Polymer wrapped carbon nanotube near-infrared photovoltaic devices

Description of equivalent WO 2010036398 A2

POLYMER WRAPPED CARBON NANOTUBE NEAR-INFRARED PHOTOVOLTAIC DEVICES

GOVERNMENT RIGHTS

0003[0001] This invention was made with Government support from the United States

0004Air Force Office of Sponsored Research, Grant No. FA9550-07-1-0364, and DAAB07- 01-D-G602, Army Night Vision and Electronic Sensors Directorate (CECOM). The United States Government has certain rights to this invention.

CROSS-REFERENCE TO RELATED APPLICATION

0006[0002] This application claims the benefit under 35 U.S.C. § 119(e) of U.S.

0007Provisional Application Ser. No. 61/049,594, filed May 1, 2008, and U.S. Provisional Application Ser. No. 61/1 10,220, filed October 31, 2008, the disclosures of which are incorporated herein in their entirety.

FIELD OF THE INVENTION

0009[0003] The present disclosure is related to the field of organic semiconductors, carbon nanotubes, infrared photodetectors and photovoltaic cells.

BACKGROUND

0011[0004] Optoelectronic devices rely on the optical and electronic properties of materials to either produce or detect electromagnetic radiation electronically or to generate electricity from ambient electromagnetic radiation.

0012[0005] Photosensitive optoelectronic devices convert electromagnetic radiation into an electrical signal or electricity. Solar cells, also called photovoltaic ("PV") devices, are a type of photosensitive optoelectronic devices that are specifically used to generate electrical power. Photoconductor cells are a type of photosensitive optoelectronic device that are used in conjunction with signal detection circuitry which monitors the resistance of the device to detect changes due to absorbed light. Photodetectors, which may receive an applied bias voltage, are a type of photosensitive optoelectronic device that are used in conjunction with current detecting circuits which measures the current generated when the photodetector is exposed to electromagnetic radiation.

0013[0006] These three classes of photosensitive optoelectronic devices maybe distinguished according to whether a rectifying junction as defined below is present and also according to whether the device is operated with an external applied voltage, also known as a bias or bias voltage. A photoconductor cell does not have a rectifying junction and is normally operated with a bias. A PV device'has at least one rectifying junction and is operated with no bias. A photodetector may have a rectifying junction and is usually but not always operated with a bias.

0014[0007] When electromagnetic radiation of an appropriate energy is incident upon an organic semiconductor material, a photon can be absorbed to produce an excited molecular state. In organic photoconductive materials, the excited molecular state is generally believed to be an "exciton," i.e., an electron-hole pair in a bound state which is transported as a quasi-particle. An exciton can have an appreciable life-time before geminate recombination ("quenching"), which refers to the original electron and hole recombining with each other (as opposed to recombination with holes or electrons from other pairs). To produce a photocurrent, the electron-hole forming the exciton is typically separated at a rectifying junction.

0015[0008] In the case of photosensitive devices, the rectifying junction is referred to as a photovoltaic heterojunction. Types of organic photovoltaic heterojunctions include a donor-acceptor heterojunction formed at an interface of a donor material and an acceptor material, and a Schottky-barrier heterojunction formed at the interface of a photoconductive material and a metal.

0016[0009] In the context of organic materials, the terms "donor" and "acceptor" refer to the relative positions of the Highest Occupied Molecular Orbital ("HOMO") and Lowest Unoccupied Molecular Orbital ("LUMO") energy levels of two contacting but different organic materials. If the HOMO and LUMO energy levels of one material in contact with another are lower, then that material is an acceptor. If the HOMO and LUMO energy levels of one material in contact with another are higher, then that material is a donor. It is energetically favorable, in the absence of an external bias, for electrons at a donor-acceptor junction to move into the acceptor material. [0010] As used herein, a first HOMO or LUMO energy level is "greater than" or

0017"higher than" a second HOMO or LUMO energy level if the first energy level is closer to the vacuum energy level. A higher HOMO energy level corresponds to an ionization potential ("EP") having a smaller absolute energy relative to a vacuum level. Similarly, a higher LUMO energy level corresponds to an electron affinity ("EA") having a smaller absolute energy relative to vacuum level. On a conventional energy level diagram, with the vacuum level at the top, the LUMO energy level of a material is higher than the HOMO energy level of the same material.

0018[0011] After absorption of a photon in the material creates an exciton, the exciton dissociates at the rectifying interface. A donor material will transport the hole, and an acceptor material will transport the electron.

0019[0012] A significant property in organic semiconductors is carrier mobility.

0020Mobility measures the ease with which a charge carrier can move through a conducting material in response to an electric field. In the context of organic photosensitive devices, a material that conducts preferentially by electrons due to high electron mobility may be referred to as an electron transport material. A material that conducts preferentially by holes due to a high hole mobility may be referred to as a hole transport material. A layer that conducts preferentially by electrons, due to mobility and/or position in the device, may be referred to as an electron transport layer ("ETL"). A layer that conducts preferentially by holes, due to mobility and/or position in the device, may be referred to as a hole transport layer ("HTL"). Preferably, but not necessarily, an acceptor material is an electron transport material and a donor material is a hole transport material. [0013] How to pair two organic photoconductive materials to serve as a donor and an acceptor in a photovoltaic heterojunction based upon carrier mobilities and relative HOMO and LUMO levels is well known in the art, and is not addressed here. [0014] As used herein, the term "organic" includes polymeric materials as well as small molecule organic materials that may be used to fabricate organic opto-electronic devices. "Small molecule" refers to any organic material that is not a polymer, and "small molecules" may actually be quite large. Small molecules may include repeat units in some circumstances. For example, using a long chain alkyl group as a substitute does not remove a molecule from the "small molecule" class. Small molecules may also be incorporated into polymers, for example as a pendent group on a polymer backbone or as a part of the backbone. Small molecules may also serve as the core moiety of a dendrimer, which consists of a series of chemical shells built on the core moiety. The core moiety of a dendrimer may be a fluorescent or phosphorescent small molecule emitter. A dendrimer may be a "small molecule." In general, a small molecule has a defined chemical formula with a molecular weight that is the same from molecule to molecule, whereas a polymer has a defined chemical formula with a molecular weight that may vary from molecule to molecule. As used herein, "organic" includes metal complexes of hydrocarbyl and heteroatom-substituted hydrocarbyl ligands. [00151 An organic photosensitive device comprises at least one photoactive region in which light is absorbed to form an exciton, which may subsequently dissociate into an electron and a hole. The photoactive region will typically comprise a donor- acceptor heterojunction, and is a portion of a photosensitive device that absorbs electromagnetic radiation to generate excitons that may dissociate in order to generate an electrical current.

0021[0016] Organic photosensitive devices may incorporate electron blocking layers

0022(EBLs). EBLs are described in U.S. Patent No. 6,451,415 to Forrest et al., which is incorporated herein by reference for its disclosure related to EBLs. EBLs (among other things) reduce quenching by preventing excitons from migrating out of the donor and/or acceptor materials. It is generally believed that the EBLs derive their exciton blocking property from having a LUMO-HOMO energy gap substantially larger than that of the adjacent organic semiconductor from which excitons are being blocked. Thus, the confined excitons are prohibited from existing in the EBL due to energy considerations. While it is desirable for the EBL to block excitons, it is not desirable for the EBL to block all charge. However, due to the nature of the adjacent energy levels, an EBL may block one sign of charge carrier. By design, an EBL will exist between two other layers, usually an organic photosensitive semiconductor layer and an electrode or a charge transfer layer. The adjacent electrode or charge transfer layer will be in context either a cathode or an anode. Therefore, the material for an EBL in a given position in a device will be chosen so that the desired sign of carrier will not be impeded in its transport to, the electrode or charge transfer layer. Proper energy level alignment ensures that no barrier to charge transport exists, preventing an increase in series resistance. [0017] It should be appreciated that the exciton blocking nature of a material is not an intrinsic property of its HOMO-LUMO energy gap. Whether a given material will act as an exciton blocker depends upon the relative HOMO and LUMO energy levels of the adjacent organic photosensitive material, as well upon the carrier mobility and carrier conductivity of the material. Therefore, it is not possible to identify a class of compounds in isolation as exciton blockers without regard to the device context in which they may be used. However, one of ordinary skill in the art may identify whether a given material will function as an exciton blocking layer when used with a selected set of materials to construct an organic PV device. Additional background explanation of EBLs can be found in United States patent application No. 11/810,782 of Barry P. Rand et al., published as 2008/0001144 Al on January 3, 2008, the disclosure of which is incorporated herein by reference, and Peumans et al., "Efficient photon harvesting at high optical intensities in ultrathin organic double-heterostructure photovoltaic diodes," Applied Physics Letters 76, 2650-52 (2000).

