Patent Grant
10685758
The present invention relates to semiconductor structures for use in radiation-heavy environments, and more particularly to three dimensional radioisotope semiconductor structures and methods of making the same.
Batteries typically comprise one or a connected set of similar units or cells acting as an electrical energy source. Most batteries operate by converting chemical energy directly into electrical energy. However, while chemical batteries are typically inexpensive to produce and may supply a reasonably high energy output, they may not be compatible with, for example, microelectronic devices due to size and durational requirements.
Other batteries generally referred to as nuclear or radioisotope batteries have been developed, which directly or indirectly convert radioactive energy released during the decay of a radioactive source into electrical energy. For instance, in some radioisotope batteries, a radioactive source emits nuclear radiation, e.g. alpha or beta particles, which produces electron-hole pairs within a planar semiconductor material. The movement of these charges over times results in an electronic current, which when connected to a load resistor operates as a source of power. However, such conventional planar radioisotope batteries often suffer efficiency, flexibility, scalability and low output power in the microwatt range.
Moreover, such batteries are susceptible to radiation-induced damage which, over time, reduces the efficiency and output of the battery.
According to one embodiment, a product includes an array of three dimensional structures, a cavity region between each of the three dimensional structures, and a first material in contact with at least one surface of each of the three dimensional structures. In addition, each of the three dimensional structures includes a semiconductor material, where at least one dimension of each of the three dimensional structures is in a range of about 0.5 microns to about 10 microns. Moreover, the first material is configured to provide high energy particle and/or ray emissions.
According to another embodiment, a product includes an array of three dimensional structures, a cavity region between each of the three dimensional structures, and a first material in contact with at least one surface of each of the three dimensional structures. In addition, at least one dimension of each of the three dimensional structures is in a range of about 0.01 microns to less than about 0.5 microns. Moreover, the first material is configured to provide high energy particle and/or ray emissions.
According to yet another embodiment, a product includes an array of three dimensional structures and a cavity region between each of the three dimensional structures. In addition, each of the three dimensional structures comprises a semiconductor material. Moreover, each of the three dimensional structures has at least one dimension that enables migration (e.g., drift and/or diffusion) of radiation-induced damage to a surface of the respective three dimensional structure at a rate that is at least 90% of a rate of the radiation-induced damage.
Other aspects and embodiments of the present invention will become apparent from the following detailed description, which, when taken in conjunction with the drawings, illustrate by way of example the principles of the invention.
For a fuller understanding of the nature and advantages of the present invention, reference should be made to the following detailed description read in conjunction with the accompanying drawings.
The following description is made for the purpose of illustrating the general principles of the present invention and is not meant to limit the inventive concepts claimed herein. Further, particular features described herein can be used in combination with other described features in each of the various possible combinations and permutations.
Unless otherwise specifically defined herein, all terms are to be given their broadest possible interpretation including meanings implied from the specification as well as meanings understood by those skilled in the art and/or as defined in dictionaries, treatises, etc.
It must also be noted that, as used in the specification and the appended claims, the singular forms “a,” “an” and “the” include plural referents unless otherwise specified.
As also used herein, the term “about” denotes an interval of accuracy that ensures the technical effect of the feature in question. In various approaches, the term “about” when combined with a value, refers to plus and minus 10% of the reference value. For example, a thickness of about 10 nm refers to a thickness of 10 nm±1 nm, a temperature of about 50° C. refers to a temperature of 50° C.±5° C., etc.
The following description discloses several embodiments of high efficiency three dimensional semiconductor structures, preferably having radioactive materials deposited thereon, and/or related systems and methods.
In one general embodiment, a product includes an array of three dimensional structures, a cavity region between each of the three dimensional structures, and a first material in contact with at least one surface of each of the three dimensional structures. In addition, each of the three dimensional structures includes a semiconductor material, where at least one dimension of each of the three dimensional structures is in a range of about 0.5 microns to about 10 microns. Moreover, the first material is configured to provide high energy particle and/or ray emissions.
