Nano-fabrication includes the fabrication of very small structures that have features on the order of 100 nanometers or smaller. One application in which nano-fabrication has had a sizeable impact is in the processing of integrated circuits. The semiconductor processing industry continues to strive for larger production yields while increasing the circuits per unit area formed on a substrate, therefore nano-fabrication becomes increasingly important. Nano-fabrication provides greater process control while allowing continued reduction of the minimum feature dimensions of the structures formed. Other areas of development in which nano-fabrication has been employed include biotechnology, optical technology, mechanical systems, and the like.
An exemplary nano-fabrication technique in use today is commonly referred to as imprint lithography. Exemplary imprint lithography processes are described in detail in numerous publications, such as U.S. Patent Publication No. 2004/0065976, U.S. Patent Publication No. 2004/0065252, and U.S. Pat. No. 6,936,194, all of which are hereby incorporated by reference.
An imprint lithography technique disclosed in each of the aforementioned U.S. patent publications and patent includes formation of a relief pattern in a formable layer (polymerizable) and transferring a pattern corresponding to the relief pattern into an underlying substrate. The substrate may be coupled to a motion stage to obtain a desired positioning to facilitate the patterning process. The patterning process uses a template spaced apart from the substrate and a formable liquid applied between the template and the substrate. The formable liquid is solidified to form a rigid layer that has a pattern conforming to a shape of the surface of the template that contacts the formable liquid. After solidification, the template is separated from the rigid layer such that the template and the substrate are spaced apart. The substrate and the solidified layer are then subjected to additional processes to transfer a relief image into the substrate that corresponds to the pattern in the solidified layer.
So that the present invention may be understood in more detail, a description of embodiments of the invention is provided with reference to the embodiments illustrated in the appended drawings. It is to be noted, however, that the appended drawings illustrate only typical embodiments of the invention, and are therefore not to be considered limiting of the scope.
Referring to the figures, and particularly to
Substrate 12 and substrate chuck 14 may be further supported by stage 16. Stage 16 may provide motion along the x-, y-, and z-axes. Stage 16, substrate 12, and substrate chuck 14 may also be positioned on a base (not shown).
Spaced-apart from substrate 12 is a template 18. Template 18 may include a mesa 20 extending therefrom towards substrate 12, mesa 20 having a patterning surface 22 thereon. Further, mesa 20 may be referred to as mold 20. Alternatively, template 18 may be formed without mesa 20.
Template 18 and/or mold 20 may be formed from such materials including, but not limited to, fused-silica, quartz, silicon, organic polymers, siloxane polymers, borosilicate glass, fluorocarbon polymers, metal, hardened sapphire, and/or the like. As illustrated, patterning surface 22 comprises features defined by a plurality of spaced-apart recesses 24 and/or protrusions 26, though embodiments of the present invention are not limited to such configurations. Patterning surface 22 may define any original pattern that forms the basis of a pattern to be formed on substrate 12.
Template 18 may be coupled to chuck 28. Chuck 28 may be configured as, but not limited to, vacuum, pin-type, groove-type, electrostatic, electromagnetic, and/or other similar chuck types. Exemplary chucks are further described in U.S. Pat. No. 6,873,087, which is hereby incorporated by reference. Further, chuck 28 may be coupled to imprint head 30 such that chuck 28 and/or imprint head 30 may be configured to facilitate movement of template 18.
System 10 may further comprise a fluid dispense system 32. Fluid dispense system 32 may be used to deposit polymerizable material 34 on substrate 12. Polymerizable material 34 may be positioned upon substrate 12 using techniques such as drop dispense, spin-coating, dip coating, chemical vapor deposition (CVD), physical vapor deposition (PVD), thin film deposition, thick film deposition, and/or the like. Polymerizable material 34 may be disposed upon substrate 12 before and/or after a desired volume is defined between mold 20 and substrate 12 depending on design considerations. Polymerizable material 34 may comprise a monomer mixture as described in U.S. Pat. No. 7,157,036 and U.S. Patent Publication No. 2005/0187339, all of which are hereby incorporated by reference.
Referring to
Either imprint head 30, stage 16, or both vary a distance between mold 20 and substrate 12 to define a desired volume therebetween that is filled by polymerizable material 34. For example, imprint head 30 may apply a force to template 18 such that mold 20 contacts polymerizable material 34. After the desired volume is filled with polymerizable material 34, source 38 produces energy 40, e.g., ultraviolet radiation, causing polymerizable material 34 to solidify and/or cross-link conforming to shape of a surface 44 of substrate 12 and patterning surface 22, defining a patterned layer 46 on substrate 12. Patterned layer 46 may comprise a residual layer 48 and a plurality of features shown as protrusions 50 and recessions 52, with protrusions 50 having thickness t1 and residual layer having a thickness t2. It should be noted that solidification and/or cross-linking of polymerizable material 34 may be through other methods including, but not limited, exposure to charged particles, temperature changes, evaporation, and/or other similar methods.
