Solar Cells Having Nanowire Titanium Oxide and/or Silicon Carbide Cores and Graphene Exteriors

Abstract

An apparatus comprising a plurality of solar cells that each comprise a nanowire titanium oxide core having graphene disposed thereon. By one approach this plurality of solar cells can comprise, at least in part, a titanium foil having the plurality of solar cells disposed thereon wherein at least a majority of the solar cells are aligned substantially parallel to one another and substantially perpendicular to the titanium foil. Such a plurality of solar cells can be disposed between a source of light and another modality of solar energy conversion such that both the solar cells and the another modality of solar energy conversion generate electricity using a same source of light.

Description

RELATED APPLICATION(S)

This is a continuation of U.S. patent application Ser. No. 14/420,860, Feb. 10, 2015, entitled Solar Cells Having Nanowire Titanium Oxide And/Or Silicon Carbide Cores And Graphene Exteriors, which application is a 371 of PCT/US13/53939, Filed Aug. 7, 2013, which is a continuation-in-part of U.S. patent application Ser. No. 13/908,215, Filed on Jun. 3, 2013, now U.S. Pat. No. 8,829,331, which is a continuation in part of U.S. patent application Ser. No. 13/682,229, filed on Nov. 20, 2012, now U.S. Pat. No. 8,586,999, which claims the benefit of U.S. Provisional Application No. 61/681,873, filed Aug. 10, 2012, which is incorporated by reference in its entirety herein.

TECHNICAL FIELD

This invention relates generally to the generation of electricity using solar energy.

BACKGROUND

Various modalities of solar energy conversion are known in the art. It is known, for example, to employ photovoltaic junctions in favor of converting sunlight directly into electricity. It is also known to convert sunlight into heat and to then utilize that heat to generate electricity.

That such approaches are known, however, is not a panacea in and of itself. Various implementation and operating problems arise with each such modality of solar energy conversion. Conversion efficiency, for example, varies amongst different modalities with many posited modalities performing quite poorly and none achieving high conversion efficiency. Those relative conversion efficiencies, in turn, quite directly impact the return on investment an enterprise can expect to receive for pursuing a given solar energy conversion system.

Dispatchability is another such example. Dispatchability refers to an ability to contribute electricity to a distribution grid at times of need. Since solar energy conversion requires the presence of the sun, converting solar energy into electricity cannot occur at night in the absence of an energy-storage mechanism. Energy storage can give rise to new concerns, however. Using batteries on a large scale for energy storage, for example, is relatively expensive in a variety of ways.

BRIEF DESCRIPTION OF THE DRAWINGS

The above needs are at least partially met through an apparatus pertaining to solar cells having silicon carbide and/or nanowire titanium oxide cores and graphene exteriors and the co-generation conversion of light into electricity described in the following detailed description, particularly when studied in conjunction with the drawings, wherein:

FIG. 1 comprises a side-elevational, sectioned schematic view as configured in accordance with various embodiments of the invention;

FIG. 2 comprises a side-elevational schematic view as configured in accordance with various embodiments of the invention;

FIG. 3 comprises a top plan view as configured in accordance with various embodiments of the invention;

FIG. 4 comprises a perspective schematic view as configured in accordance with various embodiments of the invention;

FIG. 5 comprises a perspective view as configured in accordance with various embodiments of the invention;

FIG. 6 comprises a top plan view as configured in accordance with various embodiments of the invention

FIG. 7 comprises a top plan view as configured in accordance with various embodiments of the invention;

FIG. 8 comprises a side-elevational schematic view as configured in accordance with various embodiments of the invention

FIG. 9 comprises a side-elevational schematic view as configured in accordance with various embodiments of the invention;

FIG. 10 comprises a perspective schematic view as configured in accordance with various embodiments of the invention;

FIG. 11 comprises a side-elevational schematic view as configured in accordance with various embodiments of the invention; and

FIG. 12 comprises a block diagram view as configured accordance with various embodiments of the invention.