In another general embodiment, a product includes an array of three dimensional structures, a cavity region between each of the three dimensional structures, and a first material in contact with at least one surface of each of the three dimensional structures. In addition, at least one dimension of each of the three dimensional structures is in a range of about 0.01 microns to less than about 0.5 microns. Moreover, the first material is configured to provide high energy particle and/or ray emissions.
In yet another general embodiment, a product includes an array of three dimensional structures and a cavity region between each of the three dimensional structures. In addition, each of the three dimensional structures comprises a semiconductor material. Moreover, each of the three dimensional structures has at least one dimension that enables migration (e.g., drift and/or diffusion) of radiation-induced damage to a surface of the respective three dimensional structure at a rate that is at least 90% of a rate of the radiation-induced damage.
Referring now to
As shown in
With continued reference to
In yet other approaches, the three dimensional structures 102 may include pillar structures with cavity regions 104 therebetween. U.S. patent application Ser. No. 13/742,298, filed Jan. 15, 2013, describes three dimensional pillar structures and methods of making the same, which may be adapted for use in various embodiments disclosed herein, and is incorporated herein by reference.
In more approaches, the three dimensional structures 102 may include ridge structures with cavity regions 104 therebetween. Of course, other three dimensional structures recognized by one skilled in the art upon reading the present disclosure may be used.
In yet more approaches, the three dimensional structures 102 may be arranged in the array such that a separation between each of the three dimensional structures 102 is about uniform. For instance, in one particular approach, the array of three dimensional structures 102 may be arranged in a hexagonally close packed (HCP) array.
It is important to note that the inventors found, much to their surprise, that three dimensional structures with an alpha-emitter radioisotope generated better electronic performance in terms of output power compared to two dimensional structures, e.g., flat or unetched surfaces, with similar or the same alpha-emitting radioisotopes. Thus, the three dimensional structure of semiconductor material may provide radiation hardness to the structure, where radiation hardness may be defined as the ability for a semiconductor to continually maintain output power without a significant rate of reduction of the output power due to radiation-induced damage.
In additional approaches, each of the three dimensional structures 102 may have a width, w, of about 0.5 to about 500 μm and/or a height, h, of about 1 to about 1000 μm, e.g., about 4 μm, about 10 μm, about 12 μm, about 20 μm, about 50 μm, about 500 μm, about 900 μm, etc., up to approaching the thickness of the host substrate. In some embodiments, at least one dimension of each of the three dimensional structures is in a range of about 0.5 microns to about 10 microns. Preferably, this is an average dimension measured perpendicular to a longitudinal axis of the respective three dimensional structure.
In further embodiments, at least one dimension of each of the three dimensional structures 102 may be in a range of about 0.01 μm to less than about 0.5 μm, for example, less than 0.45 μm. Preferably, this is an average dimension measured perpendicular to a longitudinal axis of the respective three dimensional structure.
In another approach, at least one dimension is in a range of about 0.01 microns to about 100 microns. Preferably, this is an average dimension measured perpendicular to a longitudinal axis of the respective three dimensional structure. A more preferred range is from about 0.01 microns to about 2 microns.
Moreover, in numerous approaches, the separation, s, between adjacent three dimensional structures 102 may be in a range from about 1 μm to about 10 μm, and/or the center-to-center spacing (i.e. the pitch, p) between the three dimensional structures 102 may be in a range from about 2 to about 10 μm. Further, in more approaches, each of the three dimensional structures 102 may have an aspect ratio of less than or equal to about 100:1, where the aspect ratio corresponds to the ratio of the height of a three dimensional structure relative to its width and/or pitch. It is important to note, however, that said dimensions (diameter, pitch, height, aspect ratio, etc.) serve only as an example and are not limiting in any way, such that various embodiments may have larger or smaller dimensions.
