[0001] This application claims priority to and benefit of U.S. Provisional Patent Application No. 60/408,722, filed Sep. 5, 2002, “Nanocomposites” Mihai Buretea et al., which is incorporated herein by reference in its entirety for all purposes.
[0002] The present invention is in the field of nanocomposites. More particularly, the invention includes composite materials comprising nanostructures (e.g., nanowires, nanorods, branched nanowires, nanotetrapods, nanocrystals, quantum dots, and nanoparticles), methods and compositions for making such composites, and articles comprising such composites. Waveguides and light concentrators comprising nanostructures that are not necessarily part of a nanocomposite are also features of the invention.
[0003] A composite material (a composite) is formed by combining two or more materials that have different properties. The composite typically has properties different from those of its constituent materials, but within the composite the original materials can still be identified (they do not dissolve; an interface is maintained between them). Typically, one material, called the matrix, surrounds and binds together discrete units (e.g., particles, fibers, or fragments) of a second material, called the filler.
[0004] Many composite materials are currently known and widely used, for example, concrete (a composite in which the matrix is cement and the filler is aggregate), fiberglass (glass fibers in a plastic matrix), and many other types of reinforced plastics. However, there is continued demand for novel composites with desirable properties for many applications.
[0005] For example, the electronics industry utilizes materials that have high dielectric constants and that are also flexible, easy to process, and strong. Finding single component materials possessing these properties is difficult. For example, high dielectric constant ceramic materials such as ferroelectric SrTiO
[0006] Novel materials would also be useful in other industries, for example, in solar energy technology. The development of solar energy technology is primarily concerned with reducing the cost of energy conversion. This is typically achieved in one of two ways: 1) increasing the conversion efficiency of light in a solar cell without proportionately increasing its cost, or 2) increasing the size of the cell without proportionately increasing its cost. In the first case, the same number of photons hit the solar cell, but a larger number of them are converted into electricity (or the ones that are converted are converted at a higher total power). In the second, the conversion efficiency is the same, but the larger surface area means that more photons are collected per unit time. Since the sun is free, this results in improved cost efficiency. Unfortunately, at the moment neither of these strategies is effective. The complexity of increased-efficiency solar cells causes their cost to be substantially greater than the increase in performance. Similarly, larger solar panels are proportionately more expensive due to difficulties in fabricating uniform devices over large areas.
[0007] Among other aspects, the present invention provides high dielectric constant nanocomposites that overcome the processing issues noted above and solar concentrators comprising nanostructures. A complete understanding of the invention will be obtained upon review of the following.
[0008] The present invention provides nanocomposites (composite materials comprising nanostructures such as nanowires, branched nanowires, nanotetrapods, nanocrystals, and nanoparticles, for example), compositions and methods for making such nanocomposites, and articles comprising such composites.
[0009] One aspect of the invention provides waveguides and light concentrators comprising nanostructures, which in some but not all embodiments are provided as part of a nanocomposite. The nanostructures absorb light impinging on the waveguide or light concentrator and re-emit light. The nanostructures can be located and/or oriented within the waveguide or light concentrator in a manner that increases the percentage of re-emitted light that can be waveguided. For example, the nanostructures can be located and/or oriented within a light concentrator in such a manner that a greater percentage of the reemitted light is waveguided (and can thus be collected at the edge of the concentrator) than would be waveguided if emission by the collection of nanostructures were isotropic (equal in every direction).
[0010] One class of embodiments provides a waveguide comprising a cladding (e.g., a material that has a lower refractive index than the core, e.g., a lower refractive index solid, liquid, or gas, e.g., air) and a core, where the core comprises one or more nanowires or branched nanowires (e.g., nanotetrapods) and a matrix. The first and second surfaces of the core are substantially parallel so light emitted by the nanowires or branched nanowires can be efficiently waveguided by total internal reflection, and the core has a higher index of refraction than the cladding, for a similar reason. The nanowires or branched nanowires can comprise essentially any convenient material (e.g., a fluorescent material, a semiconducting material) and can comprise essentially a single material or can be heterostructures. The size of the nanostructures (e.g., the diameter and/or aspect ratio of nanowires) can be varied. In embodiments in which the core comprises a plurality of nanowires, the nanowires can be either randomly or substantially nonrandomly oriented (e.g., with a majority of the nanowires being more nearly perpendicular than parallel to a surface of the core, or with the nanowires forming a liquid crystal phase). Nonrandom orientation of the nanowires can increase the efficiency of the waveguide by increasing the percentage of light that is reemitted at angles greater than the critical angle for the particular core-cladding combination. The waveguides can be connected to a collector for collecting waveguided light, and can be used in stacks to form a multilayer light concentrator, in which the different layers comprise waveguides that can be optimized to collect light of different wavelengths.
