ATOMIC LAYER DEPOSITION ON HIGH-ASPECT-RATIO ELECTRODE STRUCTURES
20220140307 · 2022-05-05
Inventors
- Isabelle M. Darolles (Altadena, CA, US)
- Azin Fahimi (Pasadena, CA, US)
- Sean A. Mendoza (Alhambra, CA, US)
- Shannon C. Santana (San Marino, CA, US)
- Zarui S. Chikneyan (Altadena, CA, US)
- Jeffrey L. Arias (Downey, CA, US)
Cpc classification
H01M4/13
ELECTRICITY
H01M4/583
ELECTRICITY
H01G11/28
ELECTRICITY
H01M4/525
ELECTRICITY
H01M4/505
ELECTRICITY
Y02E60/10
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
H01G11/24
ELECTRICITY
H01G11/36
ELECTRICITY
H01M10/0525
ELECTRICITY
International classification
H01M4/36
ELECTRICITY
H01M4/505
ELECTRICITY
H01M4/525
ELECTRICITY
Abstract
Battery electrodes using VACNT forests to create 3D electrode nanostructures, and methods of making, are described. The VACNTs are electrically and mechanically attached to the anode or cathode substrates, providing a large area of 3D surfaces for coating with active materials and high-conductivity electron pathways to the cell current collectors. A number of different active materials suitable for anodes and cathodes in lithium-ion batteries may be used to coat the individual carbon nanotubes. The high surface area provided by the VACNT forest and the nano-dimensions of the coated active materials enable both high energy-density and high power-density to be achieved with the same battery. Complete conformal coating of the individual CNTs may be achieved by a number of different methods, and coating with multiple active materials may be used to create nanolaminate coatings having improved electrochemical characteristics over single materials.
Claims
1-122. (canceled)
123. A method of making a cathode for a lithium ion battery, the method comprising the steps of: depositing a catalyst and an underlayer on a substrate, wherein the substrate is a metal foil substrate comprising a longitudinal axis and at least one hole or void; growing a plurality of vertically aligned carbon nanotubes on the substrate, wherein each nanotube of the plurality of vertically aligned carbon nanotubes has an outer surface and a longitudinal axis, and wherein the longitudinal axis of each nanotube is substantially perpendicular to the longitudinal axis of the substrate; and depositing a protective layer on the outer surface of each nanotube by atomic layer deposition.
124. (canceled)
125. The method of claim 123, wherein the substrate comprises a first and a second side, and wherein a first portion of the plurality of vertically aligned carbon nanotubes is grown on the first side of the substrate and a second portion of the plurality of vertically aligned carbon nanotubes is grown on the second side of the substrate.
126. The method of claim 124, wherein the metal foil substrate is patterned.
127. (canceled)
128. The method of claim 123, wherein a perimeter of the at least one hole or void defines an area between about 10 and about 500 μm.sup.2.
129-132. (canceled)
133. The method of claim 123, further comprising the step of incorporating a cathode active material onto the outer surface of each nanotube by a melting method prior to the step of depositing the protective layer.
134. The method of claim 123, further comprising the step of functionalizing the outer surface of each nanotube prior to the step of depositing the protective layer.
135. The method of claim 134, wherein the step of functionalizing the outer surface of each nanotube comprises UV/ozone, O.sub.2 plasma, or acid treatment.
136. The method of claim 123, further comprising the step of depositing a cathode active material onto the plurality of vertically aligned carbon nanotubes after the step of depositing the protective layer.
137. The method of claim 136, further comprising the step of depositing an additional protective layer onto the plurality of vertically aligned carbon nanotubes after the step of depositing the cathode active material.
138. (canceled)
139. The method of claim 123, further comprising the step of incorporating a cathode active material onto the plurality of vertically aligned carbon nanotubes by a sol-gel method after the step of depositing the protective layer on the outer surface of each nanotube.
140. The method of claim 139, further comprising the step of depositing an additional protective layer by atomic layer deposition onto the plurality of vertically aligned carbon nanotubes after the step of incorporating the cathode active material.
141. The method of claim 123, further comprising the step of infiltrating the plurality of vertically aligned carbon nanotubes with an organic solution containing metal precursors.
142. The method of claim 141, further comprising the step of heating and annealing the plurality of vertically aligned carbon nanotubes to form a cathode active material on the outer surface of each nanotube.
