The sputtering target composition was ZnO. The substrate temperature was between 400 and 550° C. The preferred temperature was about 450° C. The RF power was between 20 and 120 watts. The preferred power was about 100 watts. The sputtering time was between 10 and 40 minutes, and preferably about 20 minutes. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr and hydrogen at a gas pressure of about 0.1 to 4 mtorr. The preferred sputtering atmosphere pressure was about 10 mtorr argon.
[0099] The resulting p-type zinc oxide layer had a resistance of about 10 to 200 ohms/square.
Example 12
Sputtering of ZnO with Antimony as a Dopant
[0100] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering in accordance with the procedure of Example 11, except that the First Composition Layer comprised zinc and antimony. The resulting p-type zinc oxide layer showed high mobility.
Example 13
Sputtering of ZnO with Antimony as a Dopant
[0101] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering in accordance with the procedure of Example 12, except that the First Composition Layer comprised antimony. The antimony was deposited onto the self supporting substrate by thermal evaporation. The resulting p-type zinc oxide layer showed high mobility.
Example 14
Sputtering of ZnO with Arsenic as Dopant
[0102] A thin film of p-type zinc oxide was deposited onto a self supporting substrate by RF sputtering. Fused silica was used as the self supporting substrate. The sputtering target composition was ZnO. The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 60 watts. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. In addition, a basket containing arsenic was heated to a controlled temperature sufficient to evaporate the arsenic. The basket was positioned such that the arsenic was evaporated directly onto the fused silica at the same time the zinc oxide was sputtered onto the fused silica.
[0103] The resulting transparent p-type zinc oxide layer displayed visible diffraction rings, but was very clear and transparent. It will be appreciated that this process may be adapted for use with other p-type dopants besides arsenic.
[0104] Based upon arsenic vapor pressure data, As4 has a higher vapor pressure at a given temperature when compared to As3, As2, and As. Therefore, it is presently believed that As4 is the dominant volatile arsenic species at typical operating conditions. Without being bound by theory, it is believed As4 must be broken into individual arsenic atoms to be incorporated into the zinc oxide. An apparent threshold RF power of about 60 watts has been observed for the given experimental sputtering system used herein. It will be appreciated that this threshold RF power may vary depending upon the sputtering system used. Likewise, it will be appreciated that other means besides a RF field may be used to break the As4 molecular bonds.
[0105] A similar phenomenon has been observed with respect to antimony vapor pressures as with arsenic discussed above. Antimony generally requires a higher temperature to achieve the same vapor pressure as arsenic. Likewise, an apparent threshold RF power of about 90 watts has been observed for the given experimental sputtering system used herein.
Example 15
Sputtering of ZnS with Arsenic as Dopant
[0106] A thin film of p-type zinc sulfide was deposited onto a self supporting substrate by RF sputtering. Fused silica was used as the self supporting substrate. The sputtering target composition was ZnS. The substrate temperature was between 350 and 550° C. The preferred temperature was about 400° C. The RF power was between 20 and 120 watts. The preferred power was about 60 watts. The sputtering time was about 1 to 2 minutes. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. In addition, a basket containing arsenic was heated to a controlled temperature sufficient to evaporate the arsenic. The basket was positioned such that the arsenic was evaporated directly onto the fused silica at the same time the zinc sulfide was sputtered onto the fused silica. It will be appreciated that this process may be adapted for use with other p-type dopants besides arsenic.
Example 16
Conversion of ZnS to ZnO with Arsenic as a Dopant
[0107] A thin film of p-type zinc sulfide was prepared in accordance with Example 15. The p-type ZnS was used as a precursor for preparing p-type ZnO. The ZnS thin film was placed in furnace containing oxygen to convert the ZnS into ZnO. The furnace temperature, atmosphere, and annealing time may be varied to control the extent of ZnS conversion. For instance, a p-type zinc oxysulfide semiconductor may be prepared by limiting the amount of oxygen in the atmosphere and preventing complete oxidation of the ZnS. In addition, the vapor pressure of the zinc, oxygen, and arsenic may be controlled to tailor the resulting dopant concentration in the semiconductor material. It will be appreciated that this process may be adapted for use with other p-type dopants besides arsenic.
Example 17
Evaporative Deposition of ZnO with Arsenic as a Dopant
[0108] A stable, p-type zinc oxide semiconductor material was prepared. Zinc metal, doped with 2 mole % arsenic, was deposited onto a fused silica substrate by thermal evaporation in an oxygen-rich atmosphere containing 20 mtorr argon and 10 mtorr oxygen at a temperature of about 430° C. During the deposition process, the zinc and/or arsenic was partially oxidized. The resulting As-doped ZnO thin film exhibited p-type characteristics. It had a Seebeck voltage of about positive 6 mV D.C. Increasing the oxygen pressure may result in a more complete formation of ZnO. While no further heating or annealing was performed in this example, additional heating or annealing may be desirable to control the level of zinc oxidation and/or optimize the electronic properties of the p-type semiconductor material.
Example 18
Deposition of Zinc Oxide with Arsenic as Dopant
[0109] A stable, p-type zinc oxide semiconductor material is prepared. Zinc arsenide is deposited onto a self-supporting substrate surface. The surface may be fused silica, silicon wafer, borosilicate glass, or similar self supporting substrate. The zinc arsenide may be Zn3As2, ZnAs2, or a mixture thereof. In one example, the zinc arsenide layer is deposited by thermal evaporation for a period of about 2-60 seconds, with a preferred period of about 14 seconds. In another embodiment, the zinc arsenide layer may is deposited by sputtering. In yet another embodiment, the zinc arsenide layer is deposited by CVD or MOCVD.
[0110] The zinc arsenide layer is thermally annealed in an atmosphere containing oxygen for sufficient time period to oxidize the zinc arsenide layer and form zinc oxide doped with arsenic. At a given annealing temperature, some quantity of arsenic and zinc may evaporate from the zinc arsenide. Such evaporation may be taken into consideration in determining the starting composition of the zinc arsenide. Similarly, under these annealing conditions, it may be desirable to introduce additional amounts of gaseous arsenic, zinc, or oxygen to inhibit evaporation of these elements from the zinc oxide film and to influence the final composition of the semiconductor material.
Example 19
Spin Coating of Arsenic-Doped ZnO
[0111] A stable, p-type zinc oxide semiconductor material may be prepared by spin coating using arsenic as the dopant. Fused silica is used as the self supporting substrate. Zinc 2-4 pentanedionate is used as the zinc source and arsenic III ethoxide is used as the arsenic source. These compounds are dissolved in butanol which serves as a common solvent. This solution is spun onto a fused silica slide.
[0112] After a layer is spun on the substrate, it is heated to about 600° C. for about 10 minutes for pyrolysis of the organics. This procedure is repeated 5 or 6 times to get the desired film thickness. The substrate is annealed at about 700° C. for 1 to 5 hours in a nitrogen atmosphere. Control of the partial pressures of all inorganic components is desirable for the desired doped zinc oxide composition, otherwise evaporation or one or more ingredients or formation of undesired compounds may occur. The oxygen can come from the atmosphere or can come from being part of the organic precursors.
Example 20
Spin Coating of Antimony-Doped ZnO
[0113] A stable, p-type zinc oxide semiconductor material may be prepared by spin coating in accordance with the method of Example 19, except that antimony is used as the dopant instead of arsenic. Antimony chloride (SbCl3) is used as the antimony source.
Example 21
Spin Coating of P-Type ZnS
[0114] A stable, p-type zinc sulfide semiconductor material may be prepared by spin coating in accordance with the spin coating methods described above, except that a sulfur-containing organic compound is used in combination with the zinc compound and the selected p-type dopant compound. Sulfur can be engineered into organic compounds compatible with the spin coating. An example of a possible organic sulfur compound that may be used in the spin coating is 8-(p-sulfophenyl) theophylline, which is soluble in methanol and ethanol. In such cases, one may control the oxygen and sulfur partial pressures to obtain the desired p-type ZnS. For example, if oxygen is present, then a zinc oxysulfide compound may be prepared. The partial pressures of any component in the atmosphere can be determined experimentally or they can be calculated from thermodynamic data.