[0011] Another class of embodiments provides a waveguide comprising a cladding (e.g., a material that has a lower refractive index than the core, e.g., a lower refractive index solid, liquid, or gas, e.g., air), a first core, and a first layer that comprises one or more nanostructures. The first layer is distributed on but is not necessarily in contact with the first core, whose first and second surfaces are substantially parallel. Some embodiments further comprise a second core. The first layer can be in direct contact with the first and/or second core(s), or can be separated from either or both, e.g., by a layer of a material whose refractive index is between that of the first layer and the core. The first layer preferably has a thickness less than about one wavelength of the light emitted by the nanostructures. The nanostructures can be nanowires, nanocrystals, or branched nanowires (e.g., nanotetrapods). The nanostructures can comprise essentially any convenient material (e.g., a fluorescent material, a semiconducting material) and can comprise essentially a single material or can be heterostructures. The size of the nanostructures (e.g., the diameter and/or aspect ratio of nanowires) can be varied. The nanostructures can be provided in various manners, e.g., as substantially pure nanostructures or as part of a nanocomposite. In embodiments in which the waveguide comprises a plurality of nanowires, the nanowires can be either randomly or substantially nonrandomly oriented (e.g., with a majority of the nanowires being more nearly perpendicular than parallel to a surface of the first core, or with the nanowires forming a liquid crystal phase). Nonrandom orientation of the nanowires can increase the efficiency of the waveguide by increasing the percentage of light that is reemitted at angles greater than the critical angle. The waveguides can be connected to a collector for collecting waveguided light, and can be used in stacks to form a multilayer light concentrator, in which the different layers comprise waveguides that can be optimized to collect light of different wavelengths.
[0012] Another aspect of the invention provides various nanocomposites. One composite material comprises a plurality of nanowires and a polymeric or small molecule or molecular matrix that is used to orient the nanowires. Another class of embodiments provides composites comprising one or more nanostructures (for example, nanowires, nanocrystals, or branched nanowires, e.g. nanotetrapods) and a polymeric matrix comprising polysiloxane (e.g., polydimethylsiloxane). The nanostructures can comprise essentially any material (e.g., a ferroelectric, fluorescent, or semiconducting material). The composite can further comprise an additive such as e.g. a surfactant or solvent. Articles comprising such composites (e.g., an LED, laser, waveguide, or amplifier) are also features of the invention.
[0013] Yet another class of embodiments provides nanocomposites comprising a small molecule or molecular matrix or a matrix comprising an organic polymer or an inorganic glass and one or more branched nanowires (e.g., nanotetrapods) or ferroelectric or semiconducting nanowires having an aspect ratio greater than about 10. The size of the nanostructures (e.g., the diameter and/or aspect ratio of nanowires) can be varied. In embodiments in which the composite comprises a plurality of nanowires, the nanowires can be either randomly or substantially nonrandomly oriented. For example, the composite can be formed into a thin film (strained or unstrained) within which a majority of the nanowires can be substantially parallel to or more nearly perpendicular than parallel to a surface of the film.
[0014] An additional class of embodiments provides composite materials comprising nanostructures and a polymeric matrix, a small molecule or molecular matrix, or a glassy or crystalline inorganic matrix where the composite is distributed on a first layer of a material that conducts substantially only electrons or substantially only holes. The composite and the first layer can be in contact or can be separated, for example, by a second layer comprising a conductive material. The first layer can be distributed on an electrode, and can be in contact with the electrode or separated from it, for example, by a third layer comprising a conductive material. The conductive material may conduct electrons or holes or both.
[0015] In another class of embodiments, the invention provides nanocomposites that support charge recombination or charge separation. These composites comprise a matrix and one or more nanostructures (e.g., nanocrystals, nanowires, branched nanowires, or nanotetrapods), where semiconducting materials comprising the matrix and/or the nanostructures have a type I or type II band offset with respect to each other.