0023[0018] The terms "electrode" and "contact" are used interchangeably herein to refer to a layer that provides a medium for delivering photo-generated current to an external circuit or providing a bias current or voltage to the device. Electrodes may be composed of metals or "metal substitutes^" Herein the term "metal" is used to embrace both materials composed of an elementally pure metal, and also metal alloys which are materials composed of two or more elementally pure metals. The term "metal substitute" refers to a material that is not a metal within the normal definition, but which has the metal-like properties such as conductivity, such as doped wide-bandgap semiconductors, degenerate semiconductors, conducting oxides, and conductive polymers. Electrodes may comprise a single layer or multiple layers (a "compound" electrode), may be transparent, semi-transparent, or opaque. Examples of electrodes and electrode materials include those disclosed in U.S. Patent No. 6,352,777 to Bulovic et al., and U.S. Patent No. 6,420,031, to Parthasarathy, et al., each incorporated herein by reference for disclosure of these respective features. As used herein, a layer is said to be "transparent" 9 041816

0024if it transmits at least 50% of the ambient electromagnetic radiation in a relevant wavelength.

0025[0019] The functional components of organic photosensitive devices are usually very thin and mechanically weak, and therefore the devices are typically assembled on the surface of a substrate. The substrate may be any suitable substrate that provides desired structural properties. The substrate may be flexible or rigid, planar or non-planar. The substrate may be transparent, translucent or opaque. Rigid plastics and glass are examples of preferred rigid substrate materials. Flexible plastics and metal foils are examples of preferred flexible substrate materials.

0026[0020] Organic donor and acceptor materials for use in the photoactive region may include organometallic compounds, including cyclometallated organometallic compounds. The term "organometallic" as used herein is as generally understood by one of ordinary skill in the art and as given, for example, in Chapter 13 of "Inorganic Chemistry" (2nd Edition) by Gary L. Miessler and Donald A. Tarr, Prentice Hall (1999). [0021] Organic layers may be fabricated using vacuum deposition, spin coating, organic vapor-phase deposition, organic vapor jet deposition, inkjet printing and other methods known in the art.

0027[0022] Donor and acceptor layers may meet at a bilayer, forming a planar heterojunction. A hybrid or mixed heterojunction comprises a mixture of donor and acceptor materials, arranged between layers of donor material and acceptor material. A bulk heterojunction, in the ideal photocurrent case, has a single continuous interface between the donor material and the acceptor material, although multiple interfaces typically exist in actual devices. Mixed and bulk heteroj unctions can have multiple donor-acceptor interfaces as a result of having plural domains of material. Domains that are surrounded by the opposite-type material (e.g., a domain of donor material surrounded by acceptor material) may be electrically isolated, such that these domains do not contribute to photocurrent. Other domains may be connected by percolation pathways (continuous photocurrent pathways), such that these other domains may contribute to photocurrent. The distinction between a mixed and a bulk heterojunction lies in degrees of phase separation between donor and acceptor materials. In a mixed heterojunction, there is very little or no phase separation (the domains are very small, e.g., less than a few nanometers), whereas in a bulk heterojunction, there is significant phase separation (e.g., forming domains with sizes of a few nanometers to 100 nm). Isolated carbon nanotubes act as individual domains, and if present in sufficient concentrations may give rise to percolation pathways.

0028[0023] Small-molecule mixed heterojunctions may be formed, for example, by co-deposition of the donor and acceptor materials using vacuum deposition or vapor deposition. Small-molecule bulk heterojunctions may be formed, for example, by controlled growth, co-deposition with post-deposition annealing, or solution processing. Polymer mixed or bulk heterojunctions may be formed, for example, by solution processing of polymer blends of donor and acceptor materials.

0029[0024] In general, planar heterojunctions have good carrier conduction, but poor exciton dissociation; a mixed layer has poor carrier conduction and good exciton dissociation, and a bulk heterojunction has good carrier conduction and good exciton dissociation, but may experience charge build-up at the end of the material "cul-de-sacs," lowering efficiency. Unless otherwise stated, planar, mixed, bulk, and hybrid heterojunctions may be used interchangeably as donor-acceptor heterojunctions throughout the embodiments disclosed herein.

0030[0025] The photoactive region may be part of a Schottky-baπier heterojunction, in which a photoconductive layer forms a Schottky contact with a metal layer. If the photoconductive layer is an ETL, a high work function metal such as gold may be used, whereas if the photoconductive layer is an HTL, a low work function metal such as aluminum, magnesium, or indium may be used. In a Schottky-barrierjCell, a built-in electric field associated with the Schottky barrier pulls the electron and hole in an exciton apart. Generally, this field-assisted exciton dissociation is not as efficient as the dissociation at a donor-acceptor interface.

0031[0026] The devices may be connected to a resistive load which consumes or stores power. If the device is a photodetector, the device is connected to a current- detecting circuit which measures the current generated when the photodetector is exposed to light, and which may apply a bias to the device (as described for example in Published U.S. Patent Application 2005-0110007 Al₁ published May 26, 2005 to Forrest et al.). If the rectifying junction is eliminated from the device (e.g., using a single photoconductive material as the photoactive region), the resulting structure may be used as a photoconductor cell, in which case the device is connected to a signal detection circuit to monitor changes in resistance across the device due to the absorption of light. Unless otherwise stated, each of these arrangements and modifications may be used for the devices in each of the drawings and embodiments disclosed herein. [0027] ^' An organic photosensitive optoelectronic device may also comprise transparent charge transfer layers, electrodes, or charge recombination, zones. A charge transfer layer may be organic or inorganic, and may or may not be photoconductively active. A charge transfer layer is similar to an electrode, but does not have an electrical connection external to the device and only delivers charge carriers from one subsection of an optoelectronic device to the adjacent subsection. A charge recombination zone is similar to a charge transfer layer, but allows for the recombination of electrons and holes between adjacent subsections of an optoelectronic device. A charge recombination zone may include semi-transparent metal or metal substitute recombination, centers comprising nanoclusters, nanoparticles, and/or nanorods, as described for example in U.S. Patent No. 6,657,378 to Forrest et al.; Published U.S. Patent Application 2006-0032529 Al, entitled "Organic Photosensitive Devices" by Rand et al., published February 16, 2006; and Published U.S. Patent Application 2006-0027802 Al, entitled "Stacked Organic Photosensitive Devices" by Forrest et al., published February 9, 2006; each incorporated herein by reference for its disclosure of recombination zone materials and structures. A charge recombination zone may or may not include a transparent matrix layer in which the recombination centers are embedded. A charge transfer layer, electrode, or charge recombination zone may serve as a cathode and/or an anode of subsections of the optoelectronic device. An electrode or charge transfer layer may serve as a Schottky contact.

0032[0028] For additional background explanation and description of the state of the art for organic photosensitive devices, including their general- construction, characteristics, materials, and features, U.S. Patent Nos. 6,972,431, 6,657,378 and 6,580,027 to Forrest et al., and U.S. Patent No. 6,352,777 to Bulovic et al., are incorporated herein by reference in their entireties. [0029] The discovery in 1992 of photoinduced charge transfer between conjugated polymers and fullerenes (KS. Sariciftci et al., Proc. SPLE, 1852:297-307 (1993)) has inspired a great deal of research into the possible use of fullerenes in photovoltaic and photoelectric devices. This led to the fabrication of several photovoltaic systems that employ a combination of polymer and fullerenes. It has been found that fullerenes can be susceptible to photooxidation. The observation of photoinduced electron transfer at a multi-wall carbon nanotube-conjugated polymer interface (H. Ago et al., Phys. Rev. B, 61:2286 (2000)) has inspired attempts to use carbon nanotubes (CNTs) and in particular single-walled carbon nanotubes (SWNTs) as electron acceptor materials in photovoltaic devices.

0033[0030] The first reported use of CNTs as electron acceptors in a bulk- heteroj unction photovoltaic cell was a blend of SWNTs with polythiophenes, in which an increase in photocurrent of two orders of magnitude was observed (E. Kymakis, G.A.J. Amaratunga, Appl. Phys, Lett. 80:112 (2002)). In 2005, a photovoltaic effect was observed in an isolated SWNT illuminated with 1.5 μm (0.8 eV) radiation (J.U. Li, Appl. Phys. Lett. 87:073101 (2005)).

0034[0031] Kymakis (E. Kymakis and G. Amaratunga, Rev. Adv. Mat Sci. 10:300-

0035305 (2005,) has described the use of carbon nanotubes as electron acceptors in a polymeric photovoltaic system based on poly (3-octylthiophene). In this system, the nanotubes serve as electron acceptors and electron conductors; the photocurrent declines at CNT concentrations greater than about 1%, and the authors concluded that the nanotubes do not contribute to the photocurrent.