143. The method of claim 142, further comprising the step of depositing a protective layer on the plurality of vertically aligned carbon nanotubes by ALD.
144. (canceled)
145. The method of claim 123, further comprising the step of incorporating a cathode active material onto the outer surface of each of the plurality of vertically aligned carbon nanotubes by a melting method prior to the step of depositing the protective layer.
146. The method of claim 145, wherein the active material layer is selected from the group consisting of Li.sub.xV.sub.2O.sub.5, V.sub.2O.sub.5, LiNiO.sub.2, LiMn.sub.2O.sub.4, LiCoO.sub.2, FePO.sub.4, LiFePO.sub.4, Li(Mn,Ni,Co)O.sub.2, and Li(Ni,Co,Al)O.sub.2.
147. (canceled)
148. The method of claim 123, wherein a distance between adjacent holes is between about 5 μm and about 100 μm.
149. The method of claim 123, further comprising the step of incorporating a cathode active material onto the plurality of vertically aligned carbon nanotubes by ALD.
150. The method of claim 149, further comprising the step of incorporating a lithium precursor solution to the cathode active material.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION
[0060] As seen in
[0061]
[0062] Atomic Layer Deposition
[0063] A method of coating high aspect ratio structures, such as VACNTs, through atomic-layer deposition is described herein. Methods of performing ALD are described in Miikkulainen, V. et al. “Atomic Layer Deposition of Spinel Lithium Manganese Oxide by Film-Body-Controlled Lithium Incorporation for Thin-Film Lithium-Ion Batteries.” J. P
[0064] As mentioned above, VACNTs can be used as current collectors in Lithium ion batteries. VACNTs can be grown on substrates for use as current collectors. Growth of VACNTs on supports using chemical vapor deposition (CVD) is described in Zhao, N. and Kang, J. “Direct Growth of Carbon Nanotubes on Metal Supports by Chemical Vapor Deposition.” Carbon Nanotubes—Synthesis, Characterization, Applications, Dr. Siva Yellampalli (Ed.), ISBN: 978-953-307-497-9, InTech, Available from: http://www.intechopen.com/books/carbon-nanotubessynthesis-characterization-applications/direct-growth-of-carbon-nanotubes-on-metal-supports-by-chemicalvapor-deposition, which is hereby expressly incorporated by reference in its entirety for all purposes. The VACNTs can be grown to have a height of between 10 μm and about 3 mm, alternatively between about 20 μm and about 3 mm, alternatively between about 20 μm and about 2 mm, alternatively between 50 μm and about 1 mm, alternatively between about 50 μm and 800 μm, alternatively between about 100 μm and 600 μm, alternatively between about 50 μm and 500 μm, alternatively between about 20 μm and about 100 μm, alternatively between about 100 μm and 500 μm, alternatively between about 100 μm and 400 μm, alternatively between about 100 μm and 300 μm, alternatively between about 100 μm and 200 μm, alternatively between about 40 μm and about 200 μm. The VACNTs for an anode may have a height between about 20 μm and about 100 μm. The VACNTs for a cathode may have a height between about 40 μm and about 300 μm.
[0065] As seen in
[0066] Using ALD to coat VACNTs 10, however, presents several problems. As depicted in
[0067] The aspect ratios of the VACNT forests 20 can be between about 100 and about 3000, alternatively between about 100 and about 2500, alternatively between about 100 and about 2000, alternatively between about 100 and about 1:500, alternatively between about 100 and about 1000.
[0068] Gas Diffusion
[0069] One way to improve the use of ALD to coat VACNTs is to improve the diffusion of gas through the VACNT forest 20. For example, as seen in
[0070] ALD gas diffusion can also be increased by applying ALD to free-standing VACNT carpets. A free-standing nanotube carpet would also allow ALD gas penetration from both the top and bottom of the carpet.