[0016] An additional class of embodiments provides composites comprising nanostructures and a polymeric or small molecule or molecular matrix, in which the components of the matrix have an affinity for the surface of the nanostructure or for surface ligands on the nanostructures. For example, the surface ligands can each comprise a molecule found in the small molecule or molecular matrix or a derivative thereof or a monomer found in the polymeric matrix or a derivative thereof.
[0017] Another class of embodiments provides composite materials comprising one or more ferroelectric nanowires or nanoparticles and a small molecule or molecular matrix or a matrix comprising one or more polymers (e.g., an organic, inorganic, or organometallic polymer). The nanowires or nanoparticles can comprise essentially any convenient ferroelectric material, and their size (e.g., their diameter and/or aspect ratio) can be varied. The dielectric constant of the composite can be adjusted by adjusting the amount of ferroelectric nanowires or nanoparticles included in the composite. The composite (or its matrix) can further comprise an additive, for example, a surfactant, solvent, catalyst, plasticizer, antioxidant, or strengthening fiber. The composite material can be formed into a film or applied to a substrate. An additional embodiment provides a composition comprising such a composite; the composition comprises particles of the composite material, at least one solvent whose concentration can be varied, and at least one glue agent (e.g., a polymer or cross-linker). The composition can form a film, e.g., after application to a substrate.
[0018] Compositions that can be used to form a nanocomposite comprising ferroelectric nanowires or nanoparticles are another feature of the invention. In one embodiment, the composition comprises one or more ferroelectric nanowires or nanoparticles, at least one solvent, and one or more polymers. The polymers can be provided in any of a number of forms. For example, the polymer can be soluble in the solvent or can comprise oligomers soluble in the solvent, or the polymer can comprise emulsion polymerized particles. The materials and size of the nanowires and nanoparticles can be varied essentially as described above. The composition can further comprise a glue agent, cross-linking agent, surfactant, or humectant. The consistency of the composition can be controlled (e.g., by varying the solvent concentration) to make the composition suitable for use as an inkjet printing ink or screenprinting ink, or for brushing or spraying onto a surface or substrate. The composition can be used to form a film (e.g., a high dielectric nanocomposite film).
[0019] In a similar embodiment, the composition comprises one or more ferroelectric nanowires or nanoparticles, at least one solvent, and at least one monomeric precursor of at least one polymer. The materials and size of the nanowires and nanoparticles can be varied essentially as described above. The composition can further comprise a catalyst, cross-linking agent, surfactant, or humectant. The consistency of the composition can be controlled (e.g., by varying the solvent concentration) to make the composition suitable for use as an inkjet printing ink or screenprinting ink, or for brushing or spraying onto a surface or substrate. The composition can be used to form a film (e.g., a high dielectric nanocomposite film).
[0020] Methods for making the composite materials and compositions described above provide an additional feature of the invention.
[0021] Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which the invention pertains. The following definitions supplement those in the art and are directed to the current application and are not to be imputed to any related or unrelated case, e.g., to any commonly owned patent or application. Although any methods and materials similar or equivalent to those described herein can be used in the practice for testing of the present invention, the preferred materials and methods are described herein. Accordingly, the terminology used herein is for the purpose of describing particular embodiments only, and is not intended to be limiting.
[0022] As used in this specification and the appended claims, the singular forms “a,” “an” and “the” include plural referents unless the context clearly dictates otherwise. Thus, for example, reference to “a nanostructure” includes a plurality of such nanostructures, and the like.
[0023] An “aspect ratio” is the length of a first axis of a nanostructure divided by the average of the lengths of the second and third axes of the nanostructure, where the second and third axes are the two axes whose lengths are most nearly equal each other. For example, the aspect ratio for a perfect rod would be the length of its long axis divided by the diameter of a cross-section perpendicular to (normal to) the long axis.