According to yet more approaches, a width, height aspect ratio and/or semiconductor material(s) of the three dimensional structures 102 may be selected/determined by an alpha or beta particle range (e.g. the range at which the alpha and beta particles are stopped in the structures). In specific embodiments, the width of the three dimensional structures 102 may be about twice this alpha and/or beta particle range. For example, the width of the three dimensional structures 102 may be about 10 to about 100 microns, in various embodiments. According to further approaches, the dimensions (e.g. the width, aspect ratio, height, etc.) and/or composition of the three dimensional structures 102 may be selected to spread out radiation damage over a wider area to mitigate the damage.
According to still more approaches, a height of the three dimensional structures 102 may be selected to maximize the output power of the product 100. The output power of the product 100 may be about equal to or greater than about 1 W, about 10 W and about 100 W, in various embodiments. Moreover, in approaches where the three dimensional structures 102 include a semiconductor material, as discussed below, the large volume of the three dimensional semiconductor structures may dramatically increase power density instead of limiting said power density to the surface as in planar semiconductor designs that only provide microwatt power.
In various embodiments, as shown in
Radiation-induced damage in semiconductors is typically caused by the collision of an energetic particle or photon with an atom. This may result in the atom being displaced to an interstitial position or electronic charge displacement. The damage may be a radiation-induced defect within the semiconductor material. Without wishing to be bound by any theory, the inventors believe the dimensions of the three dimensional structure prevent the radiation-induced damage from becoming immobile (e.g. trapped, set, etc.) as may be seen in two dimensional structures. In three dimensional structures, the radiation-induced damage may migrate to the surface of semiconductor material thereby leaving the semiconductor material essentially intact. Radiation-induced damage may become immobile if the distance to the surface of the structure is greater than the distance that the radiation-induced damage can migrate. Furthermore, if a radiation-induced defect remains long enough, it may combine with another radiation-induced defect thereby becoming immobile.
In some approaches, the dimension of the three dimensional structure may enable drift of radiation-induced damage to the surface of the respective three dimensional structure. In other approaches, the dimension of the three dimensional structure may enable diffusion of radiation-induced damage to the surface of the respective three dimensional structure. In yet other approaches, the dimension of the three dimensional structure may enable both drift and diffusion of radiation-induced damage to the surface of the respective three dimensional structure.
In some embodiments, at least one dimension of each three dimensional structure may enable mitigation of radiation-induced damage at a rate that is at least 90% of a rate of the radiation-induced damage from the high energy particle and/or ray emissions from the first material. In some approaches, the rate of mitigation, e.g., migration, of radiation-induced damage may be dependent on heat generated during radiation-induced damage. In other approaches, the rate of mitigation of radiation-induced damage may be induced by similar factors that induce migration of radiation-induced damage.
Comparisons of the rate of mitigation of the radiation-induced damage to the rate of radiation-induced damage that occurs upon exposure of the three dimensional structures to high energy particle and/or beta emissions from a radiation source have shown the extent of self-healing by the structures disclosed herein having at least one dimension smaller than about 100 microns. Such dimension enables a rate of mitigation, e.g., migration, of radiation-induced damage to be about equal to, and often greater than, the rate of radiation-induced damage incurred during the intended use of the three dimensional structures, thereby essentially remediating the effects of any radiation-induced damage to the semiconductor material of the three dimensional structure.
Various factors may affect the rate of migration of radiation-induced damage in the semiconductor material. During irradiation of the semiconductor material, low-temperature repairs may help facilitate the movement of radiation-induced damage. Electron-hole recombination may effectively move the radiation-induced damage toward the surface of the semiconductor material.
In a preferred approach, each of the three dimensional structures 102 may include one or more semiconductor materials. According to some embodiments, the one or more semiconductor materials may include, but are not limited to, silicon, gallium arsenide, SiC, GaN, and indium phosphide. SiC and/or GaN may be of particular interest for use in the three dimensional structures 102 due to their high atomic displacement energies (>20 eV) compared to Si (>13 eV), as well as their wide band gap, making them suitable for operation at high temperatures.