[0071] Similarly, ALD gas diffusion will also be improved by using open-cell foam substrates (such as graphene, carbon, metal, or alloy foam). Open-cell foam substrates can be used to grow VACNT or other 3D structures on the ligaments between the open-cells. SEM images of VACNT grown on open-cell foam, e.g., nickel foam, are shown
[0072] Foam Substrates
[0073] A method of retaining both high electrode loadings (mg/cm.sup.2) needed for high energy density with low-aspect-ratio 3D structures for easier manufacture is herein described. The methods include using open-cell metal-foam substrates (see, e.g.,
[0074] The height of the (VACNT) 3D structures on a foam substrate 32 need only be a fraction of the height that would optimally be used on a planar foil substrate to manufacture electrodes, because after coating with active material, the foam 32 can be compressed to a fraction of its original height. The height of the VACNTs on a foam substrate may be between about 10 μm and about 100 μm, alternatively between about 10 μm and about 50 μm, alternatively between about 10 μm and about 80 μm. The height of the VACNTs on a flat substrate may be between about 10 μm and about 200 μm, alternatively between about 20 μm and about 200 μm, alternatively between about 20 μm and about 150 μm, alternatively between about 20 μm and about 100 μm, alternatively between about 10 μm and about 40 μm, alternatively between about 10 μm and about 30 μm. For instance, the height of the VANCTs on the foam substrate may be about ⅕, alternatively about ¼, alternatively about ⅓ of the height of the VACNTs on a flat substrate (e.g., about 20 μm compared to about 100 μm). By selecting the optimum combination of VACNT 10 height, cell count per unit area, ligament width, and subsequent foam compression, the resulting electrode will retain the same critical characteristics (loading and thickness) as an ideal planar electrode.
[0075] The open cell count per unit on the compressible foams are about 400 to about 10,000 per square inch, alternatively about 500 to about 10,000 per square inch, alternatively about 1,000 to about 10,000 per square inch, alternatively about 600 to about 9,000 per square inch. The porosity (void volume) can vary from about 70 to about 98%, alternatively from about 75 to about 98%, alternatively from about 75 to about 96%, alternatively from about 70 to about 99%, alternatively from about 80 to about 97%.
[0076] The width of the metal ligaments that connect to form the metal foam can be about 10 μm to about 100 μm, alternatively about 10 μm to about 95 μm, alternatively about 10 μm to about 90 μm, alternatively about 15 μm to about 100 μm, alternatively about 15 μm to about 95 μm, alternatively about 15 μm to about 90 μm, alternatively about 15 μm to about 85 μm.
[0077] The compressible foam 32 can be of any conductive material (metals or carbon) that can withstand the thermal and chemical environment required for growing the 3D structure, and the subsequent coating with any annealing of active electrode material components. The conductive material must also be able to withstand the chemical and electrochemical environment in the battery cell, and must be capable of collapsing to a thinner dimension while maintaining sufficient structural integrity and electrical conductivity to be useful as a battery electrode.
[0078] Examples of compressible foam materials that can be used for electrodes in lithium-ion batteries include but are not limited to, stainless steel, aluminum or nickel alloy for the cathode; copper or nickel for the anode; and carbon, graphene, or graphite for either the cathode or anode. In one embodiment, the foam material will have a high porosity and a high specific surface area of the ligaments. These electrodes will typically require foams with a high cell (pore) count/inch, e.g., >40 ppi to >100 ppi, ideally as high as possible, so as to provide the highest specific surface area (cm.sup.2 of ligament surface per cm.sup.3 of foam) available for the growth of the CNTs or other 3D structures. The cell (pore) count/inch may be about 40 ppi to about 100 ppi, alternatively about 50 ppi to about 100 ppi, alternatively about 60 ppi to about 100 ppi, alternatively about 40 ppi to about 95 ppi, alternatively > about 40 ppi, alternatively > about 50 ppi, alternatively > about 60 ppi, alternatively > about 70 ppi, alternatively > about 80 ppi, alternatively > about 90 ppi, alternatively > about 100 ppi, alternatively > about 110 ppi, where PPI is pores per inch.
[0079] The foam materials may also be coated with a thin layer of other materials to enhance or provide the required surface characteristics. For example, the foam may be coated with a thin layer of metal such as titanium, chrome, aluminum, copper, nickel, or ceramic such as Al.sub.2O.sub.3. A polymer/conductive carbon may be used as a matrix to mechanically and electronically bridge the foam structure. The polymers must be stable in the desired voltage range and compatible with the electrolyte. For example, polymers such as polyvinylidene fluoride (PVDF), styrene butadiene copolymer, polyacrylic acid (PAA), carboxy methyl cellulose (CMC).