[0024] A “branched nanowire” is a nanostructure having three or more arms, where each arm has the characteristics of a nanowire, or a nanostructure having two or more arms, each arm having the characteristics of a nanowire and emanating from a central region that has a distinct crystal structure, e.g., having cubic symmetry, e.g., where the angle between any two arms is approximately 109.5 degrees. Examples include, but are not limited to, bipods, tripods, and nanotetrapods (tetrapods). A branched nanowire can be substantially homogenous in material properties or can be heterogeneous (a heterostructure). For example, a branched nanowire can comprise one material at the center of the branch which is a single crystal structure and a second material along the arms of the structure that is a second crystal structure, or the materials along each of the arms can differ, or the material along any single arm can change as a function of length or radius of the arm. Branched nanowires can be fabricated from essentially any convenient material or materials. Branched nanowires can comprise “pure” materials, substantially pure materials, doped materials and the like, and can include insulators, conductors, and semiconductors.
[0025] The terms “crystalline” or “substantially crystalline,” when used with respect to nanostructures, refer to the fact that the nanostructures typically exhibit long-range ordering across one or more dimensions of the structure. It will be understood by one of skill in the art that the term “long range ordering” will depend on the absolute size of the specific nanostructures, as ordering for a single crystal cannot extend beyond the boundaries of the crystal. In this case, “long-range ordering” will mean substantial order across at least the majority of the dimension of the nanostructure. In some instances, a nanostructure can bear an oxide or other coating, or can be comprised of a core and at least one shell. In such instances it will be appreciated that the oxide, shell(s), or other coating need not exhibit such ordering (e.g. it can be amorphous, polycrystalline, or otherwise). In such instances, the phrase “crystalline,” “substantially crystalline,” “substantially monocrystalline,” or “monocrystalline” refers to the central core of the nanostructure (excluding the coating layers or shells). The terms “crystalline” or “substantially crystalline” as used herein are intended to also encompass structures comprising various defects, stacking faults, atomic substitutions, and the like, as long as the structure exhibits substantial long range ordering (e.g., order over at least about 80% of the length of at least one axis of the nanostructure or its core). In addition, it will be appreciated that the interface between a core and the outside of a nanostructure or between a core and an adjacent shell or between a shell and a second adjacent shell may contain non-crystalline regions and may even be amorphous. This does not prevent the nanostructure from being crystalline or substantially crystalline as defined herein.
[0026] The “diameter of a nanocrystal” refers to the diameter of a cross-section normal to a first axis of the nanocrystal, where the first axis has the greatest difference in length with respect to the second and third axes (the second and third axes are the two axes whose lengths most nearly equal each other). The first axis is not necessarily the longest axis of the nanocrystal; e.g., for a disk-shaped nanocrystal, the cross-section would be a substantially circular cross-section normal to the short longitudinal axis of the disk. Where the cross-section is not circular, the diameter is the average of the major and minor axes of that cross-section.
[0027] The “diameter of a nanowire” refers to the diameter of a cross-section normal to the major principle axis (the long axis) of the nanowire. Where the cross-section is not circular, the diameter is the average of the major and minor axes of that cross-section.
[0028] The term “heterostructure” when used with reference to nanostructures refers to nanostructures characterized by at least two different and/or distinguishable material types. Typically, one region of the nanostructure comprises a first material type, while a second region of the nanostructure comprises a second material type. In certain embodiments, the nanostructure comprises a core of a first material and at least one shell of a second (or third etc.) material, where the different material types are distributed radially about the long axis of a nanowire, a long axis of an arm of a branched nanowire, or the center of a nanocrystal, for example. (A shell need not completely cover the adjacent materials to be considered a shell or for the nanostructure to be considered a heterostructure; for example, a nanocrystal characterized by a core of one material covered with small islands of a second material is a heterostructure.) In other embodiments, the different material types are distributed at different locations within the nanostructure; e.g., along the major (long) axis of a nanowire or along a long axis of arm of a branched nanowire. Different regions within a heterostructure can comprise entirely different materials, or the different regions can comprise a base material (e.g., silicon) having different dopants or different concentrations of the same dopant.
[0029] The term “monocrystalline” when used with respect to a nanostructure indicates that the nanostructure is substantially crystalline and comprises substantially a single crystal. When used with respect to a nanostructure heterostructure comprising a core and one or more shells, “monocrystalline” indicates that the core is substantially crystalline and comprises substantially a single crystal.