In other embodiments the one or more semiconductor materials may include crystalline materials (e.g. single crystal silicon); amorphous materials (e.g. amorphous silicon, a-Si). In embodiments where the semiconductor material is a-Si, which is radiation hard because of the lack of crystallinity, disruptions in the crystalline lattice due to atomic displacements may not be as problematic. In yet other embodiments, the one or more semiconductor of materials may be selected to include crystalline materials or amorphous materials based on a desired radiation damage resistance.
In more embodiments, the semiconductor material(s) may include one or more icosahedral borides, such as icosahedral boron arsenide (B12As2) and icosahedral boron phosphide (B12P2), which may be particularly advantageous due to their resistance to radiation damage.
In yet more embodiments, the semiconductor material(s) may be a self-healing material (e.g. a material configured to mitigate and/or reverse radiation damage). Semiconductor material that is self healing may show increased rates of mitigation e.g., migration, of radiation-induced damage. Such semiconductor materials may have electron and/or interstitial latency diffusion properties that promote an increased rate of migration of radiation-induced damage. Various material properties such as conductivity type (e.g. n-type or p-type) and/or the presence of minority charge carriers (e.g. electrons in p-type material) may influence or enhance the migration of defects in the material. For example, the charge carriers present in a p-type (or n-type) semiconductor material may cause radiation-induced damage to be more mobile and thus more likely to migrate to the surface of semiconductor material of p-type (or n-type) conductivity.
In further approaches, the semiconductor material(s) of the three dimensional structures 102 may have a p-type conductivity region and an n-type conductivity region with a p-n junction therebetween. Other approaches include using heterojunctions to create band offsets for diode formation. In particular embodiments, the n-type and p-type regions may be electrically connected to a load circuit. For example, in one embodiment, the array of three dimensional structures 102 comprising the one or more semiconductor materials may be positioned above a formed on a substrate (not shown in
As also shown in
In another approach, the first material 106 may comprise a radioisotope. This radioisotope may be selected based on a decay type and/or a decay energy, in some embodiments. For example, in one particular embodiment, the radioisotope may be an alpha particle emitter including, but not limited to, 148Gd, 241Am, and 238Pu. In another embodiment, the radioisotope, may be a beta particle emitter including, but not limited to, 63Ni and 106Ru. In yet another embodiment, the selected radioisotope may be an alpha particle emitter because alpha particle emitters such as 148Gd and 238Pu may have a higher output power than beta particle emitters such as 63Ni and 106Ru. A higher activity may lead to a short expected lifetime of the device due to damage within the three dimensional structures comprising a semiconductor material.
In a further embodiment, the radioisotope may be 233U. In an additional embodiment, the radioisotope may be 232U, which emits a 5 MeV alpha particle with a weak emission of a low energy gamma-ray (57 keV). Use of 232U as the radioisotope may be advantageous due to its decay properties and half-life of 70 years. The half-life of 232U may be suitably long enough for a battery yet short enough to obtain the specific activity required for current generation.
In various embodiments, the radioisotope included in the first material 106 may undergo spontaneous decays in the form of both short-range alpha and beta particles along with much longer range gamma-rays. In such embodiments, self-capture may occur within the product 100 itself and shielding, using various metals, may completely contain the radiation for safe handling.
The radioisotope included in the first material 106 may lose energy by both spontaneous decays and also by heat dissipation. The heat may be mitigated by heat sinks such as liquid coolants, in more embodiments. The heat of the radioisotope may also be used as an in-situ anneal in order to repair damage as it is created, extending the life of the product 100 in still more embodiments.
Behavior and migration of radiation-induced damage from high energy particles and/or ray emissions from the first material may depend on properties of the particles and/or ray emissions. For example, but not wishing to be bound by any theory, the inventors believe that an alpha particle may have the same flux rate as all the particles and more interstitial latency will change the local concentration, which may change the diffusion max by forming a stable complex of particles. Alpha particles may induce damage that is localized closer to other particles whereas beta ray emissions may induce damage that is farther apart in the semiconductor material. Thus, migration of radiation-induced damage may be influenced by the type of high energy particle and/or ray emissions of the first, second, or additional material.