The above-mentioned system and process may be further employed in imprint lithography processes and systems referred to in U.S. Pat. No. 6,932,934, U.S. Patent Publication No. 2004/0124566, U.S. Patent Publication No. 2004/0188381, and U.S. Patent Publication No. 2004/0211754, each of which is hereby incorporated by reference.
The availability of low cost nano-patterning may provide organic solar cell designs that substantially improve the efficiency of organic photovoltaic materials. Several resources indicate that the ability to produce nanostructured materials at a reasonable cost may significantly enhance the efficiency of next generation solar cells. See, M. Jacoby, “Tapping the Sun: Basic chemistry drives development of new low-cost solar cells,” Chemical & Engineering News, Aug. 27, 2007, Volume 85, Number 35, pp. 16-22; I. Gur, et al., “Hybrid Solar Cells with Prescribed Nanoscale Morphologies Based on Hyperbranched Semiconductor Nanocrystals,” Nano Lett., 7 (2), 409-414, 2007; G. W. Crabtree et al., “Solar Energy Conversion,” Physics Today, March 2007, pp 37-42; A. J. Nozik, “Exciton Multiplication and Relaxation Dynamics in Quantum Dots: Applications to Ultrahigh-Efficiency Solar Photon Conversion,” Inorg. Chem., 2005, 44, pp. 6893-6899; and, M. Law, et al., “Nanowire dye-sensitized solar cells,” Nature Materials, 4, 455, 2005, all of which are hereby incorporated by reference.
Organic containing non-Si based solar cells may generally be divided into two categories: organic solar cells and inorganic/organic hybrid cells. In organic solar cells, N-type materials may include, but not limited to organic modified fullerene, organic photo harvested dyes coated onto nano-crystal (e.g., TiO2, ZnO), and/or the like. For example, in forming the N-material from organic modified fullerene, the solar cell may be constructed by a donor-acceptor mechanism using P-material formed of a conjugated polymer. In forming the N-material from organic photo harvested dyes, the dye-sensitized nano-crystal (e.g., TiO2, ZnO, TiO2 overcoat ZnO) may be used in conjunction with liquid electrolyte to form the solar cell (also referred to as a Gratzel solar cell).
In inorganic/organic hybrid cells, the P-type material may be formed of organic conjugated polymer and the N-type material may be formed of inorganic materials including, but not limited to TiO2, CdSe, CdTe, and other similar semiconductor materials.
The first electrode layer 62a and second electrode layer 68a of solar cell design 60a may be similar in design to the first electrode layer 62 and second electrode layer 68 of solar cell design 60. The blended PV layer 65a may be formed of PV material blended with N-type inorganic nanoparticles.
Another exemplary solar cell design may incorporate the use of dye sensitized ZnO nanowires. This design is further described in M. Law, et al., “Nanowire dye-sensitized solar cells”, Nature Materials, 4, 455, 2005, which is generally based on Grätzel cells further described in B. O'Regan, et al., “A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO2 films,” Nature 353, 737-740 (1991), both of which are hereby incorporated by reference.
The excitons (electron/hole pairs) created in the PV materials by incident photons may possess a diffusion length L. For example, excitons may posses a diffusion length L that is approximately 5 to 30 nm. Referring to
Referring to
The first electrode layer 62b and second electrode layer 68b are generally conductive and may be formed of materials including, but not limited to, indium tin oxide, aluminum, and the like. At least a portion of the first electrode layer 62b may be substantially transparent. Additionally, the first electrode layer 62b may be formed as a metal grid. The metal grid may increase the total area of the solar cell 60b having exposure to energy (e.g., the sun). Metals may be directly patterned using processes such as described in K. H. Hsu, et al., “Electrochemical Nanoimprinting with Solid-State Superionic Stamps”, Nano Lett., 7(2), 2007.
The electron acceptor layer 64b may be formed of N-type materials including, but not limited to, fullerene derivatives and the like. Fullerene may be organically modified to attach functional groups such as thiophene for electro-polymerization. Additionally, fullerene may be modified to attach functional groups including, but not limited to, acrylate, methacrylate, thiol, vinyl, and epoxy, that may undergo crosslinking upon exposure to UV and/or heat. Additionally, fullerene derivatives may be imprinted by adding a small amount of crosslinkable binding materials.