Example 22
MOCVD of P-Type ZnO
[0115] A stable, p-type zinc oxide semiconductor material may be prepared by metal organic chemical vapor deposition (MOCVD) using arsenic, antimony, or other p-type dopant. A typical MOCVD process is described above.
Example 23
MOCVD of Zinc Sulfide
[0116] A stable, p-type zinc sulfide semiconductor material may be prepared by MOCVD in accordance with the method of Example 22, except that a sulfur-containing organic compound is used in combination with the zinc compound and the selected p-type dopant compound. Sulfur can be engineered into organic compounds compatible with the MOCVD. In such cases, it is important to control the oxygen and sulfur partial pressures to obtain the desired p-type ZnS material. For example, if oxygen is present, then a zinc oxysulfide compound may be prepared.
Example 24
Bulk Preparation of Copper-Doped ZnO
[0117] A stable, p-type zinc oxide semiconductor material was prepared using copper as the dopant. The copper-doped zinc oxide p-type semiconductor was prepared in bulk by mixing 90% (atomic percent) zinc oxide and 10% (atomic percent) copper oxide powder and heating the mixture in a furnace. A Seebeck measurement of the resulting bulk material was made to confirm that the material was a p-type semiconductor. It had a Seebeck voltage in the range from about positive 40 mV D.C. to about 90 mV D.C. The electrical resistance of the resulting material was about 600 Kohms/square to 900 Kohms/square. This compound was not optimized. It is believed that smaller amounts of copper oxide may provide better results.
Example 25
Fabrication of Zinc Oxide P/N Junction
[0118] A zinc oxide p/n junction 50 was fabricated as shown schematically in FIG. 9 . A thin film of p-type zinc oxide 52 was deposited onto a self supporting silicon wafer substrate by RF sputtering in accordance with Example 4. In Example 4, a thin film of Zn3As2 56 was first deposited onto the silicon wafer 54 and the p-type zinc oxide 52 was sputtered on top of the zinc arsenide 56. A thin film of n-type zinc oxide was sputtered on top of the p-type zinc oxide at about 300° C. The sputtering target included ZnO (99.925 mole %) and Ga2O3 (0.075 mole %) that had been mixed, sintered, and annealed at about 1100° C. The sputtering step occurred at a temperature of about 350° C. The sputtering atmosphere included argon at a gas pressure of about 4 to 20 mtorr. About 10% hydrogen gas may alternatively be included in the sputtering atmosphere to produce n-type ZnO.
[0119] A positive electrode 60 and a negative electrode 62 were attached to the p/n junction 50 as shown in FIG. 9 . Current vs. voltage was measured and shown in the rectification graph of FIG. 11 . A luminescent emission at room temperature was briefly observed before the p/n junction failed. Failure occurred because the electrical resistance dropped too quickly allowing excessive current to overpower the p/n junction. A graph of the measured emission spectrum is shown in FIG. 10 . Because of the short duration of the light emission, it was not possible to obtain a detailed measurement of the spectrum.
[0120] Semiconductor heterostructures may be fabricated based upon p/n junction described above. These devices may be prepared by depositing multiple layers of p-type and n-type group II-VI semiconductors. Such heterostructures may be fabricated using matching or compatible group II-VI crystals. Examples of two possible semiconductor heterostructure devices are illustrated in FIGS. 12 and 13 . It will be appreciated that the illustrated devices are given by way of example and not limitation. Persons skilled in the art will recognize that a numerous variations of these devices are possible.
[0121] The device shown in FIG. 12 includes a self supporting substrate 62. The substrate may be a known crystalline substrate or it may be a low cost substrate including, but not limited to, silicon wafers, polycrystalline alumina, and amorphous self supporting substrate surfaces like fused silica. A layer of n-type zinc oxide 64 doped with an n-type dopant, such as gallium, is deposited on the substrate 62. The n-type zinc oxide layer 64 may be about 0.4 μm thick. The device may include additional n-type zinc oxide layers 66, 68, comprising magnesium and cadmium alloys. For example, layer 66 may have a composition of Mg0.15Zn0.85O doped with gallium, and it may have a thickness of about 0.15 μm. Layer 68 may have a composition of Cd0.06Zn0.94O doped with gallium, and it may have a thickness of about 0.05 μm. The thin cadmium zinc oxide alloy layer 68 is the active region wherein light generation occurs. Deposited on top of the active region layer 68 are one or more p-type zinc layers 70, 72. Layer 70 may have a composition of Mg0.15Zn0.85O doped with arsenic, and it may have a thickness of about 0.15 μm. Layer 72 may be p-type zinc oxide doped with a p-type dopant, such as arsenic.
[0122] It will be appreciated by persons having ordinary skill in the art that actual composition of the n-type and p-type zinc oxide layers may vary. Similarly the concentration of magnesium and cadmium in the zinc oxide alloys may vary.
[0123] FIG. 13 illustrates a device substantially identical to the device of FIG. 12 , except that there is no separate active region.
[0124] Single or multiple quantum well (MQW) heterostructures may be fabricated to render the p/n junction more efficient. A single quantum well is made of two alternating semiconductor materials. One layer is a barrier layer defined by a higher band gap than the second layer. The second layer's band gap defines the bottom of the quantum well. For example, MgO may be alloyed with ZnO to form the barrier layer, and the undoped ZnO will define the bottom of the well. This produces a more efficient device and raises the band edge. Conversely, CdO may be alloyed with ZnO to define the bottom layer of the quantum well, and the undoped ZnO defines the barrier layer. This produces a more efficient device and lowers the band edge.
[0125] An additional advantage of a quantum well is that the layers can be mechanically strained to raise or lower the band edge. Mechanical strain may exist if the two layers have slightly different crystal lattice constants. For most zinc oxide materials the band edge is around 390 nm, but some of the zinc oxide semiconductor materials fabricated in accordance with the present invention had a band edge of about 370 nm.
[0126] The number of quantum wells may vary. Good results may be obtained with just one quantum well. Typically the number of quantum wells may range from about 1 to 10, and more preferably from about 3 to 7 quantum wells. The total thickness of the quantum well alternating layers must in the vicinity of, or less than, the electron de Broglie wavelength (100 Å). These heterostructures may be fabricated through a chemical deposition process, including but not limited to those described above, such as sputtering, CVD, MOCVD, etc.
[0127] For example, one possible MQW configuration for use in connection with zinc oxide semiconductor structure may include alternating layers of ZnO (20 Å-100 Å) and CdxZn1−xO (10 Å-25 Å). The cadmium content may be varied. The amount of cadmium in the cadmium zinc oxide alloy may vary depending on the desired shifting of the band gap. In one illustrative embodiment, the cadmium content may range from about 1 to 20 mole %, and more typically about 10 mole %. The cadmium zinc oxide alloy may be replaced with a magnesium zinc oxide alloy of the general formula MgxZn1−xO.
[0128] FIG. 14A is a schematic representation of a typical state of the art GaN-based semiconductor device 80 containing MQWs 82. It will be appreciated that GaN devices are complicated to manufacture because of the expensive sapphire or SiC substrate 84 and multiple layers 86, 88 required to match the crystal lattice of GaN and the substrate. In contrast, FIG. 14B is a schematic representation of a zinc oxide based semiconductor device 90 containing MQWs 92. Because single crystal zinc oxide 94 may be deposited directly on a low-cost substrate 96, such as fused silica or a silicon wafer, the zinc oxide based semiconductor device fabricated within the scope of the present invention represents a substantial improvement over conventional GaN-based semiconductor devices.
[0129] FIG. 15A is a schematic representation of one possible zinc oxide based semiconductor device 100 fabricated with MQWs. Three quantum wells are shown containing alternating layers of undoped ZnO 102 (20 Å-100 Å) and Cd0.2Zn0.8O 104 (10 Å-25 Å). The cadmium content may be varied. The amount of cadmium in the cadmium zinc oxide alloy 104 may vary depending on the desired shifting of the band gap. The cadmium content preferably ranges from about 1 to 20 mole %, and more typically about 10 mole %.