In various embodiments, a first material 106 may be positioned to provide high energy particle and/or ray emissions to the three dimensional structures 102. The first material 106 may be in direct contact with the three dimensional structures 102, or spaced therefrom in various embodiments.
In some approaches, the first material 106 may include more than one radioisotope. For example, in one embodiment, the first material 106 may include two or more layers 602, 604 as shown in
In various approaches, the first material 106 may have a thickness selected to facilitate electron-hole charge carrier generation. In particular approaches, the first material 106 may have a thickness, t, of between about 50 to about 500 microns.
In other embodiments, the first material 106 may cover the tops of the three dimensional structures 102 and/or completely fill the cavity regions 104. In yet other embodiments, the cavity regions 104 may be under-filled, such that the first material 106 may only partially fill the cavity regions 104. For example, in approaches where the cavity regions 104 may be under-filled, the first material 106 may only fill a percentage, ranging from about 25% to about 99.5%, of the volume of the cavity regions 104.
With continued reference to
In more approaches, one or more additional materials (e.g. a second, third, fourth, fifth, sixth, etc. material) may coat and/or be deposited above the three dimensional structures 102 and/or the first material 106. In particular embodiments, the one or more additional materials may form a layer that is deposited directly on the first material 106. In other embodiments, the one or more additional materials may form a plurality of layers that are deposited above the first material 106. In further embodiments, these one or more additional materials may be stacked in such a manner as to build up to a large “sugar cube” size.
In more embodiments, at least one of the one or more additional materials may have a composition and/or one or more components therein that is/are the same or different than the first material 106. In yet more embodiments, at least one of the one or more additional material may comprise radioisotope(s) that may be different or the same from radioisotope(s) included in the first material 106. In some approaches, each of the one or more additional materials may comprise radioisotope(s), some or all of which may be the same or different from one another. For instance, in particular approaches, the radioisotopes included within the first material and/or each of the one or more additional materials may be independently selected from a group consisting of: 148Gd, 238Pu, 244Cm, 243Am, 241Am, 63Ni, 106Ru, 232U, 0.90Sr, and 0.147Pm.
As also shown in
In some approaches, the product 100 may include two or more separate arrays of three dimensional structures 102. In various embodiments, these two or more separate arrays may be stacked; electrically connected in series and/or parallel; etc. Any type of busing may be used to create the electrical interconnections.
In yet more approaches, the product 100 may be modular in order to locate required power and/or heat in multiple locations within a system to optimize performance. In such approaches, the performance may not rely on the entire radioactivity to be located in one place.
Referring now to
As shown in
In other approaches, formation of the three dimensional structures may include providing a host substrate (e.g. glass or other suitable support material) having a mold for three dimensional definition, and subsequently depositing a semiconductor material on the mold (e.g. via direct writing or depositing of materials by solution, vacuum deposition methods, etc.). These particular approaches may provide an inexpensive route to form very high aspect ratio three dimensional structures.
In preferred approaches, each of the three dimensional structures may include at least one electrically conductive and/or semiconductor material. However, in other approaches where the three dimensional structures may not include an electrically conductive and/or semiconductor material, a supplemental layer of electrically conductive and/or semiconductor material may be deposited directly on the three dimensional structures.
As also shown in
This first material may be applied via electrochemical deposition (electroplating), chemical vapor deposition, sputtering, spin coating, electrophoretic deposition, solution-based approaches (e.g. where a solution including radioactive nanoparticles may be applied to the surface to be coated and subsequently removed via evaporation to leave a coating of radioactive nanoparticles), and other suitable deposition techniques as would be understood by one having skill in the art upon reading the present disclosure. In more approaches, the first material may be dispersed throughout a polymer, and then deposited on the three dimensional structures. In even more approaches, the first material may be coated on a much smaller host material (e.g. polymeric, dielectric, semiconductor or metal spheres, etc.), and then deposited onto at least one surface of the three dimensional structures.