The electron donor layer 66b may be formed of P-type materials including, but not limited to, polythiophene derivatives (e.g., poly 3-hexylthiophene), polyphenylene vinylene derivatives (e.g., MDMO-PPV), poly-(thiophene-pyrrole-thiophene-benzothiadiazole) derivatives, and the like. Generally, the main chain conjugated backbones of these polymers may be unaltered. The side chain derivatives, however, may be altered to incorporate reactive functional groups that may undergo a crosslinking reaction upon exposure to UV and/or heat including, but not limited to, acrylate, methacrylate, thiol, vinyl, and epoxy. See, K. M. Coakley, et al., “Conjugated Polymer Photovoltaic Cells,” Chem. Mater., ACS Publications, 2004, 16, pp. 4533-4542, which is hereby incorporated by reference. The addition of semiconductor nanocrystals including, but limited to, cadmium selenide and cadmium telluride, ZnO nanowires with or without TiO2 coatings, and the like, may further improve efficiencies of the PV materials.
Fullerene derivatives and polysilicon may be deposited using ink jet techniques as described in T. Shimoda, et al. “Solution-processed silicon films and transistors,” Nature, 2006, 440, pp. 783-786, which is hereby incorporated by reference. Depositing using ink jet techniques may allow for low cost, non vacuum deposition. Silicon based lithographic processes with sacrificial resists and reactive ion etching (RIE) may be used to etch doped polysilicon type materials. Additionally, silicon based lithographic processes, including reactive ion etching, may allow for the use of high aspect ratio patterned pillars using intermediate hard masks (e.g., SiN).
Dyes may also be added to improve broadband absorption of photons and provide efficiencies in the range of approximately 1-3%. See, M. Jacoby, “Tapping the Sun: Basic chemistry drives development of new low-cost solar cells,” Chemical & Engineering News, Aug. 27, 2007, Volume 85, Number 35, pp. 16-22, which is hereby incorporated by reference.
Electron donor layer 66b may have a thickness tPV. For example, the thickness tPV of electron donor layer 66b may be approximately 100-500 nm. The electron acceptor layer 64b may be patterned to possess one or more pillars 72 having a length p.
Referring to
In one embodiment, recesses 74 may be provided with length s=2L and pillars 72 may be provided with length p<2L, wherein L is the diffusion length of the electrons created in the electron donor layer 66b. This reduction in the length p of pillars 72 may provide for a high volume of electron donor layer 66b for a given thickness tPV of the electron donor layer 66b. For example, if L=10 nm, then s=20 nm and p<20 nm. With a thickness tPV of 200 nm, the pillars 72 may have a 20:1 aspect ratio. A 20:1 aspect ratio, however, may be difficult to fabricate reliably and inexpensively due to mechanical stability.
Sub-optimal designs may be implemented. For example, if the diffusion length L is approximately 10 nm, the length p of pillar 72 may be designed at approximately 50 nm with length s of recess 74 set at approximately 100 nm. For a thickness tPV of 200 nm, pillars 72 may have about a 4:1 ratio. Additionally, the lost volume of the electron donor layer 66b may be approximately 8.7% as compared to 25% in the optimal design.
Sub-optimal designs, however, may have lower capture efficiency. As such, sub-optimal designs may be complemented with blended PV materials in the electron donor layer 66b, wherein the electron donor layer 66b may contain conjugated polymers mixed with inorganic nano-rods, as described in 1. Gur, et al., “Hybrid Solar Cells with Prescribed Nanoscale Morphologies Based on Hyperbranched Semiconductor Nanocrystals,” Nano Lett., 2007, 7(2), pp. 407-414; and, W. U. Huynh, et al., “CdSe nanocrystal Rods/Poly(3-hexylithiophene) Composite Photovoltaic Devices,” Adv. Mater., 1999, 11(11) pp. 923-927. Exemplary blended materials include, but are not limited to, mixtures of 5 nm diameter CdSe nanocrystals and Meh-PPv poly(2-methoxy-5-(2′-ethyl-hexyloxy)-p-phenylenevinylene), and 8×13 nm elongated CdSe nanocrystals and regi-regular poly(3-hexylithiophene) (P3HT). Such blended materials may substantially overcome the lost exciton capture potential due to the departure from the optimal geometry of the patterned P-N junction 70a discussed above.
ZnO may be patterned using dots rather than ZnO nanoparticles. Patterning may improve placement and uniformity as compared to ZnO nanoparticles further described in Coakley, “Conjugated Polymer Photovoltaic Cells,” Chem. Mater., ACS Publication, 2004, 16, pp. 4533-4542, which is hereby incorporated by reference. For example, patterning may be provided followed by a reactive ion etching as further described in Zhu, “SiCl4-Based Reactive Ion Etching of ZnO and MgxZn1-x Films on r-Sapphire Substrates,” J. of Electronic Mater., 2006, 35:4, which is hereby incorporated by reference. Patterning using reactive ion etching may provide for substantially precise placement in addition to size control.