[0130] The semiconductor device 100 includes a layer of n-type zinc oxide 106, approximately 2 μm thick, doped with an n-type dopant, such as Ga or Al, deposited on a self supporting substrate 108. A layer of p-type zinc oxide 110, approximately 2 μm thick, doped with a p-type dopant, such as arsenic, may be deposited on top of the MQWs, layers 102, 104. A layer of p-type zinc oxide 112, approximately 5 μm thick, doped with a p-type dopant, such as arsenic, may be deposited on top of layer 110.
[0131] FIG. 15B is a schematic representation of a zinc oxide based semiconductor device 120 similar to that of FIG. 15A except that the quantum wells include a magnesium zinc oxide alloy instead of a cadmium zinc oxide alloy. The alternating layers of magnesium zinc oxide alloy 124 may have the formula Mg0.1Zn0.9O (10 Å-25 Å). The magnesium content may be varied. The amount of magnesium the magnesium zinc oxide alloy 124 may vary depending on the desired shifting of the band gap. The magnesium content preferably ranges from about 1 to 20 mole %, and more typically about 10 mole %.
[0132] FIG. 16A is a schematic representation of one possible zinc oxide based semiconductor device fabricated with a single quantum well having a composition substantially the same as the device shown in FIG. 15A . As mentioned above, the number of quantum wells can vary, just as the composition of the quantum well layers and the p-type and n-type semiconductor material used in the device.
[0133] FIG. 16B is a schematic representation of a zinc oxide based semiconductor device similar to that of FIG. 16A except that the quantum well includes a magnesium zinc oxide alloy instead of a cadmium zinc oxide alloy.
[0134] It will be appreciated that the present invention provides methods for fabricating group II-VI semiconductor devices. The fabrication methods are commercially viable. The resulting semiconductor materials exhibit good electronic and physical properties.
[0135] The present invention may be embodied in other specific forms without departing from its structures, methods, or other essential characteristics as broadly described herein and claimed hereinafter. The described embodiments are to be considered in all respects only as illustrative, and not restrictive. The scope of the invention is, therefore, indicated by the appended claims, rather than by the foregoing description. All changes that come within the meaning and range of equivalency of the claims are to be embraced within their scope.
Claims
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The invention claimed is:
1. A solid state device comprising a p-n junction containing a p-type group II-VI semiconductor material and an n-type semiconductor material, wherein the p-type group II-VI semiconductor comprises a single crystal thin film of a group II-VI semiconductor comprising atoms of group II elements and atoms of group VI elements, wherein the group II-VI semiconductor is doped with one or more p-type dopants selected from nitrogen, phosphorus, arsenic, antimony, bismuth, copper, and chalcogenides of the foregoing, and mixtures thereof, wherein the p-type dopant concentration in the group II-VI semiconductor is greater than about 1016 atoms·cm−3, wherein semiconductor resistivity is less than about 0.5 ohm·cm, and wherein the carrier mobility is greater than about 0.1 cm2/V·s, and wherein the p-type group II-VI semiconductor material has a luminescent peak at 3.357 eV.
2. A solid state device according to claim 1, wherein the group II elements are selected from zinc, cadmium, alkaline earth metals, and mixtures thereof.
3. A solid state device according to claim 1, wherein the group VI elements are selected from oxygen, sulfur, selenium, tellurium, and mixtures thereof.
4. A solid state device according to claim 1, wherein the p-type dopant is phosphorus.
5. A solid state device according to claim 1, wherein the p-type dopant is arsenic.
6. A solid state device according to claim 1, wherein the p-type dopant is antimony.
7. A solid state device according to claim 1, wherein the p-type dopant is bismuth.
8. A solid state device according to claim 1, wherein the thin film of a group II-VI semiconductor is deposited by a chemical deposition process selected from RF sputtering, CVD (chemical vapor deposition), MOCVD (metal organic chemical vapor deposition), spin coating, electrophoresis, and hydrothermal growth processes.
9. A solid state device according to claim 1, wherein the group II-VI semiconductor material is zinc oxide.
10. A solid state device according to claim 1, wherein the group II-VI semiconductor material is zinc sulfide.
11. A solid state device according to claim 1, wherein the device is a light emitting diode.
12. A solid state device according to claim 1, wherein the device is a laser diode.
13. A solid state device according to claim 1, wherein the device is a field effect transistor.
14. A solid state device according to claim 1, wherein the device is a photodetector.
15. A solid state device according to claim 1, wherein the device emits light at a wavelength in the range from about 207 nm to 810 nm.
16. A solid state device according to claim 1, wherein the device emits light at a wavelength of about 441.6 nm.
17. A solid state device according to claim 1, wherein the device emits light at a wavelength of about 325 nm.
18. A solid state device according to claim 1, wherein the group II-VI semiconductor material is disposed on an amorphous self supporting substrate surface.
19. A solid state device according to claim 1, wherein the n-type semiconductor material is an n-type group II-VI semiconductor.
20. A solid state device comprising a p-n junction containing a p-type zinc oxide and an n-type semiconductor material, wherein the p-type zinc oxide comprises single crystal zinc oxide that is doped with one or more p-type dopants, wherein the p-type dopant concentration in the zinc oxide is greater than about 1016 atoms·cm−3, wherein semiconductor resistivity is less than about 0.5 ohm·cm, and wherein the carrier mobility is greater than about 0.1 cm2/V·s, and wherein the p-type zinc oxide semiconductor material has a luminescent peak at 4 3.357 eV.
21. A solid state device according to claim 20, wherein the p-type dopant is phosphorus.
22. A solid state device according to claim 20, wherein the p-type dopant is arsenic.
23. A solid state device according to claim 20, wherein the p-type dopant is antimony.
24. A solid state device according to claim 20, wherein the p-type dopant is bismuth.
25. A solid state device according to claim 20, wherein the p-type dopant is copper.
26. A solid state device according to claim 20, wherein the single crystal zinc oxide further comprises magnesium oxide.
27. A solid state device according to claim 20, wherein the single crystal zinc oxide further comprises cadmium oxide.
28. A solid state device according to claim 20, wherein the n-type semiconductor material is an n-type zinc oxide.
29. A solid state device according to claim 28, wherein the n-type zinc oxide contains an n-type dopant selected from ions of Al, Ga, B, H, Yb and other rare earth elements, Y, Sc, and mixtures thereof.
30. A solid state device according to claim 20, wherein the device is a light emitting diode.
31. A solid state device according to claim 20, wherein the device is a laser diode.
32. A solid state device according to claim 20, wherein the device is a field effect transistor.
33. A solid state device according to claim 20, wherein the device is a photodetector.
34. A solid state device according to claim 20, wherein the device emits light at a wavelength in the range from about 310 nm to 660 nm.
35. A solid state device according to claim 20, wherein the device emits light at a wavelength of about 441.6 nm.
36. A solid state device according to claim 20, wherein the device emits light at a wavelength of about 325 nm.
37. A solid state device according to claim 20, wherein the single crystal zinc oxide is disposed on an amorphous self supporting substrate surface.
38. A solid state device according to claim 37, further comprising a barrier layer disposed between the single crystal zinc oxide and the amorphous self supporting substrate surface.