[0080] The foam may also be compressible. In other words, the foam has the capacity to be flattened or reduced in height to about a fraction or percentage of its original height. The compressibility of the foam should be > about 30%, alternatively > about 40%, alternatively greater than about 60%, alternatively between about 30% and about 80%, alternatively between about 40% and about 80%, alternatively between about 50% and about 80%, alternatively between about 30% and about 90%, alternatively between about 40% and about 90%, alternatively between about 50% and about 90%. The foam may be reduced to about 50%, alternatively to about 40%, alternatively to about 30%, alternatively to about 20%, alternatively to about 10%, alternatively to between about 10% to about 70%, alternatively to between about 10% to about 60%, alternatively to between about 10% to about 50%, alternatively to between about 10% to about 40%, alternatively to between about 10% to about 30% of its uncompressed thickness or height.
[0081] While the current embodiment envisions using VACNTs for the 3D structure, it is recognized that other high-aspect-ratio structures could be used, such as free-standing nano rods of active material.
[0082] An open-cell foam substrate 32 can be reduced by compression to the appropriate electrode thickness after ALD deposition, e.g., to about a third of its original (uncompressed) thickness by applying a downward pressure. TABLE 1 shows a comparison of gain weight of active material for various substrates after same process. While the thickness of the electrodes are the same, open-cell foam substrates get the higher loading when processed under the same conditions.
TABLE-US-00001 TABLE 1 Weight of active material of various samples after the same coating processes (same batch of samples underwent low pressure chemical vapor deposition (LPCVD) followed by ALD) SnO.sub.2 Si wt. wt. Sample (mg) (mg) Total Thickness Foam (15 mm Sample after after Total Height Electrode diameter) Description LPCVD ALD of CNTs (foam substrate + CNTs) 1 Patterned 1.38 8.07 100 μm- CNTS on 110 μm stainless steel disc 2 Patterned 1.1 9.51 100 pm- CNTS on 110 μm stainless steel disc 3 Patterned 1.51 10.05 100 μm- CNTS on 110 μm stainless steel disc 4 CNTs on Ni 5.3 32.85 110 μm 600 μm 210 μm foam disc (after (before (after compression) compression) compression)
[0083] Moreover, as seen in TABLE 1, before compression, the foam electrode thickness is about 600 μm, and the foam electrode thickness after compression is about 210 μm. Thus, the % compression of the foam substrate is about 65%. A polymer/conductive carbon may be used as a matrix to mechanically and electronically bridge the structure. The polymers must be stable in the desired voltage range and compatible with the electrolyte. For example, polymers such as polyvinylidene fluoride (PVDF), styrene butadiene copolymer, polyacrylic acid (PAA), carboxy methyl cellulose (CMC). During compression of the foam, some of the attached VACNTs may be broken or detached, but at least 70%, alternatively at least 80%, alternatively at least 90%, alternatively at least 95% of the VACNTs remain intact and are not broken. In the case of brittle carbon foam, some of the ligaments themselves may be broken. In both cases, detachment or breakage can reduce the internal electronic conductivity of the electrode. These effects can be ameliorated by using a polymer/conductive-carbon coating.
[0084] The coatings can be applied by ALD as described in U.S. Pat. No. 7,582,544, which is hereby expressly incorporated by reference in its entirety for all purposes, and use of foam confers benefits similar to method for improving ALD on high aspect ratio structures. TABLE 1 shows the total loading of various samples after the same coatings processes, a combination of LPCVD and ALD. As seen on the TABLE 1, the foam substrate incorporated much higher loading than a regular flat substrate (e.g., stainless steel (SS) disc). Very high loading of active materials is achieved resulting in very high capacity electrode (anode) as shown
[0085] The coatings can be applied by a combination of ALD and wet methods. Sol-gel methods are easier and faster to synthesize active cathode materials; however, it is very difficult to incorporate a practical amount of active material into the dense VACNT electrode. On the other hand, the ALD method provides a very conformal coating and can provide practical loading of the active material, but a thick layer may take very long to produce. Combining these two methods, however, yields advantages. A layer of MnO.sub.x may be applied by ALD onto the VACNT in a first step, and then a solution of lithium precursors such as LiOH, LiNO.sub.3, or LiClO.sub.4 is incorporated to the MnO.sub.x/VACNT electrode by dip coating, or drop coating, or spin-coating. The organic solution must thoroughly infiltrate the VACNT forest until the stoichiometry to form LiMn.sub.2O.sub.4 is reached. After evaporation of the organic solvent, the layer of lithium precursor is reacted at a temperature greater than 300° C. in air or inert atmosphere. For example, manganese oxide was deposited onto VACNTs on graphene foam by ALD followed by dip coating in an LiOH solution. The resulting electrode was heated in air at 400° C. to form LiMn.sub.2O.sub.4 (“LMO”) and further tested in a half-cell coin cell.