0036[0032] Ajayan et al., (U.S. Patent Application Publication No. 2006/0272701 ) have described the use of SWNTs as the electron-transporting component in a photovoltaic device, using covalently attached organic dyes as the photo-responsive component. More recently, Mitra et al., have similarly employed SWNTs as the electron- txansporting component in a photovoltaic device based on Cgo-organic semiconductor heterojunctions (C. Li. et al., J. Mater. Chem. 17, 2406 (2007); C. Li and S. Mitra, Appl. Phys. Lett. 91, 253112 (2007)). These devices employ SWNTs as electron-accepting and electron-conducting elements. Previous workers have noted mat the metallic SWNTs in these devices provide short-circuit pathways for the recombination of holes and electrons, and have speculated that the devices would be more efficient if isolated semiconducting SWNTs were employed (E. Kymakis et al., J. Phys. D: Appl. Phys. 39, 1058-1062 (2006); M. Vignali et al., http://re.jrc.cec.eu.int/solarec/publications/paris polymer.pdf (undated)). However, the use of semiconducting SWNTs in such designs employ the SWNTs as electron-accepting and electron-conducting elements only, rather than as sources of photogenerated excitons. The existing and proposed devices do not take advantage of the photoelectric properties of semiconducting SWNTs.

0037[0033] Currently, all synthetic methods for growing SWNTs result in heterogeneous mixtures of SWNTs that vary in their structural parameters (length, diameter, and chiral angle), and consequently have variations in their electronic and optical properties (e.g., conductivity, electrical band gap, and optical band gap) (M. S. Arnold, A. A. Green, J. F. Hulvat et al., NatureNanotech. 1(1), 60 (2006); M. S. Arnold, S. I. Stupp, and M. C. Hersam, Nano Letters 5 (4), 713 (2005); R. H. Baughman, A. A. Zakhidov, and W. A. de Heer, Science 297 (5582), 787 (2002). All reported CNT-based photovoltaic devices reported to date employ these mixtures. [0034] Recent advances include fabrication methods for CNT thin films on various substrates such as (polyethylene terephthalate (PET), glass, polymethylmethacrylate) (PMMA), and silicon (Y. Zhou, L. Hu, G. Griiner, Appl. Phys. Lett. 88:123109 (2006)). The method combines vacuum filtration generation of CNT mats with a transfer-printing technique, and allows controlled deposition and patterning of large area, highly conducting CNT films with high homogeneity. Such films are a potential alternative to the commonly-used hole-collecting electrode material, indium-tin oxide (ITO), which is expensive and remains incompatible with roll-to-roll fabrication processing.

0038[0035] The properties of carbon nanotubes are influenced mostly by the diameter of the tube and the degree of twist. Both aligned tubes and tubes with a twist can be metallic or semiconducting, depending on whether the energy states in the circumferential direction pass through what is termed a Fermi point. At Fermi points, the valence and conduction bands meet, which allows for conduction in the circumferential direction of the tube. Tubes that have the correct combination of diameter and chirality will possess a set of Fermi points around the perimeter of their grid structures throughout the length of the tube. These tubes will show metallic like conduction. If the diameter and chirality do not generate a set of Fermi points, the tube will exhibit semiconducting behavior (P. Avouris, Chemical Physics, 281: 429-445 (2002)).

0039[0036] In addition to Fermi point matchups, the cylindrical shape and diameter of the tube affects electron transport through the way in which quantum states exist around the tube perimeter. Small diameter tubes will have a high circumferential band gap with a low number of energy states available. As the tube diameter increases, the number of energy states increases and the circumferential band gap decreases. In general, the band gap is inversely proportional to the tube diameter.

0040[0037] Furthermore, the wave properties of electrons are such that standing waves can be set up radially around a carbon nanotube. These standing waves, the lack of conduction states in small diameter tubes, and the monolayer thickness of the graphite sheet, combine to inhibit electron motion around the tube perimeter and force electrons to be transported along the tube axis.

0041[0038] If a Fermi point matchup is present, however, electron transport can occur around the tube perimeter, in addition to axial conduction, allowing for increased transport options of the electron and metallic conduction characteristics. As the tube diameter increases, more energy states are allowed around the tube perimeter and this also tends to lower the band gap. Thus, when only axial conduction is allowed, the tube exhibits semiconducting behavior. When both axial and circumferential conduction are allowed, the tube exhibits metallic conduction.

0042[0039] The power output of existing organic photovoltaic devices is not yet competitive with traditional silicon-based photovoltaic devices. In addition to being less efficient and like other thin-film approaches, they are susceptible to oxidative degradation when exposed to air, and need encapsulation. Given the cost and fragility of silicon solar cells, and the promise of easily-fabricated and inexpensive organic equivalents, there remains a need for more efficient and more stable organic photovoltaic and photoelectric devices. Also, because of organic materials' poor sensitivity to IR and near-IR radiation, there remains a need for organic photovoltaic materials capable of efficiently producing excitons upon irradiation by ER and NIR radiation. [0040] Semiconducting CNTs, despite their strong near-IR band gap absorption, have only had limited impact as the optically absorptive components of optoelectronic devices because of the strong binding energy of photogenerated electron-hole pairs.

SUMMARY

0044[0041] The present disclosure provides photoelectric and photovoltaic devices in which semiconducting carbon nanotubes serve as organic photoconductive materials, i.e. as the light-harvesting component. In particular, the present disclosure describes the use of carbon nanotubes as a material for detection of IR radiation in thin film device architecture. In these devices, semiconducting carbon nanotubes act as electron donors and separation of the photogenerated charges takes place at a heteroj unction between the semiconducting carbon nanotubes and an organic semiconductor. Appropriate selection of the diameter and optical band gaps of the semiconducting carbon nanotubes may be used to vary the responsivity of the photovoltaic device from the visible to the near- infrared region of the spectrum. Representative materials, device architectures, and procedures for fabricating the architectures are outlined herein.

0045[0042] According to an embodiment of the present disclosure, at least one or both of the organic acceptor and donor layers in the photoactive region of the photovoltaic device includes carbon nanotubes. The present disclosure describes the use of carbon nanotubes as optically active components of large-area optoelectronic devices. [0043] In one embodiment, a photovoltaic device comprises a first electrode, a second electrode, and a photoactive region disposed between and electrically connected to the ^"first electrode and the second electrode. The photoactive region further comprises a donor layer formed above the first electrode, and an acceptor layer formed above the donor layer such that the donor layer and the acceptor layer form a donor-acceptor heterojunction, wherein either the acceptor layer or the donor layer comprises a layer of polymer-wrapped carbon nanotubes.

0046[0044] In another embodiment, a photovoltaic device comprises a first electrode, a donor layer formed above the first electrode, a bulk heterojunction formed above the donor layer, wherein the bulk heterojunction comprises polymer-wrapped carbon nanotubes disposed within an organic electron acceptor. An acceptor layer is formed above the bulk heterojunction, and a second electrode is formed above the acceptor layer. Either the acceptor layer or the donor layer can comprise a layer of polymer-wrapped carbon nanotubes.

0047[0045] The inventors have discovered that excitons (bound electron-hole pairs) in

0048CNTs can be efficiently dissociated by interfacing CNTs with the electron acceptor such as evaporated Cgo- The two fullerene-based materials form a donor-acceptor heterojunction with band/orbital offsets that are sufficient to result in electron transfer from the CNTs to evaporated Ceo- The combination of the visible absorptivity of the organic semiconductors and the near-IR absorptivity of the CNTs results in broadband sensitivity to electromagnetic illumination varying from 400-1400 run in wavelength.

BRIEF DESCRPTION OF THE DRAWINGS

0050[0046] FIGs. IA and IB illustrate the architectures of planar heterojunction embodiments of the present disclosure.

0051[0047] FIGs. 2A-2D illustrate the architectures of bulk heterojunction embodiments of the present disclosure.

0052[0048] FIGs. 3 A and 3B illustrate the architectures of additional bulk heterojunction embodiments of the present disclosure.

0053[0049] FIG. 4 shows the architecture of a planar heterojunction formed by depositing a carbon nanotube film onto PTCDA (3,4,9,10-perylene-tetracarboxyl-bis- dianhydride).

0054[0050] FIG. 5 shows the current- voltage curve of the heterojunction in the dark and illuminated with simulated solar near-IR radiation.

0055[0051] FIG. 6 shows the conduction band (CB) and valence band (VB) energies of CNTs for different absorption wavelengths as well as the necessary energies for acceptable donors or acceptors.

0056[0052] FIG. 7 shows the photoluminescence of polymer- wrapped carbon nanotubes suspended in toluene, excited at 650 ran.

0057[0053] FIG. 8 shows photoluminescence intensity of thick films containing PFO and CNTs doctor bladed from toluene solution. [0054] FIG. 9A shows an example of architecture of a polymer-wrapped carbon nanotube/C₆o heterojunction diode with a 1:1 ratio of MDMO-PPV to nanotubes, by weight.