Elements in the figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale. For example, the dimensions and/or relative positioning of some of the elements in the figures may be exaggerated relative to other elements to help to improve understanding of various embodiments of the present invention. Also, common but well-understood elements that are useful or necessary in a commercially feasible embodiment are often not depicted in order to facilitate a less obstructed view of these various embodiments of the present invention. Certain actions and/or steps may be described or depicted in a particular order of occurrence while those skilled in the art will understand that such specificity with respect to sequence is not actually required. The terms and expressions used herein have the ordinary technical meaning as is accorded to such terms and expressions by persons skilled in the technical field as set forth above except where different specific meanings have otherwise been set forth herein.

DETAILED DESCRIPTION

Generally speaking, pursuant to these various embodiments, a plurality of solar cells can each comprise a nanowire titanium oxide core having graphene disposed thereon. By one approach this plurality of solar cells can comprise, at least in part, a titanium foil having the plurality of solar cells disposed thereon wherein at least a majority of the solar cells are aligned substantially parallel to one another and substantially perpendicular to the titanium foil.

A corresponding apparatus can comprise a first modality of solar energy conversion that is disposed between a source of light and a second modality of solar energy conversion. So configured, both the first modality of solar energy conversion and the second modality of solar energy conversion can independently generate electricity using a same source of light. (As used herein, this reference to a “second” modality will be understood to not merely refer to a numerically additional or supplemental modality but will instead be understood to refer to another and different-in-kind modality as compared to the first modality of solar energy conversion.)

By one approach the first modality of solar energy conversion comprises a graphene-based modality of solar energy conversion such as the aforementioned solar cells that each comprise a nanowire titanium oxide core having graphene disposed thereon. The graphene-based modality of solar energy conversion can comprise a photovoltaic transducer that directly converts light into electricity. By one approach the second modality of solar energy conversion serves to convert heat into electricity. In such a case, the graphene-based modality of solar energy conversion can be disposed directly on a heat-absorbing surface that comprises a part of the second modality of solar energy conversion. That heat-absorbing surface, for example, can comprise a fluid-carrying conduit.

Fluids employed in such a second modality of solar energy conversion can be in excess of 350 degrees Centigrade. Such temperatures, of course, are quite inhospitable to the functioning of many ordinary photovoltaic devices that employ silicon or gallium arsenide. Graphene, however, is capable of operating in a satisfactory manner at such temperatures. Accordingly, a graphene-based photovoltaic junction can be expected to maintain photovoltaic functionality at a useful level of energy conversion notwithstanding the high temperatures of the adjacent second modality of solar energy conversion.

Accordingly, so configured, such a system comprises a cogeneration system for converting light into electricity. Depending upon the design employed the relative conversion efficiency of each modality can be relatively similar. By one approach, electricity generated by the graphene-based modality of solar energy conversion can be provided in real time to a distribution grid. Heat generated by the second modality of solar energy conversion, however, can be utilized immediately to generate electricity or can be stored and utilized later (for example, during a late afternoon period of peak loading and/or during the evening hours) to generate electricity to contribute to the distribution grid.

Such a co-generation facility offers other advantages beyond the improved dispatchability capability noted above. For example, the relative cost of such a co-generation facility need not be appreciably more than the cost of building and operating the second modality of solar energy conversion as an isolated system. To some very real extent, the present teachings permit leveraging the availability of such a system by greatly increasing the power output of the overall system while greatly enhancing the ability to time shift the distribution of the generated electricity. Accordingly, the present teachings offer a highly flexible approach to generating and distributing electricity.

Graphene is a substance made of pure carbon, with atoms arranged in a regular hexagonal pattern similar to graphite, but in a one-atom thick sheet (hence leading to the oft-used graphene descriptor “two-dimensional”). Graphene is the basic structural element of many carbon allotropes including graphite, charcoal, carbon nanotubes, and fullerenes. Graphene has a number of interesting optical, electrical, and thermal properties and has been the subject of much recent research. For example, the 2010 Nobel Prize in Physics went to researchers working on “groundbreaking” experiments involving graphene.