[0086] The coatings can be also applied by a melting method. See, e.g., Hagen, M. et al. “Lithium-sulphur batteries—binder free carbon nanotubes electrode examined with various electrolytes.” J. P
[0087] Functionalization of VACNT Surfaces
[0088] Improved application of active materials to the surfaces of the VACNTs on the cathode and anode can also be accomplished by increasing the functionalization of the surfaces. Increasing the number of precursor nucleation sites and the overall affinity of the VACNT surfaces for active materials would increase the amount of active materials that can be coated onto the VACNTs. This can be accomplished with, e.g., acid functionalization, which requires a high vapor pressure acid such as fuming sulfuric acid to avoid liquid damage to the nanotube and substrate. Oxygen plasma treatment could also be employed, for which an exposure time and RF power (about 5 to about 100 Watts) must be calibrated to avoid complete destruction of the nanotubes (e.g., ˜a second to two minutes). Chemical functionalization treatment could be employed using trimethylaluminum (TMA) or tetrakis (dimethylamido) titanium (TDMAT) inside the ALD chamber at temperatures below 300 C. A thick layer of adhesion material could also be applied (˜2 nm or less) such as Al.sub.2O.sub.3 or SnO.sub.2 TiO.sub.2, prior to the ALD application of active materials.
[0089] Protective Layers to Prevent Degradation
[0090] Layering of different materials, active or otherwise, can be used to protect the primary active material from chemical or structural degradation and thereby improve cycle life.
[0091] Protective layers can be applied to prevent damage from any subsequent fabrication processes requiring high temperatures or other corrosive environments. A thin coating (approx. 1-4 nm) of inactive material (e.g., ZnO, V.sub.2O.sub.5, can be applied to VACNTs, nanotubes, or other 3D structures, by ALD. For subsequent processing by methods such as sol-gel, this protective coating will preserve the substrate conductivity and structure by protecting the CNTs from oxidation and decomposition.
[0092] Although VACNTs are very stable at very high temperatures in inert atmosphere, they will start decomposing at 420° C. in air. Moreover, wet processes for the synthesis of high voltage cathode materials (such as LiMn.sub.2O.sub.4, LiCoO.sub.2, NMC, LFP) generally involves calcination of precursors at high temperature in air. These conditions would damage the VACNTs, causing them to lose their properties/benefits. Even in the case of LiMn.sub.2O.sub.4 (LMO), where decomposition of the precursors occurs at lower temperature (below 400° C.), the damaging of the VACNTs is observed. Application of a conformal and uniform protective layer to prevent damage from any subsequent fabrication processes requiring high temperatures or other corrosive environments is needed. A thin coating (approx. 1-5 nm) of inactive material (e.g., Al.sub.2O.sub.3, ZnO, V.sub.2O.sub.5, . . . ) can be applied to VACNTs, nanotubes, and or other 3D structures, by ALD. For subsequent processing by wet methods, such as sol-gel, this protective coating will preserve the substrate conductivity and structure by protecting the CNTs from oxidation and decomposition.
[0093] For example, LiMn.sub.2O.sub.4 was formed by sol-gel method onto two types of VACNT: i) Uncoated VACNT, and ii) Al.sub.2O.sub.3 (4 nm) coated VACNT. The resulting electrodes LMO/VACNT were tested against Li metal in a half cell coin cell.