0058[0055] FIG. 9B shows the current- voltage characteristics of the device of FIG.

00599A.

0060[0056] FIG. 9C shows the spectrally resolved photoresponsivity of the device of

0061FIG. 9A.

0062[0057] FIG. 9D shows the internal quantum efficiency (IQE) of the device of

0063FIG. 9A and absorptivity of polymer wrapped carbon nanotubes. [0058] FIG. 1OA is a schematic energy level diagram for a polymer wrapped carbon nanotube/Ceo heterojunction according to an embodiment of the present disclosure.

0064[0059] FIGs. 1OB and 1OC are schematic energy level diagrams of two control devices.

0065[0060] FIG. HA shows another example of an architecture of a polymer- wrapped carbon nanotube/Coo heterojunction diode with a 1:1 ratio of MDMO-PPV to nanotubes, by weight.

0066[0061] FIG. HB shows the current-voltage characteristics of the device of FIG.

0067HA.

0068[0062] FIG. HC shows the spectrally resolved photoresponsivity of the device of

0069FIG. HA.

0070[0063] FIG. HD shows the internal quantum efficiency (IQE) of the device of

0071FIG. HA and absorptivity of polymer wrapped carbon nanotubes. [0064] The features shown in the above referenced drawings are illustrated schematically and are not intended to be drawn to scale nor are they intended to be shown in precise positional relationship. Like reference numbers indicate like elements.

DETAILED DESCRIPTION

0073[0065] In the following detailed description of the preferred embodiments, reference is made to the accompanying drawings which form a part hereof, and in which are shown by way of illustration specific embodiments in which the invention may be practiced. It is to be understood that other embodiments may be utilized and structural changes may be made without departing from the scope of the present invention. [0066] An organic photosensitive optoelectronic device according to an embodiment of the present disclosure can be used, for example, to detect incident electromagnetic radiation particularly electromagnetic radiation in the IR and near-IR spectrum or as a solar cell to generate power. Embodiments of the present invention may comprise an anode, a cathode, and a photoactive region between the anode and the cathode, wherein semiconducting polymer-wrapped carbon nanorαbes and an organic semiconductor form a heterojunction within the photoactive region. The photoactive region is the portion of the photosensitive device that absorbs electromagnetic radiation to generate excitons that may dissociate in order to generate an electrical current. Organic photosensitive optoelectronic devices may also include at least one transparent electrode to allow incident radiation to be absorbed by the device.

0074[0067] An efficient photosensitive optoelectronic device formed of carbon nanotubes contains compounds with proper energies such that the exciton created by absorption of a photon by a carbon nanotube is split into a free electron and a free hole. To efficiently split the exciton, the HOMO of the donor material should be higher in energy (less negative) than the valance band (VB) of the carbon nanotube-based acceptor. Or conversely, the LUMO of the acceptor material must be less than (more negative) than the conduction band (CB) of the carbon nanotube-based donor. The CB and VB energies as well as the necessary energies for acceptable donors or acceptors are shown in FIG. 6 (see R.B. Weisman, et al. NANO LETT 3 (2003)).

0075[0068] As used herein, the term "rectifying" denotes, inter alia, that an interface has an asymmetric conduction characteristic, i.e., the interface supports electronic charge transport preferably in one direction. The term "semiconductor" denotes materials which can conduct electricity when charge carriers are induced by thermal or electromagnetic excitation. The term "photoconductive" generally relates to the process in which electromagnetic radiant energy is absorbed and thereby converted to excitation energy of electric charge carriers so that the carriers can conduct (Le., transport) electric charge in a material. The term "photoconductive material" refers to semiconductor materials which are utilized for their property of absorbing electromagnetic radiation to generate electric charge carriers. As used herein, "top" means furthest away from the substrate, while "bottom" means closest to the substrate. There may be intervening layers (for example, if a first layer is "on" or "over" a second layer), unless it is specified that the first layer is "in physical contact with" or "directly on" the second layer; however, this does not preclude surface treatments (e.g., exposure of the first layer to hydrogen plasma). [0069] Referring to FIGs. IA and IB, architectures of two planar heterojunction embodiments for a photovoltaic device IOOA and IOOB are disclosed. The photovoltaic device IOOA comprises a conducting anode layer HOA, an electron donor layer 120A formed above the anode layer HOA, an electron acceptor layer 130A formed above the donor layer 120A and a conducting cathode layer 150A formed above the electron acceptor layer 130A. In this embodiment, a thin film of polymer- wrapped carbon nanotubes form the electron donor layer 120A. A planar heterojunction is formed between the electron donor layer 120A and the electron acceptor layer 130A. The electron donor layer 120A and the electron acceptor layer 130A form the photoactive region 122A of the device IOOA. Preferably, the polymer-wrapped carbon nanotubes (PW-CNTs) are substantially semiconducting polymer-wrapped single-wall carbon nanotubes (PW-SWNTs). Although PW-SWNTs are preferred, polymer-wrapped carbon nanotubes including multi-walled carbon nanotubes are within the scope of the invention disclosed herein. Therefore, in the various embodiments presented herein, when PW- SWNTs are mentioned in connection with a PV device, those embodiments are, only examples and other embodiments using PW-CNTs generally, including polymer-wrapped multi- walled carbon nanotubes, are within the scope of the present disclosure. [0070] When the PW-CNTs are used as the electron donor, suitable organic semiconductors for forming the electron acceptor layer 130A include, but are not limited to, evaporated C₆o having a LUMO of -4.0 eV, [84]PCBM ([6,6]-Phenyl C₈₄ butyric acid methyl ester) having a LUMO of -4.1 eV, F16-CuPc having a LUMO of -4.4 eV, PTCBI (3,4,9,10 perylenetetracarboxylic bisbenzimidazole) having a LUMO of -4.0 eV, PTCDA (3,4,9,10 perylene-tetracarboxylic dianhydride) having a LUMO of -4.7 eV, or Poly(benzimidazόbenzo phenanthroline) havbg a LUMO of -4.5 eV, TCNQ (7,7,8,8- tetracyanoquinodimethane) having a LUMO of 3.9 eV, F4-TCNQ (tetrafluorotetracyanoquinodimethane) having a LUMO of 5.2 eV, and the like. [0071] The organic semiconductor for the electron acceptor layer 130A is preferably capable of efficiently delivering the electrons to the cathode 150A, or to an electron transport layer. These suitable organic semiconductors for the electron acceptor layer 130A typically have a LUMO of lower energy than the LUMO of the carbon nanotubes, so that electron transfer from the irradiated carbon nanotubes (preferably PW- SWNTs) is rapid and irreversible.

0076[0072] There are many different organic semiconductors that could form a rectifying heteroj unction with semiconducting PW-CNTs, which results in charge separation and charge transfer of photogenerated charge and a photovoltaic effect. For a CNT with an optical band gap of 1 eV and an exciton binding energy of 0.5 eV, the expected HOMO-LUMO or electrical band gap would be 1.5 eV. Assuming a p-type doping and taking 4.6 eV as the work-function (see calculations of V. Barone, J. E. Peralta, J. Uddin et al., J, Chem. Phys. 124(2) (2006)), the LUMO or conduction band would sit at 3.5 eV with reference to vacuum while the HOMO or valence band would sit at 5.0 eV from vacuum. Thus, such a semiconducting PW-CNT would form a rectifying heteroj unction with evaporated Ceo as the electron acceptor.

0077[0073] As noted above, the exact band energy levels of semiconducting CNTs depend on their diameter, chiral twist, electrical band gap, optical band gap, local dielectric environment, and doping. Thus, semiconducting CNTs can serve as either electron accepting material or electron donating material in a heterojunction with another organic semiconductor, depending on the structure of the nanotube and the properties of the organic semiconductor. In addition to small molecule organic semiconductors, conducting polymers could be utilized as either an electron accepting or electron donating materials as well.

0078[0074] In the embodiment shown in FIG. IB, the photovoltaic device IOOB comprises a conducting anode layer HOB, an electron donor layer 120B formed above the anode layer HOB, an electron acceptor layer 130B, and a conducting cathode layer 150B. In this embodiment, a thin film of polymer- wrapped carbon nanotubes form the electron acceptor layer 130B. A planar heterojunction is formed between the electron donor layer 120B and the electron acceptor layer 130B. The electron donor layer 120B and the electron acceptor layer 130B form the photoactive region 122B of the device 10OB.

