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Kumagai H, Kawata S, Ogihara N. Crystal structure of dilithium biphenyl-4,4'-di-sulfonate dihydrate. Acta Crystallogr E Crystallogr Commun 2024; 80:22-24. [PMID: 38312157 PMCID: PMC10833366 DOI: 10.1107/s2056989023010411] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/31/2023] [Accepted: 12/04/2023] [Indexed: 02/06/2024]
Abstract
The asymmetric unit of the title compound, μ-biphenyl-4,4'-di-sulfonato-bis-(aqua-lithium), [Li2(C12H8O6S2)(H2O)2] or Li2[Bph(SO3)2](H2O)2, consists of an Li ion, half of the diphenyl-4,4'-di-sulfonate [Bph(SO3 -)2] ligand, and a water mol-ecule. The Li ion exhibits a four-coordinate tetra-hedral geometry with three oxygen atoms of the Bph(SO3 -)2 ligands and a water mol-ecule. The tetra-hedral LiO4 units, which are inter-connected by biphenyl moieties, form a layer structure parallel to (100). These layers are further connected by hydrogen-bonding inter-actions to yield a three-dimensional network.
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Estandarte AKC, Diao J, Llewellyn AV, Jnawali A, Heenan TMM, Daemi SR, Bailey JJ, Cipiccia S, Batey D, Shi X, Rau C, Brett DJL, Jervis R, Robinson IK, Shearing PR. Operando Bragg Coherent Diffraction Imaging of LiNi 0.8Mn 0.1Co 0.1O 2 Primary Particles within Commercially Printed NMC811 Electrode Sheets. ACS Nano 2021; 15:1321-1330. [PMID: 33355443 DOI: 10.1021/acsnano.0c08575] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/12/2023]
Abstract
Due to complex degradation mechanisms, disparities between the theoretical and practical capacities of lithium-ion battery cathode materials persist. Specifically, Ni-rich chemistries such as LiNi0.8Mn0.1Co0.1O2 (or NMC811) are one of the most promising choices for automotive applications; however, they continue to suffer severe degradation during operation that is poorly understood, thus challenging to mitigate. Here we use operando Bragg coherent diffraction imaging for 4D analysis of these mechanisms by inspecting the individual crystals within primary particles at various states of charge (SoC). Although some crystals were relatively homogeneous, we consistently observed non-uniform distributions of inter- and intracrystal strain at all measured SoC. Pristine structures may already possess heterogeneities capable of triggering crystal splitting and subsequently particle cracking. During low-voltage charging (2.7-3.5 V), crystal splitting may still occur even during minimal bulk deintercalation activity; and during discharging, rotational effects within parallel domains appear to be the precursor for the nucleation of screw dislocations at the crystal core. Ultimately, this discovery of the central role of crystal grain splitting in the charge/discharge dynamics may have ramifications across length scales that affect macroscopic performance loss during real-world battery operation.
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Affiliation(s)
- Ana Katrina C Estandarte
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
| | - Jiecheng Diao
- Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom
| | - Alice V Llewellyn
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
- The Faraday Institution, Quad One, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0RA, United Kingdom
| | - Anmol Jnawali
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
| | - Thomas M M Heenan
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
- The Faraday Institution, Quad One, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0RA, United Kingdom
| | - Sohrab R Daemi
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
| | - Josh J Bailey
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
- The Faraday Institution, Quad One, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0RA, United Kingdom
| | | | - Darren Batey
- Diamond Light Source, Didcot, Oxon OX11 0DE, United Kingdom
| | - Xiaowen Shi
- Diamond Light Source, Didcot, Oxon OX11 0DE, United Kingdom
| | - Christoph Rau
- Diamond Light Source, Didcot, Oxon OX11 0DE, United Kingdom
| | - Dan J L Brett
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
- The Faraday Institution, Quad One, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0RA, United Kingdom
| | - Rhodri Jervis
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
- The Faraday Institution, Quad One, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0RA, United Kingdom
| | - Ian K Robinson
- Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom
- The Faraday Institution, Quad One, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0RA, United Kingdom
- Brookhaven National Laboratory, Upton, New York 11973-5000, United States
| | - Paul R Shearing
- Electrochemical Innovation Lab, Department of Chemical Engineering, University College London, Torrington Place, London WC1E 7JE, United Kingdom
- The Faraday Institution, Quad One, Harwell Science and Innovation Campus, Didcot, Oxon OX11 0RA, United Kingdom
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Ahmed K, Inagaki A, Naga N. Joint-Linker Type Ionic Gels Using Polymerizable Ionic Liquid as a Crosslinker via Thiol-Ene Click Reactions. Polymers (Basel) 2020; 12:E2844. [PMID: 33260371 PMCID: PMC7760990 DOI: 10.3390/polym12122844] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/19/2020] [Revised: 11/26/2020] [Accepted: 11/27/2020] [Indexed: 11/26/2022] Open
Abstract
In this work, we report the synthesis of ion-conductive gels, or ionic gels, via thiol-ene click reactions. The novel gel systems consist of the multifunctional thiol monomers tris[(3-mercaptopropionyloxy)-ethyl]-isocyanurate (TEMPIC), pentaerythritol tetrakis(3-mercaptopropionate) (PEMP), and dipentaerythritol hexakis(3-mercaptopionate) (DPMP) as joint molecules and bifunctional allyl ionic liquid (IL) as a crosslinker. The thiol-ene reaction was carried out in lithium bis(trifluoromethanesulfonyl)imide (Li-TFSI) in a propylene carbonate (PC) (1 M) solvent system via a photopolymerization process. The chemical structure and mechanical, thermal, and conductive properties of the gels were investigated using Fourier transform infrared (FTIR) spectroscopy, thermogravimetric analysis (TGA), compression tests, and impedance spectroscopy, respectively. The mechanical and conductive properties of the ionic gels were found to be largely dependent on the monomer content and functionalities of the joint molecules. TGA revealed good thermal stability of the gels up to 100 °C. An ionic conductivity of 4.89 mS cm-1 was realized at room temperature (298 K) for low-functional thiol monomers, and a further increase in ionic conductivity was observed with an increase in Li+ ion content and temperature.