[0030] A “nanocrystal” is a nanostructure that is substantially monocrystalline. Nanocrystals typically have an aspect ratio between about 0.1 and about 1.5 (e.g., between about 0.1 and about 0.5, between about 0.5 and about 1, or between about 1 and about 1.5). Thus, nanocrystals include, for example, substantially spherical nanocrystals with aspect ratios between about 0.8 and about 1.2 and disk-shaped nanocrystals. Nanocrystals typically have a diameter between about 1.5 nm and about 15 nm (e.g., between about 2 nm and about 5 nm, between about 5 nm and about 10 nm, or between about 10 nm and about 15 nm). Nanocrystals can be substantially homogeneous in material properties, or in certain embodiments can be heterogeneous (e.g. heterostructures). In the case of nanocrystal heterostructures comprising a core and one or more shells, the core of the nanocrystal is substantially monocrystalline, but the shell(s) need not be. The nanocrystals can be fabricated from essentially any convenient material or materials. The nanocrystals can comprise “pure” materials, substantially pure materials, doped materials and the like, and can include insulators, conductors, and semiconductors.
[0031] A “nanoparticle” is any nanostructure having an aspect ratio less than about 1.5. Nanoparticles can be of any shape, and include, for example, nanocrystals, substantially spherical particles (having an aspect ratio of about 0.9 to about 1.2), and irregularly shaped particles. Nanoparticles can be amorphous, crystalline, partially crystalline, polycrystalline, or otherwise. Nanoparticles can be substantially homogeneous in material properties, or in certain embodiments can be heterogeneous (e.g. heterostructures). The nanoparticles can be fabricated from essentially any convenient material or materials. The nanoparticles can comprise “pure” materials, substantially pure materials, doped materials and the like, and can include insulators, conductors, and semiconductors.
[0032] A “nanostructure” is a structure having at least one region or characteristic dimension with a dimension of less than about 500 nm, e.g., less than about 200 nm, less than about 100 nm, less than about 50 nm, or even less than about 20 nm. Typically, the region or characteristic dimension will be along the smallest axis of the structure. Examples of such structures include nanowires, nanorods, nanotubes, branched nanowires, nanotetrapods, tripods, bipods, nanocrystals, nanodots, quantum dots, nanoparticles, and the like. Nanostructures can be substantially homogeneous in material properties, or in certain embodiments can be heterogeneous (e.g. heterostructures). The nanostructures can be fabricated from essentially any convenient material or materials. The nanostructures can comprise “pure” materials, substantially pure materials, doped materials and the like, and can include insulators, conductors, and semiconductors. A nanostructure can optionally comprise one or more surface ligands (e.g., surfactants).
[0033] A “nanotetrapod” is a generally tetrahedral branched nanowire having four arms emanating from a central region, where the angle between any two arms is approximately 109.5 degrees.
[0034] A “nanowire” is a nanostructure that has one principle axis that is longer than the other two principle axes. Consequently, the nanowire has an aspect ratio greater than one; nanowires of this invention have an aspect ratio greater than about 1.5 or greater than about 2. Short nanowires, sometimes referred to as nanorods, typically have an aspect ratio between about 1.5 and about 10. Longer nanowires have an aspect ratio greater than about 10, greater than about 20, greater than about 50, or greater than about 100, or even greater than about 10,000. The diameter of a nanowire is typically less than about 500 nm, preferably less than about 200 nm, more preferably less than about 150 nm, and most preferably less than about 100 nm, about 50 nm, or about 25 nm, or even less than about 10 nm or about 5 nm. The nanowires of this invention can be substantially homogeneous in material properties, or in certain embodiments can be heterogeneous (e.g. nanowire heterostructures). The nanowires can be fabricated from essentially any convenient material or materials. The nanowires can comprise “pure” materials, substantially pure materials, doped materials and the like, and can include insulators, conductors, and semiconductors. Nanowires are typically substantially crystalline and/or substantially monocrystalline, but can be, e.g., polycrystalline or amorphous. Nanowires can have a variable diameter or can have a substantially uniform diameter, that is, a diameter that shows a variance less than about 20% (e.g., less than about 10%, less than about 5%, or less than about 1%) over the region of greatest variability and over a linear dimension of at least 5 nm (e.g., at least 10 nm, at least 20 nm, or at least 50 nm). Typically the diameter is evaluated away from the ends of the nanowire (e.g. over the central 20%, 40%, 50%, or 80% of the nanowire). A nanowire can be straight or can be e.g. curved or bent, over the entire length of its long axis or a portion thereof. In certain embodiments, a nanowire or a portion thereof can exhibit two- or three-dimensional quantum confinement. Nanowires according to this invention can expressly exclude carbon nanotubes, and, in certain embodiments, exclude “whiskers” or “nanowhiskers”, particularly whiskers having a diameter greater than 100 nm, or greater than about 200 nm.