0079[0075] Preferably, the polymer-wrapped carbon nanotubes are substantially semiconducting PW-SWNTs. Carbon nanotubes may be single-walled or multi-walled. Multi- walled nanotubes contain multiple layers of graphite arranged concentrically in a tube. Generally, SWNTs exhibit better electrical properties than multi-walled nanotubes. SWNTs commercially available in bulk quantity are generally manufactured using either a high-pressure carbon monoxide (HiPCO®) process (such as HiPCO® nanotubes available from Unidym of Menlo Park, California, U.S.A.) or an arc-discharge process (such as P3 nanotubes from Carbon Solutions Inc., which are purified arc-discharge nanotubes with two open ends linked with hydrophilic carboxyl groups). [0076] As used herein, "substantially semiconducting PW-SWNTs" refer to populations of PW-SWNTs in which at least 80% by weight of the nanotubes are of the semiconducting variety, i.e. non-metallic. It will be appreciated that as the fraction of conducting nanotubes is reduced, the density of nanotubes in the photoactive regions of the photodetecting devices may be increased while maintaining a very low probability of percolating conducting paths. Accordingly, in preferred embodiments, at least 90% of the nanotubes are of the semiconducting variety, and in more preferred embodiments, at least 95% are of the semiconducting variety. In the most preferred embodiments, at least 99% of the nanotubes are of the semiconducting variety.

0080[0077] In a typical CNT mixture, one third of CNTs are metallic in nature while the remaining two thirds are semiconducting, with optical and electrical band gaps that roughly vary inversely with diameter. This heterogeneity presents an obstacle to the fabrication of efficient photovoltaic solar cells from as-produced CNT mixtures, due to excitonic quenching and nonrectifying electrical paths associated with the presence of metallic CNTs. Isolated semiconducting carbon nanotube preparations are necessary to create an efficient organic-semiconductor-semiconducting carbon nanotube heterojunction photovoltaic solar cell. At present, the only way to isolate semiconducting SWNTs is via post-synthesis processing methods.

0081[0078] Currently, a few such processing methods exist for enriching or isolating semiconducting CNTs on the laboratory scale. These methods include "constructive destruction" (P.C. Collins, M.S. Arnold, and P. Avouris, Science 292(5517), 706 (2001)); selective etching of metallic CNTs in monolayer thin films (G. Y. Zhang, P. F. Qi, X.R. Wang et al., Science 314(5801), 974 (2006)); field-flow fractionation based on dielectrophoresis (H.Q. Peng, N.T. Alvaret, C. Kittrell et al., J. Amer. Chem. Soc. 128(26), 8396 (2006)); and anion exchange chromatography of DNA-wrapped CNTs (M. Zheng, A. Jagota, M.S. Strano et al., Science 302(5650), 1545-1548 (2003)). However, the effectiveness of many of these techniques (the proportion of obtained CNTs that are semiconducting) is limited or unclear, and there are significant drawbacks to these techniques that render them impractical for producing usable quantities of semiconducting CNTs.

0082[0079] When the PW-CNTs are used as the electron acceptors, suitable organic semiconductors for forming the electron donor layer-120B include, but are not limited to, BTEM-PPV (Poly(2,5-bis(l,4,7,10-tetraoxaundecyl)- 1,4-phenylenevinylene) having a HOMO of -4.97 eV, Poly(3-decyloxythiophene) having a HOMO of -4.5 eV, CuPc (copper phthalocyanine) having a HOMO of 5.3 eV, NPD (4,4 '-Hs(N-(I- napthyl)phenylamino)biphenyl) having a HOMO of 5.4eV, pentacene having a HOMO of 5.0 eV, tetracene having a HOMO of 5.4 eV, and the like. The organic semiconductor for the electron donor layer 120B should be capable of efficiently delivering the holes to the anode HOB, or to a hole transport layer. The suitable organic semiconductors for the electron donor layer 120B are preferably those having a HOMO of higher energy than the HOMO of the carbon nanotubes, so that hole transport from (electron transfer to) the irradiated CNTs is rapid and irreversible.

0083[0080] In both embodiments IOOA and 10OB, an optional exciton blocking layer

0084140A, 140B can be provided between the photoactive regions 122A, 122B and the cathode layers 150A, 150B, respectively. Additionally, an optional exciton blocking layer 115A, 115B can be provided between the photoactive regions 112A, 122B and the anode layers HOA, HOB, respectively. An anode-smoothing layer may also be situated between the anode and the donor. Anode-smoothing layers are described in U.S. Patent 6,657,378 to Forrest et al., incorporated herein by reference for its disclosure related to this feature Polymer wrapping

0085[0081] The carbon nanotubes, as produced, are highly agglomerated and bundled.

0086To get efficient optical absorption and exciton splitting and to prevent exciton quenching, the tubes must be debundled. This is done through a known polymer wrapping process. The carbon nanotubes are placed into a solution of polymer and the appropriate solvent and the carbon nanotubes are separated using a high-power horn sordcator (cell dismembrator). If an appropriate polymer is used (various poly-thiophene polymer, poly- phenylenevinylene polymer, and poly-fluorene polymer derivatives, amongst others) the polymer will wrap with soluble side-groups on the polymer creating a carbon nanotube- polymer complex that is soluble. The main purpose of the polymer wrapping is to suspend individual nanotubes. A polymer that will form a donor-acceptor heterojunction with the carbon nanotubes so as to facilitate the splitting of the exciton is not necessary for the wrapping material, as long as another material is present in the device that can form a donor-acceptor heterojunction with the PW-CNTs. [0082] After the carbon nanotubes are polymer wrapped and solubilized, a photovoltaic device can be made by incorporating them into a donor or acceptor molecule or polymer, if needed, and casting into a device. To create a photovoltaic device with sufficient carbon nanotubes to absorb an appreciable amount of light may require a high enough concentration of carbon nanotubes that create a percolating network (greater than ~1 % by weight carbon nanotubes in the film). This means that any metallic carbon nanotubes that touch a semiconducting carbon nanotube will act as an exciton quenching center and will drastically reduce the efficiency of the photovoltaic device. Also, the metallic carbon nanotubes could act to short out the device by creating metal fibers that traverse the entire cell thickness leading to a reduced shunt resistance. To avoid this phenomenon, the carbon nanotubes are sorted by a method, such as density gradient ultracentrifugation, so that nearly all of the metallic carbon nanotubes are removed and the exciton quenching is significantly reduced.

0087[0083] In some embodiments, photoactive polymers such as poly[2-methoxy-5-

0088(3 \7'-dimethyloctyloxy)- 1 ,4-phenylenevinylene] (MDMO-PPV), poly[2-methoxy-5-(2'- ethyl-hexyloxy)-l,4-phenylene vinylene] (MEH-PPV) and poly(9,9-dioctylfluorenyl-2,7- diyl) (PFO) can be used to wrap and solubilize the carbon nanotubes. In such embodiments, the photoactive polymers wrapping the CNTs absorb light creating excitons that are separated at the wrapping polymer-to-carbon nanotube or wrapping polymer-to-organic (donor or acceptor) interface independent of the CNTs. [0084] Other examples of photoactive polymers that can be used to wrap the

0089SWNTs are PFO: Poly(9,9-dioctylfluorenyl-2,7-diyl) and polymers with the same backbone and different solublizing groups such as or PFH--Poly(9^',9-dihexylfluorenyl- 2,7-diyl) or Poly[9,9-di-(2-ethylhexyl)-fluorenyl-2,7-diyl]. Another extension is that sometimes copolymers can be used (alternating between PFO and another monomer such as Poly[(9,9-dioctylfluorenyl-2₎7-diyl)-alt-(l ,4-vinylenephenylene)], Poly[(9,9- diocrylfluorenyl-2,7-diyl)-alt-(vinyleneanthracene)] , or Poly[9,9-dioctylfluorenyl-2₅7- diyl)-co- 1 ,4-benzo- {2, l'-3 } -thiadiazole)] .

0090[0085] Another example is phenylenevinylene based polymers: such as MDMO-

0091PPV~Poly[2-methoxy-5-(3,7-dimethyl-octyloxy)-l ,4-phenylenevinylene) or MEH-PPV-- Poly[2-methoxy-5-(2-ethyl-hexyloxy)-l,4-phenylenevinylene] and polymers with the same backbone and different solublizing groups such as poly[2,5-bis(3,7- dimethyloctyloxy)- 1,4-phenylene-vinylene]. Sometimes .backbone' alternates such as copolymers can be used (alternating between PFO and- another monomer such as Poly[(9,9-dioctylfluorenyl-2,7-diyl)-alt-(l,4-vinylenephenylene)], Poly[(9,9- dioctylfluorenyl-2,7-diyl)-alt-(vinyleneanthracene)], orPoly[9,9-dioctylfiuorenyl-2,7- diyl)-co- 1 ,4-benzo- {2, 1 '-3 } -thiadiazole)] .