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Affiliation(s)
- Kumkum Ahmed
- SIT Research Laboratories, College of Engineering, Shibaura Institute of Technology, 3-7-5 Toyosu, Koto-ku, Tokyo 135-8548, Japan
| | - Aoi Inagaki
- Graduate School of Engineering and Science, Shibaura Institute of Technology, 3-7-5 Toyosu, Koto-ku, Tokyo 135-8548, Japan;
| | - Naofumi Naga
- Graduate School of Engineering and Science, Shibaura Institute of Technology, 3-7-5 Toyosu, Koto-ku, Tokyo 135-8548, Japan;
- Department of Applied Chemistry, College of Engineering, Shibaura Institute of Technology, 3-7-5 Toyosu, Koto-ku, Tokyo 135-8548, Japan
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Speulmanns J, Kia AM, Kühnel K, Bönhardt S, Weinreich W. Surface-Dependent Performance of Ultrathin TiN Films as an Electrically Conducting Li Diffusion Barrier for Li-Ion-Based Devices. ACS Appl Mater Interfaces 2020; 12:39252-39260. [PMID: 32805107 DOI: 10.1021/acsami.0c10950] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/11/2023]
Abstract
An in-depth understanding of lithium (Li) diffusion barriers is a crucial factor for enabling Li-ion-based devices such as three-dimensional (3D) thin-film batteries and synaptic redox transistors integrated on silicon substrates. Diffusion of Li ions into silicon can damage the surrounding components, detach the device itself, lead to battery capacity loss, and cause an uncontrolled change of the transistor channel conductance. In this study, we analyze for the first time ultrathin 10 nm titanium nitride (TiN) films as a bifunctional Li-ion diffusion barrier and current collector. Thermal atomic layer deposition (ALD) and pulsed chemical vapor deposition (pCVD) are employed for manufacturing ultrathin films. The 10 nm ALD films demonstrate excellent blocking capability with an insertion of only 0.03 Li per TiN formula unit exceeding 200 galvanostatic cycles at 3 μA/cm2 between 0.05 and 3 V versus Li/Li+. An ultralow electrical resistivity of 115 μΩ cm is obtained. In contrast, a partial barrier breakdown is observed for 10 nm pCVD films. High surface quality with low contamination is identified as a key factor for the excellent performance of ALD TiN. Conformal deposition of 10 nm ALD TiN in 3D structures with high aspect ratios of up to 20:1 is demonstrated. The measured capacities of the surface area-enhanced samples are in good agreement with the expected values. High-temperature blocking capability is proven for a typical electrode crystallization step. Ultrathin ALD TiN is an ideal candidate for an electrically conducting Li-ion diffusion barrier for Si-integrated devices.