[0094] Method to Form LiMn.sub.2O.sub.4 on VACNT Directly Grown on a Metal Substrate:
[0095] A wet chemical method was employed to synthesize LiMn.sub.2O.sub.4 spinel material onto VACNT. In the first step, Li(CH.sub.3COO).2H.sub.2O and Mn(CH.sub.3COO).sub.2.4H.sub.2O, in appropriate molar ratio, were dissolved in a mixture of distilled water and isopropanol. Then, the prepared solution was applied drop-wise on the top of the VACNTs. This process was followed by aging at room temperature for 10 hours without covering to obtain a gel-coated composite. Finally, the obtained gel-coated composite was calcined in air at 350° C. for 30 minutes followed by annealing at 500° C. for 1 h.
[0096] Alternatively, a protective layer may be applied onto the active material using ALD. A very thin layer of inorganic compound (approx. 0.25 nm to 10 nm) such as SnO.sub.2, TiO.sub.2, Al.sub.2O.sub.3, ZnO can be applied to anode and cathode materials. This layer acts as a “solid electrolyte interface (SEI)”, i.e., passivates the surface preventing further reduction or oxidation of the electrolyte at high and low voltages. Additionally, this layer prevents the active material from dissolution that can lead to poor cycle life. For example, manganese dissolution from LMO occurs during cycling and causes poor cycle life. A thin protective layer of Al.sub.2O.sub.3 deposited by ALD can solve the problem. As shown
[0097] Direct Deposition of Active Material by ALD onto VACNT
[0098] The ALD process has several advantages, including well-controllable thickness with high uniformity, excellent conformal deposition, and low temperature growth (normally below 300° C.; some materials can be deposited at room temperature). Several ALD cathode and anode materials for Lithium ion battery (LIBs) have been studied on flat substrate and low aspect ratio structure, for example including FePO.sub.4, Li.sub.xMn.sub.2O.sub.4 and Li.sub.xV.sub.2O.sub.5, LiCoO.sub.2, V.sub.2O.sub.5, Co.sub.3O.sub.4, RuO.sub.2, SnO.sub.2, and TiO.sub.2, Cu.sub.2S, SiO.sub.x.
[0099] The electrode (cathode or anode) may have a single active layer or multiple active layers. In the case of multiple active layers, the last active layer can also serve as protective layer, preventing the electrolyte from decomposing further at low electrochemical potential. Alternatively, the active material can be sequentially layered by, e.g., ALD, or can be applied using nanolamination of various materials.
[0100] Cathode Protective Layers
[0101] Cathodes will comprise at least one primary active material, such as Li.sub.xMn.sub.2O.sub.4 or LiCoO.sub.2, that may be protected by a layer of at least one secondary active material, such as Li.sub.cV.sub.2O.sub.5 or LiFePO.sub.4, applied by ALD.
[0102] Lithiation of primary materials may occur at multiple points in time during the ALD process, either to single layers or multiple layers simultaneously. Lithiation can be tailored at each step for the active materials. This will permit maximal and consistent lithiation of the cathode. Post-deposition anneal may be applied.
[0103] Direct deposition of cathode materials is more challenging than for the anode materials because it generally involves a mixture of two or more materials. Cathode active materials can be Li.sub.xV.sub.2O.sub.5, V.sub.2O.sub.5, LiNiO.sub.2, LiMn.sub.2O.sub.4, LiCoO.sub.2, FePO.sub.4, LiFePO.sub.4, Li(Mn,Ni,Co)O.sub.2, Li(Ni,Co,Al)O.sub.2. Cathodes can comprise a single active material layer onto VACNT, or can comprise multiple layers of various cathode active materials, such as LiMn.sub.2O.sub.4/FePO.sub.4, or LiMn.sub.2O.sub.4/LiNiO.sub.2/FePO.sub.4. In the case of multiple layers, the last active layer can also serve as protective layer, preventing the electrolyte to decompose at high electrochemical potential. Alternatively, the cathode can be a nanolamination of various materials. The nanolamination, depending on the ALD cycle ratio, can result in the formation of a new complex compound. A pre-coat of a thin ALD layer, such as Al.sub.2O.sub.3, onto VACNT may be apply prior to ALD deposition of the cathode active material, especially if further annealing is required to form the electro-active material. Nanolamination is similar to ALD, except that each cycle can involve 1 to n different precursors. See, e.g., Donders, M. E. “Remote Plasma Atomic Layer Deposition of Thin Films of Electrochemically Active LiCoO.sub.2.” ECS Transactions, Vol. 41, 220.sup.th ECS Meeting, Oct. 9-14, 2011, Boston, Mass., Number 2, which is hereby expressly incorporated by reference in its entirety for all purposes.