39. A solid state device comprising a p-n junction containing a p-type zinc oxide and an n-type semiconductor material, wherein the p-type zinc oxide comprises single crystal zinc oxide that is doped with a quantity of phosphorous, wherein the phosphorous dopant concentration in the zinc oxide is greater than about 1016 atoms·cm−3, wherein semiconductor resistivity is less than about 0.5 ohm·cm, and wherein the caffier mobility is greater than about 0.1 cm2/V·s, and wherein the p-type zinc oxide semiconductor material has a luminescent peak at 4 3.357 eV
40. A solid state device according to claim 39, wherein the p-type zinc oxide further comprises magnesium oxide.
41. A solid state device according to claim 39, wherein the p-type zinc oxide further comprises cadmium oxide.
Patent Citations (17)
| Patent | Date | Inventor | Cited By |
|---|---|---|---|
| US3664867(A) | 1972-05-01 | Galli et al. | Applicant |
| US3864725(A) | 1975-02-01 | Merrin | Examiner |
| US4399441(A) | 1983-08-01 | Vaughn et al. | Applicant |
| US5331655(A) | 1994-07-01 | Harder et al. | Examiner |
| US6291085(B1) | 2001-09-01 | White et al. | Examiner |
| US6589362(B2) | 2003-07-01 | Haga | Applicant |
| US6610141(B2) | 2003-08-01 | White et al. | Applicant |
| US6617183(B2) | 2003-09-01 | Kadota et al. | Applicant |
| US6624441(B2) | 2003-09-01 | Cantwell et al. | Applicant |
| US6664565(B1) | 2003-12-01 | Sano et al. | Applicant |
| US6673478(B2) | 2004-01-01 | Kato et al. | Applicant |
| US6707074(B2) | 2004-03-01 | Yoshii et al. | Examiner |
| US6838308(B2) | 2005-01-01 | Haga | Examiner |
| US2003/0226499(A1) | 2003-12-01 | Teherani | Applicant |
| US2004/0061114(A1) | 2004-04-01 | Yan et al. | Applicant |
| EP1219731(A1) | 2002-07-01 | Applicant | |
| JP2002-68890(A1) | 2002-03-01 | Applicant |
Non-Patent Literature (146)
- Itani, Kenya, et al., “Low-Dislocation-Density GaAs Wafers Grown by Vertical Gradient Freeze Process, Suitable for Mass prodution of Semiconductor Lasers,” Hitachi Cable Review No. 20, Aug. 2001, pp. 35-38.Applicant
- Look, D.C., et al. “The Future of ZnO Light Emitters,” Phys. Stat. Sol. (2004), pp. 1-10.Applicant
- Pearton, S.J., et al. “Wide Band Gap Ferromagnetic Semiconductors and Oxides,” Journal of Applied Physics vol. 93, No. 1, Jan. 1, 2003, pp. 1-13.Applicant
- Web Page '99 SBIR Phase I . . . Topic 14—Electronic Materials, http://www-ee.eng.buffalo.edu/faculty/paololin/492/semicon.pdf, “Low-Temperature Hydrothermal Growth of Zno for Seminconductor Substrates,” Feb. 26, 2004, 2 pages.Applicant
- Web Page “Semiconductor Photonics”, 3 pages.Applicant
- Aulbur, W.; Density Functinal Theory: Basic Ideas & Applications; Ohio State University.Applicant
- Look, D.C., and Claflin, B.; P-type doping and devices based on ZnO; Aug. 2003; Wiley-VCH Verlag GmbH & Co.Applicant
- Zunger, A.; Practical Doping Principles; NCPV and Solar Program Review Meeting 2003; pp. 831-835.Applicant
- Zhang, S.B., Wei, S.H., and Zunger, A.; Intrinsic n-type versus p-type doping asymmetry and the defect physics of ZnO; Physical Review B; Jan. 31, 2001; pp. 075205-1-075205-7; vol. 63; The American Physical Society.Applicant
- Limpijumnong, S., Zhang, S.B., Wei, S-H., and Park C.H; Doping by Large-Size-Mismatched Impurities: The Microscopic Orgin of Arsenic- or Antimony-Doped p-Type Zinc Oxide; Physical Review Letters; Apr. 16, 2004; vol. 92, No. 15; The American Physical Society.Applicant
- Yamamoto, T., and Katayama-Yoshida, H.; Solutiion Using a Codoping Method to Unipolarity for the Fabrication of p-type ZnO; Japanese Journal of Applied Physics; Feb. 15, 1999; pp. L 166-L 169, vol. 38; Japanese Journal of Applied Physics Publication Board.Applicant
- Park, C.H., Zhang, S.B., and Wei, S-H.; Origin of p-type doping difficulty in ZnO: The impurity perspective; Physical Review B; Aug. 5, 2002; pp. 073202-1-073202-3; vol. 66; The American Physical Society.Applicant
- Tsukazaki, A., Atsushi, T., Ohtomo, A., Onuma, T., Ohtani, M., Makino, T., et al; Repeated temperature modulation epitaxy for p-type doping and light-emitting diode based on ZnO; Nature Materials; Jan. 2005; pp. 42-46; vol. 4; Nature Publishing Group.Applicant
- Nonaka, M., Matsushima, S., Mizuno, M., and Kobayashi, K.; Electronic Structure of Group III Elements Dopes into ZnO by Using Molecular Orbital Calculation; Chemistry Letters 2002; Feb. 20, 2002; pp. 580-581; The Chemical Society of Japan.Applicant
- Wang, L.G., and Zunger, A.; Cluster-Doping Approach for Wide-Gap Semiconductors: The Case of p-type ZnO; Physical Review Letters; Jun. 27, 2003; pp. 256401-1-256401-4; vol. 90, No. 25; The American Physical Society.Applicant
- Norton, D.P., Heo, Y.W., Ivill, M.P., IP, K., Pearton, S.J., et al; ZnO: growth, doping and processing; Materialstoday; Jun. 2004; Elsevier Ltd.Applicant
- Lee, E-C., Kim, Y.-S., Jin, Y.-G., and Chang, K.J.; First-Principles Study of p-Type Doping and Codoping in ZnO; Journal of the Korean Physical Society; Dec. 2001; pp. S23-S26; vol. 39.Applicant
- Morhain, C., Teisseire, M., Vezian, S., Vigue, F., Raymond, F., et al; Spectroscopy of Excitons, Bound Excitons and Impurities in h-ZnO Epilayers; Sep. 30, 2001; pp. 881-885; vol. 229, No. 2; Wiley VCH; Berlin.Applicant
- Bandyopadhyay, S., Paul, G.K., Roy, R., Sen, S.K., and Sen, S; Study of structural and electrical properties of grain-boundary modified ZnO films prepared by sol-gel technique; Materials Chemistry and Physics; May 17, 2001; pp. 83-91; vol. 74; Elsevier Science B.V.Applicant
- Wilkinson, J., Xiong, G., Ucer, K.B., and Williams, R.T.; Lifetime and Oscillator Strength of Excitonic Luminescence in Zinc Oxide; Department of Physics, Wake Forest University, Winston-Salem, N.C.Applicant
- Kobayashi, A., Sankey, O.F., and Dow, J.D.; Deep energy levels of defects in the wurtzite semiconductors AIN, CdS, CdSe, and ZnO; Physical Review B; Jul. 15, 1983; pp. 946-956; vol. 28, No. 2; The American Physical Society.Applicant
- Daneu, N., Reenik, A., and Bernik, S.; Grain Growth Control in Sb2O3-Doped Zinc Oxide; Journal of the American Ceramic Society; 2003; pp. 1379-1394; vol. 86, No. 8.Applicant
- Ohyama, M.; Sol-Gel Preparation of Transparent and Conductive Aluminum-Doped Zinc Oxide Films with Highly Preferential Crystal Orientation; Journal of the American Ceramic Society; 1998; pp. 1622-1632; vol. 81, No. 6.Applicant
- Duan, X.L., Yean, D.R., Cheng, X.F., Sun. H.Q., Sun, Z.H., et al; Microstructure and Properties of Co2: ZnAl2O4/Si02 Nanocomposite Glasses Prepared by Sol-Gel Method; Journal of the American Ceramic Society; 2005; pp. 399-403; vol. 88, No. 2.Applicant