0092[0086] Thiophene based polymers such as P3HT or those using other solublizing groups could be used: P3BT--poly(3-butyl-thiophene-2,5-diyl); P3HT-poly(3-hexyl- thiophene-2,5-diyl); P30T-poly(3-octal-thiophene-2,5-diyl); P3DT-poly(3-decyl- thiophene-2,5-diyl), etc. Sometimes backbone alternates such as copolymers can be used (alternating between PFO and another monomer such as Poly[(9,9-dioctylfluorenyl- 2₎7-diyl)-alt-(l₎4-vinylenephenylene)]_> Poly[(9,9-dioctylfluorenyl-2_>7-diyl)-alt- (vinyleneanthracene)] , or Poly[9,9-dioctylfluorenyl-2,7-diyl)-co- 1 ,4-benzo- {2, l'-3 } - thiadiazole)]. Other conducting polymer backbones such as PPE polymers: Poly(2,5- dioctyl-l,4-ρhenylene), with the same additions and low-bandgap polymers such as poly[2₎6-(4,4-bis-(2-ethylhexyl)-4H-cyclopenta[2,l-b;3,4-b ]-dithiophene)-alt-4₁7- (2,1,3- T/US2009/041816

0093benzothiadiazole)] (PCPDTBT) are also suitable. Variations might be made to the backbone or alternating unit.

0094[0087] FIG. 7 shows the photoluminescence of polymer- wrapped carbon nanotubes suspended in toluene, excited at 650 nm, showing that the wrapping works well with MDMO-PPV, and that for certain carbon nanotube chiralities, PFO gives much brighter photoluminescence. The signal intensity is an indicator of the amount of carbon nanotubes that are individually dispersed. Aggregated and bundled nanotubes show no photoluminescence signal because of quenching due to metallic nanotubes in contact with semiconducting nanotubes. This shows that MDMO is comparable to MEH-PPV in its ability to solubilize carbon nanotubes in toluene. This suggests that minor changes to the side-groups do not significantly alter the wrapping efficiency and that many similar polymers may be used.

0095[0088] MDMO-PPV wrapping imparts solubility to the carbon nanotubes in organic solvents thus facilitating their solution-based processing. The MDMO-PPV was also expected to effectively isolate the carbon nanotubes from one-another, thus niinimizing the direct electronic coupling between the optically active semiconducting nanotubes and any quenching metallic nanotubes.

0096[0089] In the inventors' experiments, the carbon nanotubes were first wrapped by a semiconducting polymer, polyP-me&oxy-S-^V'-dimethyloctyloxy)-!^- phenylenevinylene] (MDMO-PPV). High pressure carbon monoxide (HiPCO) grown nanotubes that varied from 0.7-1.1 nm in diameter were utilized because to insure spectral responsivity extending to 1400 nm in wavelength. The MDMO-PPV wrapped nonotubes were purified by centrifugation in order to remove bundles of nanotubes and insoluble material. The polymer-nanotube mixture was spread over a hot indium tin oxide (ITO)-coated glass substrate via doctor-blading in an inert nitrogen atmosphere. A thin film of evaporated Ceo was thermally evaporated on top of the polymer-nanotube mixture to form the donor-acceptor interface, followed by a 10 nm buffer layer of 2,9- dimethyl-4,7-diphenyl-l,10-phenanthroline (BCP), and then the Ag cathode. [0090] FIG. 8 shows the inventors' experimental results on [84] PCBM that verifies that the theoretical quenching due to the energy levels described in FIG. 6 is relatively accurate. The data shown in FIG. 8 were taken from a thick film doctor bladed from toluene solutions. The film containing PFO and CNTs is a reference for the effect of adding fullerene additives. The addition of [84] PCBM completely quenches all nanotube luminescence in the wavelength probed (950 to 1350 nm when excited at 650 nm), indicating that the [84] PCBM energy level is deeper than the LUMO minus the exciton binding energy, and results in efficient splitting of excitons in the CNTs. This indicates that [84] PCBM is an effective material for splitting excitons on the CNTs. Therefore, [84] PCBM is an effective electron acceptor material to be used in conjunction with the substantially semiconducting PW-CNTs used as the photoconductive material. [0091] Referring to FIGs. 9A-9D, the current-voltage characteristics (FIG. 9B) and spectrally resolved photoresponsivity (FIG. 9C) of a PW-CNT/Cβoheterojunction diode with a 1:1 ratio of MDMO-PPV to nanotubes, by weight, shown in FIG. 9A are depicted. The thickness of the layers in the device are provided in FIG. 9 A. The diodes have rectification ratios of more than four orders of magnitude under dark conditions (FIG. 9B). The forward bias current-voltage characteristics follow the Shockley diode equation with a diode ideality factor of 2.5 and a series resistance of 120Ω. Referring to FIG. 9C, the near-IR responsivity of the diodes at OV bias (plot line 92) and -0.5V bias (plot line 93) is compared with the absorption spectrum of isolated semiconducting CNTs in an aqueous surfactant solution of sodium cholate in de-ionized H₂O (plot line 94). The photoresponsivity is red-shifted by about 40 meV from the solution absorption spectrum but follows the same shape. The peak photoresponsivity of the devices at 1155 nm at a bias of OV (plot line 92) and -0.5V (plot line 93) was about 10 and 17 mA/W, respectively. In comparison, the responsivity of control devices without carbon nanotubes was immeasurable in the near-infrared (<0.1 μA/W).

0097[0092] FIG. 9D is a plot of the internal quantum efficiency (IQE) of the device of

0098FIG. 9 A. (See solid line 95). IQE is the ratio of the photoresponsivity of the device under -0.5V bias (plot line 93 in FIG. 9C) to the near-IR absorbtivity of the PW-CNTs (dashed line 97 in FIG. 9D). The near-IR absorptivity of the PW-CNTs (dashed line 97) was quantified by measuring the spectrally resolved reflectivity of the device and then subtracting the absorption due the ITO. As shown, the peak IQE in the near-IR exceeds about 20% over the broad spectral range of 1000 to 1350 nm. The substantially large IQE indicates that there is a favorable mechanism for exciton dissociation in the devices. [0093] To test the hypothesis that the active/dissociating interface in our device was the PW-CNT/Cβo interface, the inventors fabricated two control device architectures in which the PW-CNT/Cβo interface was broken. The schematic energy diagrams of these structures are shown in FIGs. 1OB and 1OC. In the first control device architecture shown in FIG. 1OB, a 40 nm layer of sub phthalocynine (SubPc) 14 was inserted between the PW-CNT layer 11 and the evaporated C₆O 13 to break the PW-CNT/C₆₀ interface. The HOMO and LUMO energies of SubPc are similar to those in the MDMO-PPV. The second control device architecture was fabricated to test for exciton dissociation within the MDMO-PPV wrapped carbon nanotube layer, itself. In this architecture, the evaporated Ceo layer 13 was removed and a buffer layer of PFO 15 was inserted as a hole transport layer between the ITO and the PW-CNT layer 11 to prevent the nanotubes from directly bridging the anode and cathode. The corresponding energy diagram for the second control device architecture is shown in FIG. 1OC.

0099[0094] Near-IR responsivity originating from the PW-CNTs was not observed in either control device (responsivity <0.1 μA/W) indicating that there was an insufficient driving force for exciton dissociation at the PW-CNT/ITO, PW-CNT/SubPc, and PW- CNT/MDMO-PPV interfaces. Measurable photocurrent in response to near-infrared illumination was only observed when the PW-CNT/Cβo interface was left intact. [0095] FIGs. 1OA - 1OC show the expected energy alignments between the various organic semiconductors and an (8,4) semiconducting PW-CNT. An (8,4) nanotube has a diameter of 0.84 nm and an expected optical band gap in the polymer matrix at 1155 nm. The electron affinity (EA) and ionization potential (IP) of the nanotube were determined from first principles calculations of the nanotube electronic band structure by Spataru et al., Excitonic effects and optical spectra of single- walled carbon nanotubes, Physical Review Letters 92(7) (2004), and Perebeinos et al., Scaling of excitons in carbon nanotubes, Physical Review Letters 92(25) (2004), and of the work function by Barone et al. , Screened exchange hybrid density-functional study of the work function of pristine and doped single-walled carbon nanotubes, Journal of Chemical Physics 124(2) (2006). First principles calculations of the electronic structure of evaporated Ceo shows that an offset of 0.2 eV between the EA of the nanotube and the LUMO of evaporated C$o is expected (see FIGs. 1OA and 10B). For comparison, the 9 041816

0100binding energy of an exciton in an (8,4) semiconducting PW-CNT with a relative dielectric permittivity of 3.5 is expected to be 0.1 eV. Therefore, the energy offset should be sufficient to result in exciton dissociation and charge transfer from the carbon nanotubes to evaporated Ceo.