In further approaches, the first material may include one or more metals which may be subject to neutron activation. For example, in one embodiment, the method 400 may include applying a coating of Ni to at least one surface of the three dimensional structures, and then neutron activating the Ni to create the Ni radioisotope, 63Ni. Such an embodiment may be advantageous as it will be easier to complete the metal connection to the three dimensional structures.
In additional embodiments, the method 400 may also include applying one or more additional materials above the first material. In preferred approaches, each of these one or more materials may be configured to provide high energy particles and/or ray emissions. These additional materials may be applied via any of the deposition techniques disclosed herein and/or any other suitable deposition techniques as would be understood by one having skill in the art upon reading the present disclosure. The one or more additional materials may each comprise at least one radioisotope, which may the same or different as a radioisotope present in the first material.
In yet more embodiments, the method 400 may include depositing a functional and/or support material below and/or above the array of three dimensional structures. As an example, this functional material may be metallic to form electrical contacts, which may be connected to a load circuit.
As discussed in greater detail below, the three dimensional structures disclosed herein, which preferably include one or more semiconductor materials, may suffer radiation damage. Accordingly, in some approaches, the method 400 may involve thermal annealing the three dimensional structures to anneal out some, the majority or substantially all of the radiation damage.
As also discussed below, the heat generated by the first material, which serves as the radiation source and is positioned on at least one surface of the three dimensional structures, may mitigate the radiation damage to the three dimensional structures. Accordingly, the method 400 may include selecting the composition and/or other physical parameters (e.g. carrier type, carrier concentration, thickness, density, quantity of alpha and/or beta emitters, radiation intensity therein) of the first material (and the one or more additional materials where appropriate) to optimize this self-healing process. In some approaches, varying temperatures may affect radiation-induced damage that occurs upon exposure of the three dimensional structures to radiation such as high energy particle and/or ray emissions from the first material, second material, and/or additional material.
Referring now to
As shown in
As also shown in
Method 700 may have any of the features described for all the embodiments (for example, method 400) as described above.
Measuring and/or Mitigating Radiation Damage
In various approaches, the three dimensional structures disclosed herein, which preferably include one or more semiconductor materials, may suffer radiation damage. Radiation damage in semiconductors is typically caused by the collision of an energetic particle or photon with an atom. This may result in the atom being displaced to an interstitial position or electronic charge displacement. The damage site may limit the charge carrier generation and collection.
The radiation damage associated with the three dimensional structures disclosed herein may be studied via current-voltage measurements utilizing, for example, a Parameter Analyzer in some embodiments. For measurements involving three dimensional structures without a radioactive material thereon (e.g. the first material 106 of
However, for measurements involving three dimensional structures with a radioactive material deposited thereon, the radiation source may be said radioactive material. For example, in one embodiment, the radioactive material may include microcurie to kilocurie deposits of alpha emitters, and the extent of the radiation damage to the three dimensional structure may be measured by monitoring the electrical output as a function of time. It has been found in some embodiments, that visible damage to the three dimensional structures may occur with a dose of 1×1018 alphas/cm2. However in other embodiments, a determination of the impact of radiation damage on that current production may be accomplished with lower alpha deposits.
Moreover, it has also been found in various approaches that while the radioactive material may serve as the radiation source, the heat generated by the radioactive material may nevertheless mitigate the radiation damage to the three dimensional structures. Stated another way, the heat generated by the radioactive material may be used as an in-situ anneal in order to repair damage as it is created, extending the life of the three dimensional structures, as well as any device encapsulating said structures. The required temperature for this self-annealing may depend on several factors: radiation type, dose, energy, and the semiconductor material. For example, temperatures as low as 340 K may be effective for annealing radiation damage in a-Si and 448 K for annealing damage in SiC. For example, temperatures as low as 340 K may be effective for annealing radiation damage in a-Si and 448 K for annealing damage in SiC.