A single layer of graphene is nearly transparent. That said, however, a stack of forty-three graphene layers has an opacity of about ninety-nine percent and essentially completely absorbs light throughout the visible and near infrared regions of the solar spectrum notwithstanding having a film thickness of less than fifteen nanometers.

Referring now to the drawings, FIG. 1 depicts an object 100 having a core 101 that consists essentially of a wide band-gap material. This reference to a wide band-gap material will be understood to refer to a material having a valence band and a conduction band that differ by at least two electron volts. By one approach this core 101 can comprise titanium oxide. The reference to the core 101 consisting essentially of this material will be understood to refer to a core 101 that is largely pure in these regards but which can include trace impurities (and which can also include, for example, purposefully-introduced n-type or p-type dopants designed to elicit specific electrical performance).

In FIG. 1 the core 101 comprises a sphere. As will be shown below the core 101 can in fact assume any of a wide variety of regular and irregular forms. That said, by one approach the core 101 has at least one nanoscale bisectional dimension that does not exceed, for example, one hundred nanometers. This requirement does not specify that all dimensions of the core 100 are so limited, however. When the core 101 comprises, for example, a nanowire the core 101 might have a longitudinal length in excess of many hundreds of nanometers. (It is not necessary that the referred-to bisector divide the core 101 into two equal halves. Instead, as used herein a reference dimension is a “bisector” if the corresponding line passes through opposing points on the periphery and includes a geometric center of the core 101 as per a corresponding frame of reference. For example, when the core 1011 comprises a cylinder, a lateral cross-sectional diameter of that cylinder can serve as a bisector for these purposes.)

The depicted object 100 also has a shell 102 consisting essentially of graphene conformally disposed about at least a substantial portion of the core. As used herein this reference to “substantial” will be understood to refer to an amount in excess of fifty percent.

The thickness of this graphene shell 102 can vary with the application setting. For many purposes, however, the thickness can range from about one layer to about forty-three layers or so. Accordingly, for many purposes the thickness of the shell 102 is very thin. Generally speaking, when employed in a photovoltaic setting, the number of layers need be no more than are required to achieve a particular amount of light absorption (for example, forty-three layers of graphene will absorb nearly all incident light). It will be presumed herein that the shell 102 has an essentially uniform thickness for a given object 100 but these teachings will accommodate variations in these regards if desired and/or as appropriate to the needs of a given application setting. For example, in some application settings it can be useful if the shell 102 has no more than about ten layers of graphene

Generally speaking, electron/hole recombination rates are dependent on a variety of factors. In order to achieve a high efficiency solar cell, the material selected for the core 101 can be chosen to optimize charge separation in preference to electron/hole recombination.

By one approach, the shell 102 is conformally applied to the core 101 by contacting a reactant at elevated temperatures with nanopowders of different compounds such as borides, carbides, nitrides, oxides, and sulfides. Typical examples of such compounds are boron carbide, silicon carbide, silicon nitride, silicon oxide, titanium oxide, zinc oxide, iron sulfide, and so forth.

More particularly, by one approach the corresponding synthesis carries out the reaction(s) using size and shape-selected nanopowders of the selected material for the core 101. Per the reaction, hydrocarbon molecules decompose on the surfaces of the nanopowders to form the graphene layer(s) that comprises the shell 102. In particular, the nanomaterials cited above act as catalysts for the reactions to form graphene and result in highly unusual core/shell nanostructures in which the shell 102 is graphene and the cores 101 are composed of nanoparticles of the particular starting material. Additions of dopants during or after synthesis allows their incorporation into the shell or functionalization of the shell to produce desired dopant levels.

By one approach the reactions to form the graphene occur with first order kinetics at temperatures that are typically about 1000 degrees Centigrade lower in the presence than in the absence of the nanopowders. At least one reason for this dramatic lowering in reaction temperature is believed to be the ubiquitous presence of defects of various kinds on the surfaces of the nanomaterials. Because of the large surface area of the nanomaterials (relatively speaking) and the lowering of the activation energies of the reactions due to the presence of detects, the reaction kinetics are rapid at modest reaction temperatures.