- Sohn, K.S., Hwang, D.K., and Myoung, J.M.; Time Integrated/Resolved Photoluminescense of ZnO Films Deposited on Sapphire and GaAs; Japanese Journal of Applied Physics; Dec. 2003; pp. 7376-7378; The Japan Society of Applied Physics.Applicant
- Sun, X.W.; Optical properties of epitaxially grown zinc oxide films on sapphire by pulsed laser deposition; Journal of Applied Physics; Jul. 1, 1999; pp. 408-411; vol. 86, No. 1; American Institute of Physics.Applicant
- Burden, A.P., Bishop, H.E., Brierley, M., Friday, J.M., Hood, C., et al.; Incorporating consumer-priced field emitting inks into arrays of triode devices; Solid State Electronics; 2001; pp. 987-996; vol. 45; Printable Field Emitters Ltd.Applicant
- Minami, T., Miyata, T., Shirai, T., and Nakatani, T.; Electroluminescent Oxide Phosphor Thin Films Prepared by a Sol-gel Process; Mat. Res. Soc. Symp. Proc.; 2000; pp. Q4.3.1-Q4.3.6; vol. 621; Materials Research Society.Applicant
- Qiu, C., Chen, H., Wong, M., and Kwok, H.S.; Dependence of the Current and Power Efficiencies of Organic Light-Emitting Diode on the Thickness of the Constituent Organic Layers; IEEE Transactions On Electron Devices; Sep. 2001; pp. 2131-2137; vol. 48; IEEE.Applicant
- Matsuda, T., Kawabe, M., Iwata, H., and Ohzone, T.; Visible Electroluminescence from MOS Capacitors with Si-implanted SiO2; IEICE Trans. Electron.; Sep. 11, 2002; pp/ 1895-1904; vol. E85-C, No. 11.Applicant
- Ong, H.C., Li, A.S.K., and Du, G.T.; Depth profiling of ZnO thin films by cathodoluminescence; Applied Physics Letters; Apr. 30, 2001; pp. 2667-2669; vol. 78, No. 18; American Institute of Physics.Applicant
- Washington, P.L., Ong, H.C., Dai, J.Y., and Chang, R.P.H.; Determination of the optical constants of zinc oxide thin films by spectroscopic ellipsometry; Applied Physics Letter; Jun. 22, 1998; pp. 3261-3263; vol. 72, No. 25; American Institute of Physics.Applicant
- Sekiguchi, T., Ohashi, N., and Yamane, H.; Cathodoluminescence Study of ZnO and GaN; Solid State Phenomena; 1998; pp. 171-182; vols. 63-64; Scitec Publications; Switzerland.Applicant
- Kouyate, D., Ronfard-Haret, J.-C., and Kossanyi, J.; Photo- and electro-luminescence of rare earth-doped semiconducting zinc oxide electrodes: Emission from both the dopant and the support; Journal of Luminescence; 1991; pp. 205-210; vol. 50; Elsevier Science Publishers B.V.Applicant
- Kossanyi, J., Kouyate, D., Pouliquen, J., Ronfard-Haret, J.C., Valat, P., et al.; Photoluminescence of Semiconducting Zinc Oxide Containing Rare Earth Ions as Impurities; Journal of Luminescence; 1990; pp. 17-24; vol. 46; Elsevier Science Publishers B.V. (north-Holland).Applicant
- Wang, Y.G., Lau, S.P., Lee, H.W., Yu. S.F., Tay, B.K., et al.; Photolumimescence study of ZnO films prepared by thermal oxidation of Zn metallic films in air; Journal of Applied Physics; Jul. 1, 2003; pp. 354-358; vol. 94, No. 1; American Institute of Physics.Applicant
- Yu, S.F., Yuen, C., Lau, S.P., Wang, Y.G., Lee, H.W., et al.; Ultraviolet amplified spontaneous emission from zinc oxide ridge waveguides on silicon substrate; Applied Physics Letter; Nov. 24, 2003; pp. 4288-4290; vol. 83, No. 21; American Institute of Physics.Applicant
- Xiong, G., Wilkinson, J., Lyles, J., Ucer, K.B., and Williams, R.T.; Luminescence and stimulted emission in zinc oxide nanoparticles, films, and crystals.Applicant
- Ong, H.C., Dai, J.Y., and Du, G.T.; Studies of electronic structure of ZnO grain boundary and its proximity by using spatially resolved electron energy loss spectroscopy; Applied Physics Letter; Jul. 8, 2002; pp. 277-279; vol. 81, No. 2; American Institute of Physics.Applicant
- Agne, T., Guan, Z., Li, X.M. Wolf. H., and Wichert, T.; Incorporation of the Donor Indium in Nanocrystalline ZnO; phys. stat. sol.; 2002; pp. 819-823; vol. 229; Wiley-VCH Verlag Berlin GmbH; Berlin.Applicant
- Qadri, S.B., Kim, H., Horwitz, J.S., and Chrisey, D.B.; Transparent conducting films of ZnO-ZrO2: Structure and properties; Journal of Applied Physics; Dec. 1, 2000; pp. 6564-6566; vol. 88, No. 11; American Institute of Physics.Applicant
- Han, J., Mantas, P.Q., and Senos, A.M.R.; Grain growth in Mn-doped ZnO; Journal of the European Ceramic Society; 2000; 2753-2758; vol. 20.Applicant
- Jin, Y., Zhang, B., Yang, S., Wang, Y., Chen, J., et al.; Room temperatue UV emission of MgxZn1-xO films; Solid State Communications; 2001; pp. 409-413; vol. 119; Elsevier Science Ltd.Applicant
- Petrik, N.G., Alexandrov, A.B., and Vall, A.I.; Interfacial Energy Transfer during Gamma Radiolysis of Water on the Surface of ZrO2and Some Other Oxides; J. Phys. Chem. B; 2001; pp. 5935-5944; vol. 105; American Chemical Society.Applicant
- Counio, G., Esnouf, S., Gacoin, T., and Boilot, J.-P.; CdS:Mn Nanocrystals in Transparent Xerogel Matrices; Synthesis and Luminescence Properties; J. Phys. Chem.; 1996; pp. 20021-20026; vol. 100; American Chemical Society.Applicant
- Stravrev, K., Kynev, K., St. Nikolov, G., and Dyakovitch, V.A.; Semiempirical Assignment of the Electron Transitions in Manganese (II)-Doped II-VI Compounds; J. Phys. Chem. Solids; 1987; pp. 841-844; vol. 48, No. 9; Pergamon Journals Ltd.Applicant
- Falcony, C., Ortiz, A., Dominguez, J.M., Farias, M.H., Cota-Araiza, L. et al.; Luminescent Characteristics of Tb Doped Al2O3 Films Deposited by Spray Pyrolysis; J. Electrochem Soc.; Jan. 1992; pp. 267-271; vol. 139, No. 1; The Electrochemical Society, Inc.Applicant
- Bachir, S., Kossanyi, J. Sandouly, C., Valat, P., and Ronfard-Haret, J.C.; Electroluminescence of Dy3+ and Sm3+ Ions in Polycrystalline Semiconducting Zinc Oxide; J. Phys. Chem; 1995; pp. 5674-5679; vol. 99; American Chemical Society.Applicant
- Bachir, S., Kossanyi, J., and Ronfard-Haret, J.C.; Electroluminescence of Ho3+ Ions In a ZnO Varistor-Type Structure; Solid State Communications; 1993; pp. 859-863; vol. 89, No. 10; Elsevier Science Ltd.; Great Britain.Applicant
- Chakrabarti, S., Ganguli, D., Chaudhuri, S., and Pal, A.K.; Crystalline magnesium oxide films on soda lime glass by sol-gel processing; Meterials Letters; May 2002: pp. 120-123; vol. 54; Elsevier Science B.V.Applicant
- Arkles, B.; Commercial Applications of Sol-Gel-Derived Hybrid Materials; MRS Bulletin; May 2001; pp. 402-407.Applicant