Further, it has been found in more approaches that damage and/or degradation of the three dimensional structures including one or more semiconductor and/or electrically conductive materials may occur at elevated temperatures, due to intrinsic properties of said material(s), as well as the external processing conditions. As the carrier concentration of a semiconductor is related to both the material's band gap and the operating temperature, wide band gap materials such as SiC (3.3 eV) and GaN (3.4 eV) may offer potentially superior operation at elevated temperatures compared to Si (1.1 eV).
Another possible degradation route may involve inter-diffusion between the metals and the semiconductors, which may occur at elevated temperatures over long periods. Accordingly, the use of refractory metals and compounds in various approaches may prevent this.
In one particular embodiment, the radiation damage associated with a 1 cm3 U3O8—Si radioisotope battery was analyzed.
An output power as a function of time for the U3O8—Si radioisotope battery may reach 50% of its original output power (>100 mW/cm3) after 6 years. Accordingly, to form a 100 W, 1000 cm3 battery, which may be built with a compact 10 cm×10 cm×10 cm array, 45 KCi of 232U may be used, which is about twice the length of a Rubix cube. It is important to note, that this configuration may generate a significant amount of heat. However, annealing effects due to heat deposited in the three dimensional semiconductor structures may benefit such a battery. Additionally, these self-annealing processes may be increased by designing a thermal management system to operate at an optimum temperature. Designing such a thermal management system may include selecting a particular radiation source (e.g. radioisotope), which may operate at a temperature to optimize the self-annealing process.
Degradation of a Two Dimensional Structure Compared to Degradation of a Three Dimensional Structure
Demonstrations with the semiconductor Si showed no degradation in generated power after an alpha radiation using 210Po up to a dose of >1e10 cm-2 for a three dimensional structure, whereas a two dimensional structure has shown degradation of >40% in output power under similar conditions.
Three dimensional structured Si diodes showed improved radiation hardness to alpha irradiation compared to two dimensional structured diodes. Later testing showed improved characteristics with no power degradation observed to >4e10 cm-2 dose (two dimensional diodes showed 10% degradation after 1e9 cm-2 dose).
Uses
Embodiments of the present invention may be used in a wide variety of applications, particularly those applications which utilize power generation devices.
For instance, embodiments of the present invention may be useful in high radiation fields such as nuclear reactors, space, spent fuel, etc.
In addition, embodiments of the present invention may be useful as betavoltaic, alphavoltaic, radioisotope battery, radioisotope thermal generator, thermoelectric, sensors, electronics, electronics for harsh environments, radiation hard electronics, nuclear fuel monitoring, and radiation tolerant materials.
Moreover, embodiments of the presents invention may be useful as small nuclear batteries. Small nuclear batteries from micro watts to 100 W have a wide variety of commercial and government applications. This technology, depending on the application and power, will make the batteries an off the shelf power supply enabling the long term use of micro-powered devices and sensors capable of uninterrupted operation from years to as long as exceeding decades.
In addition, embodiments of the present invention may be useful as higher power devices, which may enable deep space probes to operate with a lower size and weight budget than conventional nuclear power supplies.
Accordingly, embodiments of the present invention thus have applications in the defense, international communities, space and other communities.
Any of the structures, methods, etc. described above, taken individually or in combination, in whole or in part, may be included in or used to make one or more systems, devices, etc. In addition, any of the features presented herein may be combined in any combination to create various embodiments, any of which fall within the scope of the present invention.
Moreover, while various embodiments have been described above, it should be understood that they have been presented by way of example only, and not limitation. Thus, the breadth and scope of a preferred embodiment should not be limited by any of the above-described exemplary embodiments, but should be defined only in accordance with the following claims and their equivalents.
The United States Government has rights in this invention pursuant to Contract No. DE-AC52-07NA27344 between the United States Department of Energy and Lawrence Livermore National Security, LLC for the operation of Lawrence Livermore National Laboratory.
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| Number | Date | Country | |
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| Parent | 14214244 | Mar 2014 | US |
| Child | 15494219 | US |