The reaction rates are largely determined by temperature and temperature, of course, can be carefully controlled. Shell 102 thickness (i.e., the number of graphene layers), however, is largely controlled by the length of time the reaction is allowed to proceed at a controlled temperature. A layer-by-layer growth mechanism is therefore inherent in the presently-disclosed synthesis method making this a very powerful way of precisely controlling a key parameter that can serve as an important determinant of the ultimate performance of the material in a solar cell device.

This extremely versatile aspect of the described one-step synthesis method therefore allows one to adjust, in addition to core size and composition, the shell thickness parameter so as to be able to optimize the graphene photophysics. As alluded to above, the photophysics of graphene (involving excited-state transition lifetimes and charge-transport kinetics) can be highly useful to achieve a highly-efficient and commercially-viable solar cell. For example, a film consisting of 20 nanoparticles (each sized from around ten to eighty nanometers) that each have a monolayer graphene shell 102 would have a thickness of about 200-1600 nanometers and would absorb around ninety-five percent of the incident light. Such a very thin film solar cell would be expected to operate at considerably higher efficiencies while being considerably less costly than prior art solar cells.

The examples above presumed to encapsulate individual small particles with a graphene shell. These teachings will accommodate other approaches, however. By one approach, for example, the core 101 can comprise a plurality of nanoparticles 201 that are annealed to one another as illustrated in FIG. 2. In this simple example the resultant nanowire of the wide band-gap material comprises three sequentially-connected nanoparticles 201. It will be understood, of course, that such a nanowire can comprise a considerably larger number of such nanoparticles 201. Accordingly, although the lateral cross section of such a nanowire may remain within the aforementioned one hundred nanometer bisectional dimensional limitation the length of the nanowire can be of essentially any dimension of choice. By one approach the shells are applied subsequent to the annealing step.

By way of a more specific example (but without intending any specific limitations by way of these corresponding details), silicon carbide nanowires can be synthesized in a variety of ways. For example, chemical vapor deposition procedures can serve in these regards. As another example, silicon carbide nanoparticles can be heated to 2000K in the presence of a catalyst such as iron powder.

The graphene shells 102 surrounding the nanowires can in turn be synthesized to a predetermined thicknesses by reaction of the nanowires with carbonaceous substances at elevated temperatures as already stated or by heating the nanowires in vacuum to 1500K or in one bar of argon to 2000K. One straightforward and economically attractive synthesis procedure for objects 100 having a silicon carbide nanowire core 101 and a graphene shell 102 would comprise heating commercial silicon carbide powders to 2000K in argon to grow the nanowires, following which the catalyst is removed and the resultant material then reheated to 2000K in argon to form epitaxial graphene layers to a predetermined thickness and doping level

It may be noted and emphasized that these teachings will accommodate using cores 101 having any of a wide variety of forms. With reference to FIG. 3, for example, the cores 101 can comprise nanowires 300. As illustrated in FIG. 4, a graphene shell 102 of a desired thickness can then be readily conformally applied to such a core 101. By way of further illustrative examples, FIG. 5 illustrates a core 101 comprising a nanotube 500, FIG. 6 illustrates cores 101 comprising nanofibrils 600, and FIG. 7 illustrates a core 101 comprising a nanofabric 700. Again, these examples are intended to represent a non-exhaustive listing of possibilities in these regards.

Generally speaking, a viable solar cell will comprise a plurality of such objects 100 and hence will comprise a plurality of cores 101 that each have a shell 102 disposed thereabout. By one useful approach, when the cores 101 comprise generally longitudinal members (such as nanowires, nanorods, and/or nanotubes), the plurality of cores 101 can be disposed with their longitudinal axes oriented at least substantially parallel to one another. In particular, by one approach these longitudinal axes are also oriented substantially coaxial and parallel to anticipated light beams.

FIG. 8 presents one illustrative example in these regards. In this illustrative example a solar cell 800 has a first electrical pathway 801 and an opposing second electrical pathway 802 (the latter being transparent or at least translucent to permit light 804 to pass therethrough). These two electrical pathways 801 and 802 in turn couple to an electrical load 803 of choice such as but not limited to an electricity-distribution grid (via, for example, one or more transformers, regulators, and so forth as desired).