As illustrated in
Additionally, materials at the air interface may assist in cycling photons through electron donor layer 66b. For example, as previously discussed, materials at the air interface may include, but are not limited to, fullerene derivatives, ITO, conjugated polymers and TiO2. Each of these materials include high indexes ranging from approximately 1.5 (e.g., polymers) to greater than approximately 2 (e.g., fullerenes). As such, light approaching the air interface at inclination exceeding the critical angle may internally reflect. If the first electrode layer 62d is a metal contact grid, this may assist with cycling photons back through electron donor layer 66d.
The first electrode layer 62e may be adjacent to electron donor layer 66e. The first electrode layer 62e may also be isolated from electron acceptor layer 64e and/or 64f.
Solar cell design 60e may be patterned using dual patterning steps. Dual patterning steps may nominally double the area of the patterned p-n junction 70a and the thickness tPV of the electron donor layer 66e. Using imprinting, a thin PV material film (e.g., <10 nm) may remain and may prevent direct contact between pad 80 and underlying pillars 72 of electron acceptor layer 64e. The thin PV material film may be even further reduced (e.g., <5 nm) to provide for conductivity between the electron acceptor layer 64e and electron acceptor layer 64f.
Referring to
Referring to
Referring to
Referring to
Second electron acceptor layer 64h may be formed by template 18b using imprint lithography or other methods, as described above. Template 18b may include a patterning region 95 and a recessed region 93, with patterning region 95 surrounding recessed region 93. As a result of recessed region 93 of template 18b, second electron acceptor layer 64h may be non-contiguous. For example, second electron acceptor layer 64h may not be in superimposition with recessed region 93 resulting from capillary forces between any of the material of second electron acceptor layer 64h, template 18b, and/or electron acceptor layer 64g, as further described in U.S. Patent Publication No. 2005/0061773, which is hereby incorporated by reference. Generally, the non-contiguous portion of the second electron acceptor layer 64h may result in minor loss of electron capture due to lack of matrix of the N-type material. Electron acceptor layer 64g may also be formed non-contiguous depending on design considerations.
Referring to
Referring to
Solar cell 60g may be subjected to substantially the same process described above to form additional electron donor and electron acceptor layers. For example, in
Referring to
Referring to
Referring to
The spacing between residual layer 82k of second electron acceptor layer 64k and residual layer 82j of electron acceptor layer 64j may be on the order of the diffusion length L, 5-10 nm. Further, the second electron acceptor layer 64k may be positioned within unfilled region 77. As a result, the second electron acceptor layer 64k may be coupled to electron layer 64j with both in electrical communication with electrode layer 62j.
Referring to
Solar cell 60j may be subjected to substantially the same process described above to form additional electron donor and electron acceptor layers. For example, in
As illustrated in
Electrode layer 106 may be formed of materials including, but not limited to, aluminum, indium tin oxide, and the like. The electrode layer 106 may have a thickness t4. For example, the electrode layer 106 may have a thickness t4 of approximately 1 to 100 μm.
Adhesive layer 108 may be formed of adhesion materials as further described in U.S. Publication No. 2007/0212494, which is hereby incorporated by reference. Adhesive layer 108 may have a thickness t5. For example, adhesive layer 108 may have a thickness t5 of approximately 1-10 nm.
As illustrated in
Additionally, patterned layer 46a may have one or more gaps 102. The size of the gaps 102 and number of gaps 102 may be such that gaps 102 do not consume more than 1-10% of the total area of the multi-layer substrate 100. As illustrated in
As illustrated in
Conformal coating 110 may have a thickness t8. For example, conformal coating 110 may have a thickness of approximately 1-10 nm. As illustrated, conformal coating 110, by way of gap 102, may be in direct communication with electrode layer 104.
It should be noted that an N-type conformal coating may then be further coated or deposited using ink jet with a P-type material. P-type material may include, but is not limited to, polythiophene derivatives, polyphenylene vinylene derivatives, poly-(thiophene-pyrrole-thiophene-benzothiadiazole) derivatives, and the like as discussed herein. This may be followed by the fabrication of a top conductor leading to a solar cell similar to the one in
The distance between the gaps 102 and the size of the gaps 102 may be selected, to not only minimize loss of device area (as discussed earlier), but also may address a competing requirement: minimization of the distance traveled by the charged particle to the bottom electrode, wherein the charged particle is created by disassociation of the exciton at the patterned P-N interface.
Number | Date | Country | |
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60990810 | Nov 2007 | US | |
61024597 | Jan 2008 | US | |
61111066 | Nov 2008 | US |