- Murray, C.E., Noyan, I.C., and Mooney, P.M.; Mapping of strain fields about thin film structures using x-ray microdiffraction; Applied Physics Letters; Nov. 17, 2003; pp. 4163-4165; vol. 83, No. 20; Amercian Institute of Physics.Applicant
- Modena, S., Soraru, G.D., Blum, Y., and Raj, R.; Passive Oxidation of an Effluent System: The Case of Polymer-Derived SiCO; Journal of the American Ceramic Society; 2005; pp. 339-345; vol. 88.Applicant
- Noyan, I.C., Wang, P.-C., Kaldor, S.K., and Jordan-Sweet, J.L.; Deformation field in single-crystal fields semiconductor substrates caused by metallization features; Applied Physics Letters; Apr. 19, 1999; pp. 2352-2354; vol. 74, No. 16; American Institute of Physics.Applicant
- Noyan, I.C., Jordan-Sweet, J., Liniger, E.G., and Kaldor, S.K.; Characterization of substrate-thin-film interfaces with x-ray microdiffraction; Applied Physics Letters; Jun. 22, 1998; pp. 3338-3340; vol. 72, No. 25; American Institute of Physics.Applicant
- Tuller, H.L.; ZnO Grain Boundaries: Electrical Activity and Diffusion; Journal of Electroceramics; 1999; pp. 33-40; vol. 4:S1; Kluwer Academic Publishers; Boston.Applicant
- Westin, G., Ekstrand, A., Nygren, M., Osterlund, R., and Merkelbach, P.; Preparation of ZnO-based Varistors y the Sol-Gel Technique; J. Mater. Chem.; 1994; pp. 615-621; vol. 4.Applicant
- Wang, M., Yang, X., and Wang., F.; Properties of Sensitive Materials Mainly Composed of ZnO; J. Mater. Sci. Technol.; 2000; p. 204; vol. 16, No. 2.Applicant
- Baptista, J.L., and Mantas, P.Q.; High Temperature Characterization of Electrical Barriers in ZnO Varistors; Journal of Electroceramics; 2000; pp. 215-224; vol. 4:1; Kluwer Academic Publishers; The Netherlands.Applicant
- Brankovic, Z., Brankovic, G., Poleti, D., and Varela, J.A.; Structural and electrical properties of ZnO varistors containing different spinel phases; Ceramics International; 2001; pp. 115-122; vol. 27; Elsevier Science Ltd. And Techna S.r.l.Applicant
- Tanaka, A., and Mukae, K.; Evaluation of Single Grain Boundaries in ZnO: Rare-Earth Varistor by Micro-Electrodes; Key Engineering Materials; 1999; pp. 235-240; vols. 157-158; Trans Tech Publications, Switzerland; CSJ Series-Publications of the Ceramic Society of Japan vol. 1, The Ceramic Society of Japan.Applicant
- Pandey, R., Jaffe, J.E., and Kunz, A.B., Ab initio band-structure calculations for alkaline-earth oxides and sulfides; Physical Review B; Apr. 15, 1991; pp. 9228-9237; vol. 43, No. 11; The American Physical Society.Applicant
- Canney, S.A., Sashin, V.A., Ford, M.J., and Kheifets, A.S.; Electronic band structure of magnesium and magnesium oxide: experiment and theory; J. Phys. Condens. Matter; 1999; pp. 7507-7522; vol. 11; IOP Publishing Ltd.Applicant
- Yamasaki, A., and Fujiwara, T.; Electronic structures of the MO oxides (M=Mg, Ca, Ti, V) in the GW approximation; Physical Review B; 2002; pp. 245108-1-245108-9; vol. 66; The American Physical Society.Applicant
- Mikajlo, E.A., Sashin, V.A., Nixon, K.L., Seoule De Bas, B., Dorsett, H.E., and Ford, M.J.; Band Structures of the Group I and II Oxides: Using EMS Measurements as a Test of Theoretical Models.Applicant
- Johnson, P.D.; Some Optical Properties of MgO in the Vacuum Ultraviolet; Physical Review; May 15, 1954; pp. 845-846; vol. 94, No. 4.Applicant
- Narazaki, A., Tanaka, K., Hirao, K., Hashimoto, T., Nasu, H., et al.; IR and XPS Studies on the Surface Structure of Poled ZnO-TeO2 Glasses wtih Second-Order Nonlinearity; Journal of the American Ceramic Society; 2001; pp. 214-217; vol. 84.Applicant
- Schonberger, U., and Aryasetiawan, F.; Bulk and surface electronic structures of MgO; Physical Review B; Sep. 15, 1995; pp. 8788-8793; vol. 52, No. 12; The American Physical Society.Applicant
- Gonzalez, R., Chen, Y., Sebek. R.M., Williams, G.P., Williams, R.T., et al.; Properties of the 800-nm luminescence band in neutron-irradiated magnesium oxide crystals; Physical Review B; Mar. 1, 1991; pp. 5228-5233; vol. 43, No. 7; The American Physical Society.Applicant
- Balzer, B., Hagemeister, M., Kocher, P., and Ludwig, J.G; Mechanical Strength and Microstructure of Zinc Oxide Varistor Ceramics; Journal of the American Ceramic Society; 2004; pp. 1932-1938; vol. 87.Applicant
- Sheng, H., Emanetoglu, N.W., Muthukumar, S., Yakshinskiy, B.V, Feng, S., et al.; Ta/Au Ohmic Contacts to n—type ZnO; Journal of Electronic Materials; 2003; p. 935; vol. 32, No. 9.Applicant
- Sheng, H., Emanetoglu, N.W., Muthukumar, S., Feng, S., and Lu, L.; Nonalloyed Al Ohmic Contacts to MgxZn12xO; Journal of Electronic Materials; 2002; p. 811; vol. 31, No. 7.Applicant
- Xiong, G., Wilkinson, J., Mischuck, B., Tu Zemen, S., Ucer, K.B., et al; Control of p-and n-type conductivity in sputter deposition of undoped ZnO; Applied Physics Letters; Feb. 18, 2002; p. 1195; vol. 80, No. 7.Applicant
- Yamamoto, T., and Katayama-Yoshida, H.; Unipolarity of ZnO with a wide-band gap and its solution using codoping method; Journal of Crystal Growth; 2000; pp. 552-555; vol. 214/215; Elsevier Science B.V.Applicant
- Chang, R., Marks, T., Mason, T., and Poeppelmeir, K.; n/p-Type Transparent Conductors; pp. 259-260.Applicant
- Olorunyolemi, T., Birnboim, A., Carmel, Y., Wilson, O.C., Lloyd, I.K.; Thermal Conductivity of Zinc Oxide: From Green to Sintered State; Journal of the American Ceramic Society; 2002; pp. 1249-1253; vol. 85.Applicant
- Martin, L.P., and Rosen, M.; Correlation between Surface Area Reduction and Ultrasonic Velocity in Sintered Zinc Oxide Powders; Journal of the American Ceramic Society; 1997; pp. 839-846; vol. 80.Applicant
- Wilkinson, J., Xiong, G., Ucer, K.B., and Williams, R.T.; Lifetime and Oscillator Strength of Excitonic Luminescence in Zinc Oxide.Applicant
- Sekiguchi, T., Haga, K., and Inaba, K.; ZnO films grown under the oxygen-rich condition; Journal of Crystal Growth; 2000; pp. 68-71; vol. 214-215; Elsevier Science B.V.Applicant
- Van De Walle, C.G.; Hydrogen as a Cause of Doping in Zinc Oxide; Physical Reveiw Letters; Jul. 31, 2000; pp. 1012-1015; vol. 85, No. 5; The American Physical Society.Applicant
- Kato, H., Sano, M., Miyamoto, K., and Yao, T.; Effect of O/Zn on Flux Ratio on Crystalline Quality of ZnO Films Grown by Plasma-Assisted Molecular Beam Epitaxy; Japanese Journal of Applied Physics; 2003; pp. 2241-2244; vol. 42; The Japan Society of Applied Physics.Applicant
- Nakahara, K., Tanabe, T., Takasu, H., Fons, P., Iwata, K., et al.; Growth of undoped ZnO Films with Improved Electrical Properties by Radical Source Molecular Beam Epitaxy; Japanese Journal of Applied Physics; 2001; pp. 250-254; vol. 40; The Japan Society of Applied Physics.Applicant