In this example, each of the cores 101 physically and electrically connects to the first electrical pathway 801 but not to the second electrical pathway 802. By one approach, the longitudinal axes of these cores 101 can range from about two hundred nanometers to no more than about five thousand nanometers.

By one approach, the nanowires that comprise the cores 101 in this example essentially consist of silicon carbide and have a length of from about three hundred to about five thousand nanometers and cross-sectional diameters of from about ten to about eighty nanometers coaxially. These cores 101 are surrounded by anywhere from a monolayer forty-three or so layers of graphene that essentially constitute the graphene shells 102.

These aligned silicon carbide cores 101 can be grown prior to growing the shells 102 by reacting a dilute mixture of methane in hydrogen with a silicon substrate carrying a catalyst to enable a vapor-liquid-solid growth mechanism. By one approach the catalyst facilitates the growth of aligned silicon carbide nanowires. A catalyst that forms a gallium/iron/silicon alloy, for example, allows the reaction with the carbon in the methane to occur in such a way as to lead to the growth of aligned silicon carbide nanowires.

The aligned silicon carbide nanowires can be grown the desired length by allowing the reaction to occur for a corresponding length of time at a temperature of about 1300 to about 1600 K. When the desired nanowire length has been reached, the gas mixture flowing over the nanowires is changed to pure methane to thereby create conditions for growing the graphene shells 102. Again, the number of layers in the shells 102 is controlled by the length of time growth is allowed to proceed at a given temperature.

The bottoms of the resulting nanowire nanostructures are attached to the first electrical pathway 801 that comprises, for example, silicon or some other conducting base, thus electrically connecting all of the cores 101. The tops of the nanowires carry graphene layers that are in electrical contact with all of the coaxial graphene shells 102 surrounding the nanowire cores 101. The growth process thus automatically creates a solar cell nanostructure that provides separate electrical connections to cores 101 and shells 102.

By one approach, dark current and majority carrier transport can be minimized by preventing contact of the coaxial graphene shells 102 with the silicon base and with the silicon carbide nanowire cores. This can be accomplished, for example, by chemical vapor deposition of a monolayer or multilayers of an insulator such as silicon dioxide prior to depositing the graphene shells 102.

Solar energy conversion efficiency associated with such a configuration is strongly enhanced in the nanostructured radial coaxial shell/core nanowire configuration over conventional planar solar cell configurations in part because electron diffusion lengths are very much shorter. This is particularly the case with regard to the thin graphene shells 102.

In addition, it may be observed that such a solar cell functions by virtue of the internal photoemission of energetic electrons emanating from the graphene layers and that are injected into the conduction band of the silicon carbide cores loll upon irradiation by light. The tens of milliamperes per square centimeter of photocurrent produced in this way is expected to have energies of about one electron volt under standard sunlight intensities. The stated cell performance is due in part to the potential barrier created when graphene forms a junction with silicon carbide. The magnitude of this potential barrier is estimated to be somewhat less than one electron volt based on calculations using the Anderson approximation which employs known values of quantities such as the work functions, electron affinities and electrical conductivities of graphene and silicon carbide

The described graphene/silicon carbide junction is also noteworthy in that the junction joins graphene (a zero band-gap material in which electrons behave as if they were massless fermions obeying Dirac wave functions according to the theory of quantum electrodynamics) to a wide band-gap semiconductor, silicon carbide, in which electrons obey the dictates of quantum mechanics. One of the functions of this junction, whose width is less than one nanometer, is to effectively transform “Dirac” electrons into “Schroedinger” electrons during the process of photoemission while concurrently minimizing the recombination of electrons with holes.

Generally speaking, restructuring of the atoms constituting such a junction has been shown to occur during junction synthesis. This restructuring still further enhances the interfacial area thus facilitating the complex functions of the junction. It is known, for example, that the position of the Fermi level of graphene changes at the heterojunction with a wide band-gap semiconductor. This exceptional circumstance does not occur with other metal/semiconductor heterojunctions at least in part because unlike the very large number of quantum states found with ordinary metals, graphene has only a small number of states near the Fermi level. The unique quantum physics of the graphene/semiconductor heterojunction is expected to benefit the characteristics of quantum structured solar cells such as their dark current behavior.