0101[0096] In contrast, exciton dissociation at the interface of the MDMO-PPV and the carbon nanotubes should not be expected. Rather, it is expected that these two materials will form a straddling type I heterojunction where both the IP and EA of the carbon nanotubes lie within the HOMO and LUMO levels of MDMO-PPV. The existence of a straddling type I heterojunction between MDMO-PPV and carbon nanotubes has been experimentally supported by photoluminescence spectroscopy in which strong photoluminescence from polymer- wrapped semiconducting carbon nanotubes has been observed at the optical band gap of the nanotubes in response to direct optical exciton of the polymer absorption band.

0102[0097] The planar heterojunctions described above can _vbe formed by depositing a thin film of organic semiconductor directly on top of a percolating network of CNTs. An electron transporting and/or exciton blocking layer 140A may optionally be added, followed by deposition of the cathode layer 150A, to produce the photovoltaic device architecture IOOA shown in FIG. IA. Alternatively, a thin film of CNTs can be stamped onto a thin film of an organic donor material deposited on an anode. Deposition of the optional electron transporting and/or exciton blocking layer 140B, followed by the cathode layer 150B, produces the photovoltaic device architecture IOOB shown in FIG. IB.

0103[0098] Thin films of percolating networks of CNTs can be prepared by direct growth, by vacuum filtration through porous membranes, spray-based deposition strategies, spin-coating, layer-by-layer deposition approaches, dielectrophoresis, and evaporation.

0104[0099] FIGs. 2A-2B show two hybrid planar-bulk heterojunction embodiments for a photovoltaic device 200A and 200B. Referring to FIG. 2A, the photovoltaic device 200A comprises a conducting anode layer 210A and a bulk heterojunction layer 220A comprising polymer wrapped carbon nanotubes disposed within an organic electron donor material formed above the anode layer 210A. An electron acceptor layer 230A is formed above the bulk heterojunction layer 220A and a conducting cathode layer 250A formed above the electron acceptor layer 230A. The bulk heterojunction layer 220A and the electron acceptor layer 230A form the photoactive region 222A of the device 200A. Alternatively, the layers 220A and 230 A can be configured such that the polymer wrapped carbon nanotubes in the layer 220A and the electron acceptor material of the layer 230A form a bulk heterojuction.

0105[00100] The suitable organic semiconductor donor materials for forming the bulk heterojunction layer 220A include, but are not limited to, BTEM-PPV (Poly(2,5- bis(l,4,7,10-tetraoxaundecyl> 1,4-phenylenevinylene), Poly(3-decyloxythiophene)., CuPc (copper phthalocyanine), NPD (4,4'-bis(N-(l-napthyl)phenylamino)biphenyl), pentacene, tetracene, and the like. The suitable organic semiconductors for the electron acceptor layer 230A include, but are not limited to, evaporated C₆₀, [84]PCBM ([6,6]-Phenyl C₈₄ butyric acid methyl ester), F16-CuPc, PTCBI (3,4,9JO perylenetetracarboxylic bisbenzimidazole), PTCDA (3,4,9,10 perylene-tetracarboxylic dianhydride), or Poly(benzimidazobenzophenanthroline), TCNQ (7,7,8,8-tetracyanoquinodimethane), F4- TCNQ (tetrafluorotetracyanoquinodimethane), and the like. [00101] Referring to FIG. 2B, the photovoltaic device embodiment 200B comprises a conducting anode layer 210B and an electron donor layer 220B formed above the anode layer 210B. A bulk heterojunction layer 230B comprising polymer wrapped carbon nanotubes is disposed within an organic electron acceptor material formed above the donor layer 220B, and a conducting cathode layer 250B is formed above the-bulk heterojunction layer 230B. The bulk heterojunction layer 230B and the electron donor layer 220B form the photoactive region 222B of the device 200B. [00102] The suitable organic semiconductor acceptor materials for forming the bulk heterojunction layer 230B include, but are not limited to, evaporated C_&o, [84JPCBM ([6,6]-Phenyl C₈₄ butyric acid methyl ester), F16-CuPc, PTCBI (3,4,9,10 perylenetetracarboxylic bisbenzimidazole), PTCDA (3,4,9,10 perylene-tetracarboxylic dianhydride), or Poly(benzimidazobenzophenanthroIine), TCNQ (7,7,8,8- tetracyanoquinodimethane), F4-TCNQ (tetrafluorotetracyanoquinodimethane), and the like. The suitable organic semiconductors for the electron donor layer 220B include, but are not limited to, BTEM-PPV (Poly(2,5-bis(l,4,7,10-tetraoxaundecyl)- 1,4- 9 041816

0106phenylenevinylene), Poly(3-decyloxythiophene), CuPc (copper phthalocyanine), NPD (4_>4^>-bis(N-(l-napthyl)phenylamino)biphenyl)_J pentacene, tetracene, and the like. [00103] According to another embodiment 200C illustrated in FIG. 2C, both of the electron acceptor layer 230C and the electron donor layer 220C in the photoactive region 222C can be bulk heterojunctions comprising polymer-wrapped carbon nanotubes and the respective acceptor-type or donor-type organic semiconductor materials. [00104] In FIG. 2D, a bulk heterojunction PV device 200D according to another embodiment is shown. The device 200D comprises a conducting anode layer 210D, a conducting cathode layer 250D and a bulk heterojunction layer 220D provided between and electrically connected to the two electrodes. The bulk heterojunction layer 220D comprises polymer-wrapped carbon nanotubes disposed within an organic semiconductor material that can be either an organic electron acceptor or electron donor materials disclosed herein. In this embodiment, the bulk heterojunction layer 220D forms the photoactive region of the device 200D. Optionally, one or more exciton blocking layers can be provided in the device. An exciton blocking layer 215D can be provided between the anode layer 210D and the bulk heterojunction layer 220D. Another exciton blocking layer 240D can be provided between the cathode layer 250D and the bulk heterojunction layer 220D either in conjunction with the first exciton blocking layer 215D or independent of the first exciton blocking layer 215D.

0107[00105] In the devices of 200A, 200B, 200C and 200D, preferably, the polymer- wrapped carbon nanotubes are substantially semiconducting PW-SWNTs. An optional exciton blocking layer 240A, 240B, 240C can be provided between the photoactive regions 222A, 222B, 222C and the cathode layers 250A, 250B, 250C, respectively. Additionally, an optional exciton blocking layer 215A, 215B, 215C can be provided between the photoactive regions 222A, 222B, 222C and the anode layers 210A, 210B, 210C, respectively. An anode-smoothing layer may also be situated between the anode and the donor.

0108[00106] FIGs. 3A-3B show additional hybrid planar-bulk heterojunction embodiments for a photovoltaic device 300A and 300B. Referring to FIG. 3A, the photovoltaic device embodiment 300A comprises a conducting anode layer 310A, a thin film of polymer- wrapped carbon nanotubes as an electron donor layer 320A formed 16

0109above the anode layer 310A, and a bulk heteroj unction layer 325 A comprising polymer- wrapped carbon nanotubes disposed within an organic electron acceptor material formed above the donor layer 320A. An electron acceptor layer 330A is formed above the bulk heteroj unction layer 325A and a conducting cathode layer 350A is formed above the acceptor layer 330A. The electron donor layer 320A, the bulk heteroj unction layer 325 A and the electron acceptor layer 330A form the photoactive region 322 A of the device 300A.

0110[00107] The suitable organic semiconductor acceptor materials for forming the bulk heteroj unction layer 325A and the electron acceptor layer 330A are the same as those discussed in conjunction with the embodiment of FIG. IA. [00108] Referring to FIG. 3B, the photovoltaic device embodiment 300B comprises a conducting anode layer 310B, an electron donor layer 320B formed above the anode layer 310B and a bulk heterojunction layer 325B comprising polymer-wrappεd carbon nanotubes disposed within an organic electron donor material formed above the donor layer 320B. A thin film of polymer- wrapped carbon nanotubes as an electron acceptor layer 330B is formed above the bulk heterojunction layer 325B and a conducting cathode layer 350B is formed above the bulk heterojunction layer 325B. The electron donor layer 320B, the bulk heterojunction.layer 325B and the electron acceptor layer 330B form the photoactive region 322B of the device 300B. [00109] As in the embodiment 300A, the suitable organic semiconductor acceptor materials for forming the bulk heterojunction layer 325B are the same as those discussed in conjunction with the embodiment of FIG. IA. The possible organic semiconductor materials for the electron donor layer 320B are same as those discussed in conjunction with the embodiment of FIG. IB.