- Wang, X., Du, G., Gu, C., Jia, J., Li, X., et al.; Two-step growth of ZnO thin films on diamond/Si low-pressure metal-organic chemical vapour depositon; J. Phys. D: Appl. Phys.; 2002; pp. L74-L76; vol. 35; IOP Publishing Ltd., United Kingdom.Applicant
- Han, J., Mantas, P.Q., and Senos, A.M.R.; Grain growth in Mn-doped ZnO; Journal of the European Seramic Society; 2000; pp. 2753-2758; vol. 20; Elsevier Science Ltd.Applicant
- Fons, P., Iwata, K., Niki, S., Yamada, A., Matsubara, K., et al.; Uniaxial locked growth of high-quality epitaxial ZnO films on (1 1 2 0)α-A12O3: Journal of Crystal Growth; 2000; pp. 532-536; vol. 209; Elsevier Science B.V.Applicant
- Haga, K., Kamidaira, M., Kashiwaba, Y., Sekiguchi, T., Watanabe, H.; ZnO thin films prepared by remote plasma-enchance CVD method; Journal of Crystal Growth; 2000; pp. 77-80; vol. 214/215; Elsevier Science B.V.Applicant
- Fons, P., Iwata, K., Niki, S., Yamada, A., and Matsubara, K.; Growth of high-quality epitaxial ZnO films on α-A12O3; Journal of Crystal Growth; 1999; pp. 627-632; vol. 201/202; Elsevier Science B.V.Applicant
- Myoung, J-M., Yoon, W-H., Lee, D-H., Yun, I., Bae, S-H., et al.; Effects of Thickness Variation of Properties of ZnO Thin Films Grown by Pulsed Laser Deposition; Japanese Journal of Applied Physics; 2002; pp. 28-31; vol. 41; The Japan Society of Applied Physics.Applicant
- Yuldashev, S.U., Panin, G.N., Choi, S.W., Yalishev, V.S., Nosova, L.A., et al.; Electrical and Optical Properties of ZnO Films Grown on GaAs Substrates; Jpn. J. Appl. Phys; 2003; pp. 3333-3336; vol. 42; The Japan Society of Applied Physics.Applicant
- Nonaka, M., Matsushima, S., Mizuno, M., Kobayashi, K.; Electronic Structure of Group III Elements Doped into ZnO by Using Molecular Orbital Calculation; Chemistry Letters; 2002; pp. 580-581; The Chemical Society of Japan.Applicant
- Lin, G-R., and Wang, S-C.; Comparison of High-Resistivity ZnO Films Sputtered on Different Substrates; Japanese Journal of Applied Physics; 2002; pp. L398-:401; vol. 41; The Japan Society of Applied Physics.Applicant
- Mantas, P.Q., and Baptista, J.L.; The Barrier Height Formation in ZnO Varistors; Journal of the European Ceramic Society; 1995; pp. 605-615; vol. 15; Elsevier Science Limited, Great Britain.Applicant
- Albertsson, J., and Abrahams, S.C.; Atomic Displacement, Anharmonic Thermal Vibration, Expansivity and Pyroelectric Coefficient Thermal Dependences in ZnO; Acta Cryst.; 1989; pp. 34-40; vol. B45; International Union of Crystallography.Applicant
- Blevins, J.D.; Wide Bandgap Semiconductor Substrates: Current Status and Future Trends.Applicant
- Teke, A., Ozgur, U., Dogan, S., Gu, X., Morkoc, H., et al.; Excitonic fine structure and recombination dynamics in single-crystalline ZnO; Physical Review B; 2004; pp. 195207-1-195207-10; vol. 70; the American Physical Society.Applicant
- Look, D.C., Reynolds, D.C., Litton, C.W., Jones, R.L., Eason, D.B., et al.; Characterization of homoepitaxial p-type ZnO grown by molecular beam epitaxy; Applied Physics Letters; Sep. 2, 2002; pp. 1830-1832; vol. 81, No. 10; American Institute of Physics.Applicant
- Kim, K-K., Kim, H-S., Hwang, D-K., Lim, J-H., and Park, S-J.; Realization of p-type ZnO thin films via phosphorus doping and thermal activation of the dopant; Applied Physics Letters; Jul. 7, 2003; pp. 63-65; vol. 83, No. 1; American Institute of Physics.Applicant
- Look, D.C.; Emerging Research Fonts Comments by David C. Look; ISI Essential Science Indicators; Apr. 28, 2005.Applicant
- Senger, R.T., and Bajai, K.K.; Binding energies of excitons in polar quantum well heterostructure; Physical Review B; 2003; pp. 205314-1-205314-9; vol. 68; The American Physical Society.Applicant
- Subramanyam, T.K., Naidu, B., and Uthanna, S.; Structure and Optical Properties of dc Reactive Magnetron Sputtered Zinc Oxide Films; Cryst. Res. Technol.; 1999; pp. 981-988; vol. 34.Applicant
- Muth, J.F. , Brown. J.D., Johnson, M.A.L., Yu, Z., Kolbas, R.M., et al.; Absorption coefficient and refractive index of GaN, AIN and AlGaN alloys; 1999; MRS Internet J. Nitride Semicond.Applicant
- Yoshikawa, H., and Adachi, S.; Optical Constants of ZnO; Japanese Journal of Applied Physics; 1997; pp. 6237-6243; vol. 36.Applicant
- Springer, J., Poruba, A., Vanecek, M., Fay, S., Feitknecht, L., et al.; Improved optical model for thin film silicon solar cells; Presented at the 17th European Photovoltaic Solar Energy Conference, Munich 2001.Applicant
- Neethling, J.H., Scriven, G.J., and Krekels, T.; A TEM investigation of Zn3As2 grown on (001) and (111) InP by MOVPE; Journal of Materials Science; 2001; pp. 3997-4002; vol. 36; Kluwer Academic Publishers.Applicant
- Brink, D.J., and Engelbrecht, A.A.; Ellipsometric investigation of rough zinc arsenide epilayers; Applied Optics; Apr. 1, 2002; pp. 1894-1898; vol. 41, No. 10; Optical Society of America.Applicant
- Scriven, G.J., Leitch, A.W.R., Neethling, J.H., Kozyrkov, V.V., and Watters, V.J.; The growth of Zn3As2 on InP by atmospheric pressure MOVPE; Journal of Crystal Growth; 1997; pp. 813-816; vol. 170; Elsevier Science B.V.Applicant
- Engelbrecht, J.A.A., Scriven, G.J., Neethling, J.H., and Wagener, M.C.; Crack formation in Zn3As2 epilayers grown by MOVPE; Journal of Crystal Growth; 2000; pp. 235-244; vol. 216; Elsevier Science B.V.Applicant
- Norman, A.G., Olson, J.M., Romero, M.J., and Al-Jassim, M.M.; Electron Microscopy Studies of Potential 1-eV Bandgap Semiconductor Compounds AnGeAs2 and Zn3As2 Grown by MOVPE; National Renewable Energy Laboratory.Applicant
- Miles, G.C., and West, A.R.; Polymorphism and Thermodynamic Stability of Zn7Ab2O12; Journal of the American Ceramic Society; 2005; pp. 396-398; vol. 88.Applicant
- Tomlins, G.W., Routbort, J.L., and Mason, T.O.; Oxygen Diffusion in Single-Crystal Zinc Oxide; Journal of the American Ceramic Society; 1998; pp. 869-876; vol. 81.Applicant
- Botha, J.R., Scriven, G.J., Engelbrecth, J.A.A., and Leitch, A.W.R.; Photoluminescence properties of metalorganic vapor phase epitaxial Zn3As2; Journal of Applied Physics; Nov. 15, 1999; pp. 5614-5618; vol. 86, No. 10; American Institute of Physics.Applicant
- Xiong, G., Wilkinson, J., Mischuck, B., Tuzemen, S., Ucer, K.B., et al.; Control of p-and n-type conductivity in sputter depositon of undoped ZnO; Applied Physics Letters; Feb. 18, 2002; pp. 1195-1197; vol. 80, No. 7; American Institute of Physics.Applicant