A useful attribute of a graphene/silicon carbide solar cell is its temperature stability. Both graphene and silicon carbide are high-temperature materials in that they have very high melting points and are thermodynamically stable. Diffusional processes of dopants in these materials are very slow at temperatures up to about 1000K thus helping to preserve the rectifying properties of the corresponding Schottky barrier up to temperatures of at least 600K.

The graphene/wide band-gap semiconductor materials all share these attributes with graphene/silicon carbide being an example. The graphene/wide band-gap materials are therefore uniquely capable of functioning as high-temperature solar cells in a co-generation application setting.

As another example in these regards (and still referring to FIG. 8), these teachings will accommodate providing a titanium foil and using a hydrothermal synthesis process to form a plurality of substantially aligned titanium oxide nanowires to serve as the nanowire cores 101. Again, this plurality of nanowire cores 101 are disposed substantially perpendicular to the titanium foil. (As used in these regards, the word “substantially” will be understood to mean within twenty-five degrees.) (As it is known in the art to form titanium oxide nanowires on a titanium foil using a hydrothermal synthesis process that exposes titanium foils to aqueous solutions consisting of mixtures of alkaline hydroxides in pressure vessels at elevated temperatures, for the sake of brevity no further elaboration is provided here in these particular regards aside from noting that, upon growing the desired aligned nanowires, these teachings will accommodate activating corresponding pressure relief values to thereby permit removing foil sections that have the desired aligned nanowires and replacing such foil sections with fresh foil sections to permit the process to be repeated upon closing the relevant pressure valves.)

By one approach such titanium oxide nanowires 101 can be doped (either n-type or p-type as desired) using a post-growth heat treatment process in conjunction with one or more predetermined (i.e., intended rather than accidental or incidental) dopants of choice. As one illustrative example in these regards, but without intending to suggest any particular limitations in these regards, p-type doping can be accomplished by heating the aforementioned titanium oxide nanowires 101 in a vacuum or by treatment with hydrogen gas (or another reactant of choice) at temperatures of 600 to 900 degrees Centrigrade for corresponding appropriate lengths of time and at particular pressures (to achieve a particular doping level).

Such an approach can serve to introduce oxygen vacuities in the titanium oxide lattice to thereby effectively create titanium in a trivalent state. Such doping can serve to reduce the average valency of the titanium oxide nanowires 101 to thereby increase the electrical conductivity thereof in a controlled way. Such an approach to p-type doping can help to optimize the characteristics of the graphene-titanium oxide junction in order to yield a solar cell that displays maximum efficiency with respect to converting light to electricity.

After such doping, the aligned titanium oxide nanowires 101 can be exposed to a hydrocarbon gas such as methane at temperatures of 900 to 1000 degrees Centrigrade for appropriate lengths of time to accomplish the desired chemical vapor deposition of graphene in the spaces between the wires as well as on the top surfaces of the nanowires 101 themselves. By one approach this graphene shell 102 is only lightly applied and comprises, for example, no more than about ten layers in thickness.

By one illustrative approach, and referring to FIG. 9, such solar cells 800 can be employed in conjunction with one or more Fresnel lenses 901 including linear Fresnel lens installations. By one approach, and as illustrated, it would even be possible to dispose the solar cells 800 directly on the lens 901 itself.