[0104] A single layer of LiMn.sub.2O.sub.4 can also be applied. A layer of LiMn.sub.2O.sub.4 (LMO) is obtained by alternating ALD cycles of two binary compounds Li.sub.2O (or LiOH) and MnO.sub.x. The resulting thick layer is subsequently heated in air at 300° C. for 5 minutes to form LiMn.sub.2O.sub.4. SEM image of VACNT coated with LMO cathode material is shown
[0105] Anode Protective Layers
[0106] Anodes will comprise at least one primary active material, such as amorphous or poly-silicon which can be deposited on the substrate by LPCVD or FUND. See, e.g., Forney, M. W. et al. “High performance silicon free-standing anodes fabricated by low pressure and plasma-enhanced chemical vapor deposition onto carbon nanotube electrodes.” J. Power Sources 228: 270-80 (Apr. 15, 2013), which is hereby expressly incorporated by reference in its entirety for all purposes. This primary active material (Si) can then be coated with a second active material, such as SnO.sub.x or TiO.sub.2. to serve as a protective layer. This protective layer will be lithium-ion conductor and will protect the silicon from further reacting with the electrolyte during cycling.
[0107] Protective anode secondary layers may also be organic materials, such as Alucone, applied by molecular layer deposition (MLD). A protective layer may also be a combination of inorganic and organic layers to make a protective, and partially active, secondary layer (applied by MLD+ALD or other methods). An anode may also be comprised of a thin (˜2 nm) ALD coating of an adhesion layer (e.g. Si, SnO, or Al.sub.2O.sub.3) and a low-melting-temperature active material (<400° C., for example, Sn or Sn/Al alloy), which is then melted so as to cover the CNTs by wicking down the forest.
[0108] Active materials can be SnO.sub.2, SiO.sub.x, RuO.sub.2, TiO.sub.2, Cu.sub.2S. These active materials are binary compounds. Anodes can comprise a single active material layer covering VACNTs, or can comprise multiple layers of various anode active materials, such as SiO.sub.x/SnO.sub.2, or SiO.sub.x/SnO.sub.2/TiO.sub.2. In the case of multiple layers, the last active layer can also serve as protective layer, preventing the electrolyte from decomposing further at low electrochemical potential. Alternatively, the anode can be nanolamination of various materials.
[0109] Method of Making a Single Layer of SnO.sub.2:
[0110] Tetrakis(dimethylamino)tin(IV) (“TDMASn”) is employed as an Sn precursor and H.sub.2O as an oxidizing agent, has been tuned and optimized to allow coating of the high aspect ratio VACNT forest. Thermal ALD of SnO.sub.2 thin films were deposited at 200° C. using TDMASn (99.99%-Sn) and H.sub.2O. Ar gas was used as a carrier gas at a flow rate of 120 sccm. The process was performed at a purge pressure of 1.2 Torr and a deposition pressure of 10 Torr. The TDMASn precursor cylinder temperature is held at 55° C., with a dedicated 30 sccm Ar flow during cylinder charging and dosing. The ALD SnO.sub.2 sequence was as follows: [0111] TDMASn flow-through ampoule charge (1 s) with Ar gas at 30 sccm. [0112] TDMASn dose from ampoule (2 s) at 30 sccm. [0113] TDMASn exposure to sample (45 s) at 10 Torr. [0114] Chamber purge with argon (90 s) at 1.2 Torr. [0115] H.sub.2O dose from vapor-draw ampoule (0.300 s). [0116] H.sub.2O exposure to sample (60 s) at 10 Torr. [0117] Chamber purge with argon (90 s) at 1.2 Torr
The resulting layer of SnO.sub.2 is uniform and conformal from the bottom to the top of the VACNT forest, as shown
[0118] The amount of ALD active materials can well be controlled with different numbers of deposition cycles. The thickness of the deposited material can range from 0.5 nm to 50 nm. The increase of the thickness will increase the loading of the electrode and thus the areal capacity. Because of the high surface area of the 3D VACNT structure and the ability to coat tall VACNT forests, very high loading of material (mg/cm.sup.2) can be achieved while electrochemical performances are maintained due to the nano dimensions of the active material layer and the high electrical conductivity of the nanotubes.