[0035] The phrase “substantially nonrandom” used to describe the orientation of nanowires means that the nanowires do not occupy a purely random distribution of orientations with respect to each other. A collection of nanowires is substantially nonrandomly oriented if, when the position of each nanowire is represented as a vector of unit length in a three-dimensional rectangular coordinate system, at least one component of the vector average of the nanowires' orientations is non-zero (when representing a nanowire by a vector, any intrinsic difference between the two ends of the nanowire can typically be ignored). For example, the nanowires in a collection of nanowires (e.g., the nanowires in a composite material comprising nanowires) would have substantially nonrandom orientations if a higher percentage of the nanowires pointed in one direction (or in one of at least two specific directions) than in any other direction (e.g., if at least 10%, at least 50%, at least 75%, or at least 90% of the nanowires pointed in a particular direction). As another example, nanowires in a thin film of a composite comprising nanowires would be substantially nonrandomly oriented if a majority of the nanowires had their long axes more nearly perpendicular than parallel to a surface of the film (or vice versa) (the nanowires can be substantially nonrandomly oriented yet not point in at least one specific direction). The preceding examples are for illustration only; a collection of nanowires could possess less order than these examples yet still be substantially nonrandomly oriented.
[0036] A “surface ligand” of a nanostructure is a molecule that has an affinity for and is capable of binding to at least a portion of the nanostructure's surface. Examples include various surfactants. Surface ligands or surfactants can comprise e.g. an amine, a phosphine, a phosphine oxide, a phosphonate, a phosphonite, a phosphinic acid, a phosphonic acid, a thiol, an alcohol, an amine oxide, a polymer, a monomer, an oligomer, or a siloxane.
[0037] A “type I band offset” between two semiconducting materials means that both the conduction band and the valence band of the semiconductor with the smaller bandgap are within the bandgap of the other semiconductor.
[0038] A “type II band offset” between two semiconducting materials means that either the conduction band or the valence band, but not both, of one semiconductor is within the bandgap of the other semiconductor.
[0039]
[0040]
[0041]
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[0044]
[0045]
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[0047] Composite materials comprising nanostructures (nanocomposites) are provided, along with articles comprising nanocomposites and methods and compositions for making such composites.
[0048] One class of embodiments provides waveguides and light concentrators comprising nanostructures. This class of embodiments is based on the ability of certain nanostructures (e.g., nanostructures comprising a fluorescent material) to absorb and re-emit light that can then be waveguided by total internal reflection within at least one core. In many but not all embodiments, the nanostructures are provided in the form of a nanocomposite. In some embodiments, the nanostructures are substantially nonrandomly oriented to increase the efficiency of the waveguide or light concentrator.
[0049] Methods for orienting nanostructures within a composite material are discussed, including using the matrix or components thereof to orient the nanostructures. Accordingly, one aspect of the invention provides nanocomposites in which the matrix is used to orient nanowires.
[0050] The invention also provides nanocomposites comprising nanostructures and a polysiloxane matrix, as well as articles comprising such composites. Another class of embodiments provides nanocomposites comprising branched nanowires or ferroelectric or semiconducting nanowires. Yet another class of embodiments includes the use of nanocomposites with blocking layers that conduct substantially only electrons or substantially only holes. Other nanocomposites are provided that support charge recombination or charge separation (e.g., for use in luminescent or photovoltaic devices). An additional class of embodiments provides composites in which interaction between the nanostructures and the matrix is enhanced, for example, by surface ligands on the nanostructures.
[0051] One general class of embodiments provides nanocomposites that comprise ferroelectric nanowires or ferroelectric nanoparticles and that can thus possess high dielectric constants. Compositions for making such nanocomposites (e.g., compositions suitable for use as inkjet or screen printing inks) are also provided, as are methods for making all the above composites and compositions. The following sections describe the invention in more detail.