By way of another illustration and referring now to FIGS. 10 and 11, solar cells employing the present teachings can be applied in combination with a second modality of solar energy conversion such as a solar-heat based system 1000 having fluid-carrying tubes 1002 that absorb heat from sunlight 804 reflected from a corresponding parabolic trough solar collector 1001. In particular, and as illustrated in particular in FIG. 11, solar cells 800 as described herein can be externally disposed on at least a portion of the liquid-carrying conduit 1002 itself (such as on a portion of the conduit 1002 that receives the reflect light from the parabolic trough solar collector 1001). When the solar cells include a titanium foil as described above, the solar cells 800 can be disposed on the liquid-carrying conduit 1002 by physically attaching the titanium foil itself to the surface of the fluid-carrying solar collector 1001

FIG. 12 provides another illustrative example in these regards. In this example a co-generation facility 1200 employs a tower 1201 having a solar collector section 1202. Light 804 (from a star such as the Earth's sun 1203) may be received at the solar collector section 1202 directly from the light source but is also received, in a relatively greater quantity, as reflected from (typically) a plurality of solar reflectors 1204.

In this example the solar collector section 1202 includes one or more fluid-carrying conduits (for example, as shown in FIGS. 10 and 11) that carry a fluid, such as a molten salt, that is heated by the received light. As described above, grapheme-based photovoltaic transducers are again directly disposed on these conduits and serve to directly convert received sunlight into electricity. Again, when the graphene-based photovoltaic transducers include a titanium foil as described above, the graphene-based photovoltaic transducers can be disposed on these conduits by physically attaching the titanium foil itself to the surface of these conduits.

This electricity can be directed via one or more conductors 1205 to a distribution grid 1210 or, if desired, to an electricity-storage facility such as a bank of batteries.

The aforementioned hot fluid (which can exceed four hundred degrees Centigrade at operating temperatures) flows in this system to a storage tank 1206 where the heat can be banked until needed. When needed, that heat drives a steam generator 1207 that provides steam to a turbine generator 1208 that generates electricity to be provided to the distribution grid 1210. Cooled/cooling salt in such a system can be passed to and stored in a cold salt storage tank until needed.

So configured, direct conversion of photons to electricity is provided by the solar cells 800 while the associated heat is converted to electricity via, for example, conventional electromagnetic induction technology. Such a co-generation solar-based system can potentially convert around fifty percent of the solar flux energy content at moderate temperatures to electricity with photovoltaics and electromagnetic induction making roughly equal contributions.

The efficiency of such nanowire core solar cells depends not only on the nature of the junction between them as explained above but also on the ability of light to be absorbed by the nanostructured graphene shells in the first instance. In particular, in two out of three dimensions, such nanowires are small as compared to the wavelength of solar radiation. In fact, the absorption of light appears to be enhanced by about a factor of two for such nanowires as compared to bulk material. At least part of the reason for this appears to be that electromagnetic radiation enters or is transmitted by the aligned nanowires along their entire length. Thus, the large surface-to-volume ratio (compared to bulk materials) contributes significantly to the quantity of absorbed light.

As a result, radiation is absorbed very efficiently by such graphene shell/silicon-carbide-or-titanium-oxide nanowires. Furthermore, the light is distributed over a large graphene surface area because the graphene shells 102 surround each nanowire in such an embodiment. It is likely therefore that much higher radiation intensities can be tolerated by such nanostructured cells.

Each one of the vast numbers of such nanowires present in such a photovoltaic device comprises a unique structure that individually acts as an effective nantenna and optical rectifier. Calculations for cylindrical nanowires of radius twenty nanometers show that total light absorption occurs for nanowire lengths of about four hundred nanometers (which is, in turn, in the range of the wavelengths of visible light). Each nanowire can therefore be seen to simultaneously possess both the light (electromagnetic wave) gathering power of an antenna and the rectifying properties of a photovoltaic device.

The opacity of graphene (which is generally independent of the wavelength of light), combined with its use as a nantenna shell surrounding the nanowires, helps to ensure maximal harvesting of the incident sunlight. Consequently, the high solar collection efficiency of these graphene-based nantennas coupled with the highly efficient rectification properties of the graphene/silicon-carbide-or-titanium-oxide junctions combine to create a new and highly efficient class of solar cells.