[0119] Methods of Fabricating Cathodes and Anodes for Lithium Ion Batteries
[0120] Referring to
[0127] An alternative method is also described in
[0135] Referring to
[0142] An alternative method is also described in
[0150] Referring to
[0157] An alternative method is also described in
[0166] An additional alternative method is also described in
[0176] Referring to
[0185] An alternative method is also described in
[0192] An alternative method is also described in
[0202] Characteristics of Lithium Ion Batteries Including VACNTs
[0203] A battery cell is the basic electrochemical unit that provides the source of electrical energy through conversion of chemical energy and includes an assembly of electrodes (anode and cathode), separators, electrolyte, container, and terminals. The battery cell is a single power generating unit that has two electrodes (a cathode and an anode). The electrolyte is the chemical substance that reacts with the electrodes and produces the electric current. Types of battery cells include a cylindrical cell, a button or coin cell, a prismatic cell, and a pouch cell.
[0204] The total volume of the battery cell is calculated according to the following equation:
The energy density of a battery (Volumetric Energy) is calculated according to the following equation:
The volume ratio (VR) between the active and inactive materials is calculated according to the following equation:
In order to achieve an ideal actual battery performance, the volume ratio (VR) between the active electrode materials (active material layers) and the other battery components (substrate including VACNT forests, separator, foil, packaging) has to be maximized.
[0205] A thin film of active materials can be deposited onto the foil current collectors using ALD, CVD, and sputter methods to produce cell electrodes. Film thickness can be several nanometers to a few micrometers. Thicker films are required to achieve high loadings and thus high energy densities but would drastically reduce the rate performance (or power density). Additionally, growing a thick film on a planar substrate by ALD would take a long time and have high manufacturing cost. The deposition time can be shortened by coating a very thin film of active materials on the planar substrate, but then the VR becomes very small and the resulting energy density is low. The electrodes in conventional lithium ion batteries are usually much thicker (between 40 μm and 80 μm) and thus have a higher VR and higher energy density. By using VACNT structures, much higher areal capacity (for the same thickness) can be achieved than conventional electrode, and thus, higher energy density. Also, because the material coating thickness is kept at the nanoscale, and the VACNT provides a much greater active surface area, the resulting electrode also has much higher power density.
[0206] The volumetric energy density of a battery cell that include VACNT structures in the anode and cathode may be up to about 1700 Wh/L, alternatively up to about 1600 Wh/L, alternatively between about 500 and about 1600 Wh/L, alternatively between about 600 and about 1600 Wh/L, alternatively between 750 and about 1600 Wh/L, alternatively between about 750 and about 1400 Wh/L. The volumetric energy density of lithium ion batteries with traditional electrode structures are typically between 300 and 900 Wh/L, typically up to about 720 Wh/L. The volumetric energy density may also be as low as 20 Wh/L when constructing the battery for very high power applications (e.g. 10,000 W/L) as may be used in hybrid electric vehicles, alternatively between about 20 Wh/L to about 400 Wh/L, alternatively between about 20 Wh/L to about 300 Wh/L, alternatively between about 10 Wh/L to about 400 Wh/L.
[0207] The specific energy density or gravimetric energy density of a battery cell that includes VACNT structures in the anode and cathode may be between about 250 and about 700 Wh/kg, alternatively between about 250 and about 600 Wh/kg, alternatively between about 400 and about 600 Wh/kg, alternatively between about 500 and about 600 Wh/kg, alternatively between about 550 and about 650 Wh/kg, alternatively between about 10 and about 600 Wh/kg, alternatively between about 10 and about 500 Wh/kg, alternatively between about 10 and about 400 Wh/kg, alternatively between about 10 and about 300 Wh/kg, alternatively between about 5 and about 300 Wh/kg. The energy density of lithium ion batteries with traditional electrode structures are typically below 250 Wh/kg.
[0208] The total capacity of a battery cell that include VACNT structures in the anode and cathode can be between about 2 and about 15 mAh/cm.sup.2, alternatively between about 2 and about 9 mAh/cm.sup.2, alternatively between about 2 and about 6 mAh/cm.sup.2.
[0209] Although the foregoing invention has, for the purposes of clarity and understanding, been described in some detail by way of illustration and example, it will be obvious that certain changes and modifications may be practiced which will still fall within the scope of the appended claims.