[0052] Waveguides and Light Concentrators
[0053] One aspect of the present invention provides waveguides and light concentrators (e.g., solar concentrators) comprising nanostructures. Energy (e.g., light) is absorbed and re-emitted by the nanostructures and is waveguided by total internal reflection within a core. In many embodiments, the nanostructures are provided in the form of a nanocomposite.
[0054] Dye and Quantum Dot Solar Concentrators
[0055] As mentioned previously, typical approaches to reducing the cost of solar energy conversion are to increase the efficiency and/or size of a solar cell without proportionately increasing its cost. A different method of improving cost performance is to increase the intensity of light on a single cell. Assuming that the cell does not burn or saturate under the increased illumination, and assuming that the apparatus used to concentrate the light does not cost proportionately more than the increase in intensity, this can also produce an improvement in cost efficiency. One idea for this type of device is to take a large plastic or glass sheet and dope it with organic dye molecules that absorb and reemit light with high efficiency. Solar concentrators of this type are described in e.g., Weber et al. (1976)
[0056] By using a very large area concentrator, the intensity of the impinging light can be greatly concentrated, as represented by the equation C=S*G, where C is the ratio of light concentration collected, S is the ratio of the surface area of the sheet being illuminated by impinging light to the area of the collector at the edge of the sheet, and G represents losses in the concentrator that affect the ratio of the photons striking the surface of the concentrator to the number of photons that get guided to the edge of the sheet. In a standard concentrator, there are a number of inefficiencies that influence G. First, dye molecules only absorb a narrow band of wavelengths, and so most of the light that hits the concentrator is not absorbed, but simply passes through and is lost. This can be a substantial loss in overall efficiency. Second, dye molecules emit with finite quantum efficiency. As a result, even the photons that are absorbed do not all get re-emitted. Third, dye molecules are photo-unstable and eventually the concentrator stops working as the dye photobleaches. Finally, of the photons that are re-emitted, only those that emit at angles greater than the critical angle actually get wave guided and eventually collected. All other photons are lost. Other factors such as losses due to reabsorption or scatter within the concentrator also affect G, however, the factors above represent the major contributors to loss in this type of concentrator. As a result of these issues, solar concentrators of this type have not been implemented in a commercial product to date.
[0057] In order to improve the overall efficiency of a concentrator of the type described above, improvements in the following five characteristics are possible: 1) absorption efficiency; 2) absorption bandwidth (the breadth of the absorption spectrum); 3) quantum yield of the fluorophores in the concentrator; 4) photostability of the fluorophores in the concentrator; and 5) the angular distribution of intensities emitted from the fluorophores in the concentrator after illumination from above (the percentage of the reemitted photons have an angle greater than the critical angle and therefore get waveguided).
[0058] An improvement upon the dye molecule concentrator was made by replacing the dye molecules with quantum dots. See, e.g., Barnham et al. (2000) “Quantum-dot concentrator and thermodynamic model for the global red-shift”
[0059] In a quantum dot concentrator having quantum dots embedded in a transparent sheet surrounded by air, where the collection of dots emits light isotropically, at most ½*(cos(asin(n
[0060] Ideas for improving the performance of a quantum dot concentrator include incorporating quantum dots with higher fluorescence quantum efficiency (e.g., greater than 30% or greater than 50%) or quantum dots with a substantially monodisperse size and/or shape distribution (see e.g., U.S. patent application Ser. No. 20020,071,952 by Bawendi et al entitled “Preparation of nanocrystallites”).
[0061] Light Concentrators
[0062] In a first general class of embodiments, the light concentrators of this invention comprise at least one core, at least one adjacent material that has a lower index of refraction than the core and that is in contact with at least a portion of a surface of the core, and a plurality of nanostructures. The nanostructures absorb light that impinges on a surface of the concentrator and re-emit light. The location of the nanostructures within the concentrator and/or the orientation of the nanostructures is controlled such that the fraction of the light emitted by the nanostructures that is waveguided by the core or cores is greater than ½*(cos(asin(n
[0063] The location of the nanostructures within the concentrator can be controlled. For example, the nanostructures can be located within the core or can be outside the core, e.g., in the material adjacent to the core. Alternatively or in addition, the orientation of the nanostructures can be controlled. For example, the light concentrator can comprise any nanostructures that have a definable unique axis of symmetry (e.g. a unique crystal axis such as the c-axis of a wurtzite na