In addition to such clear benefits as an enabler of efficient and inexpensive solar cells, these teachings can also be readily extended to other areas of interest. For example, these teachings can be readily leveraged in favor of a new class of biosensors: color sensitive retinal implants. Just as cochlear implants stimulate auditory nerve cells in the cochlea of the ear, so retinal implants stimulate cells in the retina of the eye that connect to the optic nerve. The search for such visual aids has been underway for a long time with the ultimate goal of providing color vision to the visually impaired. The ability to optimize the electrical response to light wavelength by controlling the length of these nanowires make these nanostructures uniquely suited to color discriminative retinal implant applications. Furthermore, because these biosensors are photosensors as well as photovoltaics, the incoming light itself can source the energy that powers their operation thus potentially obviating the need for batteries.

It will be appreciated that although the aforementioned first modality of solar energy conversion generates electricity photovoltaically while the second modality of solar energy conversion generates electricity thermally, the first modality will also typically produce heat as a byproduct of photovoltaic conversion. This heat can in fact augment the total electricity generated thermally by the second modality of solar energy conversion.

Those skilled in the art will recognize that a wide variety of modifications, alterations, and combinations can be made with respect to the above described embodiments without departing from the scope of the invention, and that such modifications, alterations, and combinations are to be viewed as being within the ambit of the inventive concept.

Claims

1. An apparatus comprising:

a core consisting essentially of wide band-gap material, wherein the core comprises a longitudinal member;

a shell consisting essentially of graphene conformally disposed about at least a substantial portion of the core, the shell being partially transparent to sunlight.

2. The apparatus of claim 1 wherein the shell comprises at least a single layer of graphene.

3. The apparatus of claim 1 wherein the shell comprises no more than about ten layers of graphene.

4. The apparatus of claim 1 wherein the longitudinal member comprises a nanowire.

5. The apparatus of claim 4 wherein the nanowire consists of a cylindrically-shaped member.

6. The apparatus of claim 4 wherein the length of the nanowire is more than twenty times greater than a widest lateral cross-section thereof.

7. The apparatus of claim 6 wherein the lateral cross section is at least twenty nanometers.

8. The apparatus of claim 1 wherein the wide band-gap material comprises at least one of:

boron;

iron;

titanium;

zinc;

carbon; and

silicon.

9. The apparatus of claim 8 wherein the wide band-gap material further comprises at least one of:

a boride;

a carbide;

a nitride;

an oxide; and a sulfide.

10. The apparatus of claim 1 wherein the wide band-gap material comprises at least one of:

a boride;

a carbide;

a nitride;

an oxide; and

a sulfide.

11. The apparatus of claim 1 wherein the apparatus comprises a plurality of the cores that each have one of the graphene shells disposed thereabout.

12. The apparatus of claim 10 wherein the plurality of cores are disposed with their longitudinal axes oriented substantially parallel to one another.

13. The apparatus of claim 11 wherein the longitudinal member has a length of at least 400 nanometers.

14. The apparatus of claim 12 wherein each of the cores comprises a nanowire having a radius of at least 20 nanometers.

15. The apparatus of claim 1 wherein the connection between a pathway connecting the shell and the core comprises a photovoltaic junction.

16. The apparatus of claim 1 wherein the core and the shell can include a dopant.

17. A photovoltaic transducer comprising:

a core consisting essentially of a wide band-gap material, wherein the core comprises a nanowire;

a shell consisting essentially of graphene conformally disposed about at least a substantial portion of the nanowire, the shell being partially transparent to sunlight;

wherein sunlight entering the nanowire and that is transmitted along the nanowire is at least mostly absorbed by the graphene notwithstanding the partial transparency of the shell.

18. The photovoltaic transducer of claim 17 wherein the graphene comprises at least a single monolayer of graphene.

19. The photovoltaic transducer of claim 18 wherein all of the sunlight that enters the nanowire and that is transmitted along the length of the nanowire is substantially absorbed by the graphene shell.

20. The photovoltaic transducer of claim 17 further comprising:

a plurality of the nanowires disposed on a shared substrate, wherein each of the nanowires has one of the graphene shells conformally disposed thereabout.

21. The photovoltaic transducer of claim 20 wherein each of the nanowires comprising the plurality of the nanowires are disposed substantially perpendicular to the shared substrate.