- Look, D.C., Renlund, G.M., Burgener, II, R.H., and Sizelove, J.R.; As-doped p-type ZnO produced by an evaporation/sputtering process; Applied Physics Letters; Nov. 2004; vol. 85.Applicant
- Aoki, T., Shimizu, Y., Miyake, A., Nakamura, A., Nakanishi, Y., and Hatanaka, Y.; p-type ZnO Layer Formation by Excimer Laser Doping; phys. stat. sol.; 2002; pp. 911-914; vol. 229, No. 2; Wiley-VCh Verlag Berling GmbH, Berlin.Applicant
- Lee, J-M., Kim, K.K., Park, S-J., and Choi, W.K.; Low-resistance and non-alloyed ohmic contacts to plasma treated ZnO; Applied Physics Letters; Jun. 11, 2001; pp. 3842-2844; vol. 78, No. 24; American Institute of Physics.Applicant
- Yamamoto, T.; Codoping Method to Realize Low-Resistivity p-type ZnO Thin Films; Asia Display/IDW '01, Oct. 16-19, 2002, Nagoya, Oct. 18, PH1-2.Applicant
- Wang, L.G., and Zunger, A.; Cluster-Doping Appraoch for Wide-Gap Semiconductors: The Case of p-type ZnO; Physical Review Letters; Jun. 27, 2003; pp. 256401-1-256401-4; vol. 90, No. 25; The American Physical Society.Applicant
- Nakahara, K., Takasu, H., Fons, P., Yamada, A., Iwata, K., et al.; Growth of N-doped and Ga+N-codoped ZnO films by radical source molecular beam epitaxy; Journal of Crystal Growth; 2002; pp. 503-508; vol. 237-239; Elsevier Science B.V.Applicant
- Recnik, A., Daneu, N., Walther, T., and Mader, W.; Structure and Chemistry of Basal-Plane Inversion Boundaries in Antimony Oxide-Doped Zinc Oxide; Journal of the American Ceramic Society; 2001; pp. 2357-2668; vol. 84.Applicant
- Nonaka, M., Matsushima, S., Mizuno, M., and Kobayashi, K.; Electronic Structure of Group III Elements Doped into ZnO by Using Molecular Orbital Calculation; Chemistry Letters; 2002; pp. 580-581; The Chemical Society of Japan.Applicant
- Ryu, Y.R., Kim, W.J., and White, H.W.; Fabrication of homostructural ZnO p-n junctions; Journal of Crystal Growth; 2000; pp. 419-422; vol. 219; Elsevier Science B.V.Applicant
- Lu, J., Ye, Z., Wang, L., Huang, J., and Zhao, B.; Structural, electrical optical properties of N-doped ZnO films synthesized by SS-CVD; Materials Science in Semiconductor Processing; 2003; pp. 491-496; vol. 5; Elsevier Science Ltd.Applicant
- Zhenguo, J., Kun, L., Chengxing, Y., Ruixin, F., and Zhizhen, Y.; Structural, optical and electrical properties of ZnO thin films prepared by reactive deposition; Journal of Crystal Growth; 2003; pp. 246-251; vol. 253; Elsevier Science B.V.Applicant
- Ji, Z., Yang, C., Liu, K., and Ye, Z.; Fabrication and characterization of p-type ZnO films by pyrolysis of zinc-acetate—ammonia solution; Journal of Crystal Growth; 2003; pp. 239-242; vol. 253; Elsevier Science B.V.Applicant
- Ye, Z-Z., Lu, J-G., Chen, H-H., Zhang, Y-Z., Wang, L., et al.; Preparation and characteristics of p-type ZnO films by DC reactive magnetron sputtering; Journal of Crystal Growth; 2003; pp. 258-264; vol. 253; Elsevier Science B.V.Applicant
- Minegishi, K., Koiwai, Y., Kikuchi, Y., Yano, K., Kasuga, M., et al.; Growth of p-type Zinc Oxide Films by Chemical Vapor Deposition; Japanese Journal of Applied Physics; 1997; pp. L 1453-L 1455; vol. 36.Applicant
- Joseph, M., Tabata, H., and Kawai, T.; p-type Electrical Conduction in ZnO Thin Films by Ga and N Codoping; Japanese Journal of Applied Physics; 1999; pp. L 1205-L 1207; vol. 38; Publication Board, Japanese Journal of Applied Physics.Applicant
- Ashrafi, A.B.M.A., Suemune, I., Kumano, H., and Tanaka, S.; Nitrogen-Doped p-Type ZnO Layers Prepared with H2O Vapor-Assisted Metalorganic Molecular-Beam Epitaxy; Japanese Journal of Applied Physics; 2002; pp. L 1281-L 1284; vol. 41; The Japan Society of Applied Physics.Applicant
- The Promise of Solid State Lighting for General Illumination: Light Emitting Diodes (LEDs) and Organic Light Emitting Diodes (OLEDs); 2001; pp. 1-29; Optoelectronics Industry Development Association, Washington, D.C.Applicant
- Talbot, D.; LEDs vs. the Light Bulb; Technology Review; May 2003; pp. 30-36.Applicant
- Johnson, S.; LEDs—An Overview of the State of The Art in Technology and Application; Light Right 5 Conference, May 27-31, 2002, Nice, France.Applicant
- Tuzemen, S., Xiong, G., Wilkinson, J., Mischick, B., Ucer, K.B., et al.; Production and properties of p-n junctions in reactively sputtered ZnO; Physica B; 2001; pp. 1197-1200; vol. 308-310; Elsevier Science B.V.Applicant
- Guo, X-L., Choi, J-H., Tabata, H., and Kawai, T.; Fabrication and Optoelectronic Properties of a Transparent ZnO Homostructural Light-Emitting Diode; Japanese Journal of Applied Physics; 2001; pp. L 177-L 180; vol. 40; The Japan Society of Applied Physics.Applicant
- Xiong, G., Wilkinson, J., Tuzemen, S., Ucer, K.B., and Williams, R.T.; Toward a new ultraviolet diode laser: luminescence and p-n junctions in ZnO films.Applicant
- Hoffman, R.L., Norris, B.J., and Wager, J.F.; ZnO-based transparent thin-film transistors; Applied Physics Letters; Feb. 3, 2003; pp. 733-735; vol. 82, No. 5; American Insistute of Physics.Applicant
- Bockowshi, M.; Growth and Doping of GaN and AIN Single Crystals under High Nitrogen Pressure; Cryst. Res. Technol.; 2001; pp. 771-787; vol. 36; Wiley-VCH Verlag Berlin GmbH, Berlin.Applicant
- Katayama-Yoshida, H., Sato, K., and Yamamoto, T.; Materials design for new functional semiconductors by ab initio electronic structure calculation: Prediction vs. experiment; JSAP International; Jul. 2006; pp. 20-27; No. 6.Applicant
- Mukai, T., Morita, D., and Nakamura, S.; High-power UV InGaN/AlGaN double-heterostructure LEDs; Journal of Crystal Growth; 1998; pp. 778-781; vol. 189/190; Elsevier Science B.V.Applicant
- Xing, H., Green, D.S., McCarthy , L., Smorchkova, I.P., Chavarkar, P., et al.; Progress in Gallium Nitride-based Bipolar Transistors.Applicant
- Piprek, J., and Nakamura, S.; nano-Scale Effects in GaN-based Light-Emitting Diodes; 2004.Applicant
- Piprek, J.; Simulation of GaN-based Light-Emitting Devices; 2004.Applicant
- Bunea, G.E., Herzog, W.D., Unlu, M.S., Goldberg, B.B., and Molnar, R.J.; Time-resolved photoluminescence studies of free and donor-bound exciton in GaN grown by hydride vapor phase epitaxy.Applicant
- Yao, T.; Plasma-Assisted MBE Growth of ZnO; Molecular Beam Epitaxy; pp. 98-105.Applicant
- Chapter 2 Geometric Structure of Metal Oxides; pp. 55-58.Applicant
- Chapter 4 Electronic Structure of Non-Transition-Metal-Oxide Surfaces; pp. 143-150.Applicant
- IP, K., Khanna, R., Norton, D.P., Pearton, S.J., Ren, F., et al.; Thermal Stability of Tungsten-Based Schottky Contacts to N-Type ZnO.Applicant