0111[00110] In both embodiments 300A and 300B, the bulk heterojunction layers 325A and 325B can be formed by depositing a mixed film of both organic semiconductor material and polymer- wrapped carbon nanotubes, or by vapor deposition of an organic semiconductor onto a thin mat of polymer- wrapped carbon nanotubes. This bulk heterojunction layer may then be sandwiched between a layer of polymer-wrapped carbon nanotubes (320A, 320B) and a layer of organic semiconductor (330A, 330B). [00111] In both embodiments 300A and 300B, preferably, the polymer-wrapped carbon nanotubes are substantially semiconducting PW-SWNTs. An optional exciton blocking layer 340A, 340B can be connected between the photoactive regions 322A, 322B and the cathode layers 350A, 350B, respectively. Additionally, an optional exciton blocking layer 315A, 315B can be connected between the photoactive regions 322A, 322B and the anode layers 310A, 310B, respectively. An anode-smoothing layer may also be situated between the anode and. the donor.

0112[00112] The small molecule organic semiconductors discussed herein can be deposited by vacuum thermal evaporation (VTE), organic vapor phase deposition (OVPD). or via solution-based processing methods. Depending on the background growth pressure, substrate temperature, growth rate, the molecular structure of the organic semiconductor, and the roughness of the substrate, various morphologies and degrees of crystalline order can be obtained, which influence charge transport and interfacial morphology. In the instance in which organic semiconductors are deposited directly on top of percolating networks of CNTs, the inherent roughness of the CNT network may be used to cause roughness-induced crystallization or crystalline growth in order to improve device characteristics.

0113[00113] One technique for sorting carbon nanotubes by their band gap, diameter, and electronic-type that is currently amenable to the fabrication of organic semiconductor-semiconducting CNT heterojunction photovoltaic solar cells is density gradient ultracentrifugation (DGU) (M. S. Arnold, A. A. Green, J. F. Hulvat et al., Nature Nanotech. 1(1), 60 (2006); M. S. Arnold, S. I. Stupp, and M. C. Hersam, Nano Letters 5 (4), 713 (2005)). Using DGU, bulk samples (gram scale) of up to 99% single electronic type (either semiconducting or metallic) can be readily produced. Furthermore, DGU can be used to sort SWNTs by their diameter, optical band gap, and electrical band gap as well.

0114[00114] Incorporation of a network of nanotubes into a matrix can be carried out by several methods known in the art, including but not limited to vapor deposition of the matrix material and spin-casting of polymer-nanotube blends. (See for example U.S. Patent No. 7,341,774 the content of which is incorporated herein by reference, and references therein.) [00115] As discussed above, the properties of carbon nanotubes are influenced by the diameter of the tube and its cbirality. This is illustrated in FIGs. 11 A-IlD where the current-voltage characteristics and spectrally resolved photoresponse for a PW-CNT/Ceo heteroj unction diode 400 of FIG. HA are shown. The diode 400 comprises an ITO anode layer 410, a PW-CNT layer 420, a C₆o acceptor layer 430, and optional BCP electron blocking layer 440 and a Ag cathode 450. The thickness of the layers are provided in FIG. HA. The PW-CNT is wrapped with MDMO-PPV polymer at 1:1 ratio by weight and the PW-CNT/Cδo interface forms the heterojunction. The diode 400 has dark current rectification ratios >10³ at ±1 V (see FIG. HB), which is particularly remarkable given that the PW-CNT layer 420 consists of a high density of metallic tubes whose presence would be expected to result in large shunt currents. The absence of such parasitic effects from the metal tubes suggests that they are, indeed, electrically and energetically isolated from the semiconducting tubes by the wrapped polymer. [00116] Referring to FIG. HB, a fit to the forward bias current- voltage characteristics (solid line) follows the ideal diode equation with an ideality factor of 2.0 and a specific series resistance of 0.99 Ω-cm². Here, the ideality factor ~2 suggests that carrier recombination is the dominant source of dark current, which is again remarkable considering the high density of metallic tubes which should lead to significant shunt currents (and hence resistance-limited transport).

0115[00117] The near-ER responsivities of the diode at 0 V and -0.7 V are compared in

0116FIG. HC. Due to the diametric heterogeneity of the nanotubes, photoactive response is observed over a wide range from both En (λ=^;900-1450 nm) and E₂₂ (λ«550-900 nm) absorption features, with the peak polymer response at λ=500 nm. The chirality indices (n,m) of the nanotube responsible for each absorption feature are labeled in the FIG. HC, as are the absorption regions of the polymer and small molecule constituents of the device. The very broad spectral coverage is a direct result of the diametric polydispersity of the SWNTs which collectively cover the spectrum from 550nm to 1600nm. [00118] Referring to FIG. HC, the diode responsivity at λ=l 155 nm at a bias of 0

0117V and -0.7 V was 12 mA/W and 21 rnA/W, respectively, corresponding to a peak EQE=2.3%. At λ= 1-300 nm, the detector responsivity was 11 and 21 mA/W (EQE=2.0%), respectively, whereas the response of devices lacking CNTs at these wavelengths was not measurable (<0.1 μA/W). The IQE of the SWNTs in the near-IR (FIG. HD) was > 20% between λ=1000 and λ=1400, suggesting that SWNT-based devices with much higher EQE should be achievable.

EXAMPLES

0119I. Materials

0120[00119] The method of Arnold et al., Nature Nanotech, 1 :60-65 (2006) is used to isolate semiconducting CNTs using density gradient ultracentrifugation. A commercially- available CNT powder is suspended in water with a 1 :4 mixture of sodium dodecyl sulfate and sodium cholate (2% surfactant) by ultrasonic treatment. The nanotube suspension is then loaded onto an iodixanol linear density gradient and centrifuged to sort the nanotubes by buoyant density. After fractionation of the density gradient, the iodixanol is removed by dialysis in surfactant solutions. Suitable organic semiconductors are well-known in the art, and are commercially available from a number of suppliers.

0121II. Planar heteroiunction with near-IR sensitivity

0122[00120] Raw HiPCO single-walled carbon nanotubes (Carbon Nanotechnologies

0123Inc.) (10 mg) were mixed with 10 ml of 2% (w/v) sodium cholate (Sigma-Aldrich, 995) in water. The mixture was homogenized in an ultrasonic bath for 15 minutes using a hom probe ultrasonicator. Coarse aggregates and large bundles of single- walled carbon nanotubes were then removed via ultracentrifugation (15,000 g, 12 hours). An aliquot of the resulting suspension (100 μl) was filtered via vacuum filtration on an AI₂O₃ membrane (0.02 μm pores, Whatman Inc.). The nanotube film was then transferred to a planar PDMS stamp by pressing the PDMS into the membrane with finger pressure. The film was then stamped (1000 N-cm-2, 60 s, room temperature, ambient atmosphere) onto a substrate consisting of 100 nm of PTCDA (3,4,9,10-perylene tetracarboxylic dianhydride) on Ag-coated ITO (indium tin oxide). The PTCDA and Ag had been evaporated via thermal evaporation in a 1E-7 torr vacuum at a rate of 0.15nm/s. Testing was done in ambient, and a xenon lamp plus an AMI .5G filter was utilized to approximate the solar spectrum. A calibrated photodiode was utilized to determine the light intensity. [00121] The current density-voltage curve of the resulting device (FIG. 4) was obtained by pressing a gold contact pad onto the surface of the SWNT network and applying a voltage. The potential in the x-axis of FIG. 5 denotes the potential of the carbon nanotube film with respect to that of the ITO/Ag electrode. In the dark, the device exhibited typical diode behavior, but when illuminated with simulated near-IR solar radiation (AMI .5G spectrum, filtered through a dielectric long-pass filter with a 950 run cut-off) a photoelectric effect was observed (FIG. 5).

0124rV. Bulk heteroiunctions

0125[00122] In one embodiment, a layer of substantially semiconducting or mixed

0126SWNTs is transferred by PDMS stamping onto a transparent anode. A suspension of substantially semiconducting SWNTs in a solution of an organic acceptor is spin-cast onto the SWNT layer. An acceptor layer, and an optional electron transport and/or exciton blocking layer, are then deposited, followed by a cathode layer.

0127[00123] In another embodiment, an organic donor layer is deposited onto an anode substrate, and a suspension of substantially semiconducting SWNTs in a solution of an organic acceptor is spin-cast onto the donor layer. A layer of substantially semiconducting or mixed' SWNTs is applied by PDMS stamping, followed by deposition of an optional electron transport and/or exciton blocking layer. A cathode layer is then deposited.

0128[00124] As discussed above, excitons in carbon nanotubes can be split by interfacing them with the organic acceptor, evaporated C_έo, and internal quantum efficiency as large as about 35 % at 1200 nm has been observed. (See FIG. 9D). It is expected that the spectral range of the carbon nanotube/organic hybrid photovoltaic devices can further extend into the near-infrared by using carbon nanotubes with larger diameter.

0129[00125] While the present invention is described with respect to particular examples and preferred embodiments, it is understood that the present invention is not limited to these examples and embodiments. The present invention as claimed therefore includes variations from the particular examples and preferred embodiments described herein, as will be apparent to one of skill in the art.