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Affiliation(s)
- Jan Speulmanns
- Fraunhofer Institute for Photonic Microsystems (IPMS), Center Nanoelectronic Technologies (CNT), Königsbrücker Str. 178, 01099 Dresden, Germany
| | - Alireza M Kia
- Fraunhofer Institute for Photonic Microsystems (IPMS), Center Nanoelectronic Technologies (CNT), Königsbrücker Str. 178, 01099 Dresden, Germany
| | - Kati Kühnel
- Fraunhofer Institute for Photonic Microsystems (IPMS), Center Nanoelectronic Technologies (CNT), Königsbrücker Str. 178, 01099 Dresden, Germany
| | - Sascha Bönhardt
- Fraunhofer Institute for Photonic Microsystems (IPMS), Center Nanoelectronic Technologies (CNT), Königsbrücker Str. 178, 01099 Dresden, Germany
| | - Wenke Weinreich
- Fraunhofer Institute for Photonic Microsystems (IPMS), Center Nanoelectronic Technologies (CNT), Königsbrücker Str. 178, 01099 Dresden, Germany
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Kim K, Park J, Jeong G, Yu JS, Kim YC, Park MS, Cho W, Kanno R. Rational Design of a Composite Electrode to Realize a High-Performance All-Solid-State Battery. ChemSusChem 2019; 12:2637-2643. [PMID: 30895733 DOI: 10.1002/cssc.201900010] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/02/2019] [Revised: 02/28/2019] [Indexed: 06/09/2023]
Abstract
A potential solid electrolyte for realizing all-solid-state battery (ASB) technology has been discovered in the form of Li10 GeP2 S12 (LGPS), a lithium superionic conductor with a high ionic conductivity (≈12 mS cm-1 ). Unfortunately, the achievable Li+ conductivity of LGPS is limited in a sheet-type composite electrode owing to the porosity of this electrode structure. For the practical implementation of LGPS, it is crucial to control the pore structures of the composite electrode, as well as the interfaces between the active materials and solid- electrolyte particles. Herein, the addition of an ionic liquid, N-methyl-N-butylpyrrolidinium bis(trifluoromethylsulfonyl)imide ([Py14 ][TFSI]), is proposed as a pore filler for constructing a highly reliable electrode structure using LGPS. [Py14 ][TFSI] is coated onto the surface of LGPS powder through a wet process and a sheet-type composite electrode is prepared using a conventional casting procedure. The [Py14 ][TFSI]-embedded composite electrode exhibits significantly improved reversible capacity and power characteristics. It is suggested that pore-filling with [Py14 ][TFSI] is effective for increasing contact areas and building robust interfaces between the active materials and solid-electrolyte particles, leading to the generation of additional Li+ pathways in the composite electrode of ASBs.
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Affiliation(s)
- KyungSu Kim
- Advanced Batteries Research Center, Korea Electronics Technology Institute, 25 saenari-ro, Bundang-gu, Seongnam, 13509, Republic of Korea
| | - Jesik Park
- Advanced Batteries Research Center, Korea Electronics Technology Institute, 25 saenari-ro, Bundang-gu, Seongnam, 13509, Republic of Korea
| | - Goojin Jeong
- Advanced Batteries Research Center, Korea Electronics Technology Institute, 25 saenari-ro, Bundang-gu, Seongnam, 13509, Republic of Korea
| | - Ji-Sang Yu
- Advanced Batteries Research Center, Korea Electronics Technology Institute, 25 saenari-ro, Bundang-gu, Seongnam, 13509, Republic of Korea
| | - Yong-Chan Kim
- Department of Advanced Materials Engineering for Information and Electronics, Kyung Hee University, 1732 Deogyeong-daero, Giheung-gu, Yongin, 17104, Republic of Korea
| | - Min-Sik Park
- Department of Advanced Materials Engineering for Information and Electronics, Kyung Hee University, 1732 Deogyeong-daero, Giheung-gu, Yongin, 17104, Republic of Korea
| | - Woosuk Cho
- Advanced Batteries Research Center, Korea Electronics Technology Institute, 25 saenari-ro, Bundang-gu, Seongnam, 13509, Republic of Korea
| | - Ryoji Kanno
- Department of Electronic Chemistry, Interdisciplinary Graduate School of Science and Engineering, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama, 226-8502, Japan
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Markus IM, Lin F, Kam KC, Asta M, Doeff MM. Computational and Experimental Investigation of Ti Substitution in Li1(NixMnxCo1-2x-yTiy)O2 for Lithium Ion Batteries. J Phys Chem Lett 2014; 5:3649-3655. [PMID: 26278733 DOI: 10.1021/jz5017526] [Citation(s) in RCA: 17] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 06/04/2023]
Abstract
Aliovalent substitutions in layered transition-metal cathode materials has been demonstrated to improve the energy densities of lithium ion batteries, with the mechanisms underlying such effects incompletely understood. Performance enhancement associated with Ti substitution of Co in the cathode material Li1(NixMnxCo1-2x)O2 were investigated using density functional theory calculations, including Hubbard-U corrections. An examination of the structural and electronic modifications revealed that Ti substitution reduces the structural distortions occurring during delithiation due to the larger cation radius of Ti(4+) relative to Co(3+) and the presence of an electron polaron on Mn cations induced by aliovalent Ti substitution. The structural differences were found to correlate with a decrease in the lithium intercalation voltage at lower lithium concentrations, which is consistent with quasi-equilibrium voltages obtained by integrating data from stepped potential experiments. Further, Ti is found to suppress the formation of a secondary rock salt phase at high voltage. Our results provide insights into how selective substitutions can enhance the performance of cathodes, maximizing the energy density and lifetime of current Li ion batteries.
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Affiliation(s)
- Isaac M Markus
- †Materials Science and Engineering Department, University of California Berkeley, Berkeley, California 94720, United States
| | | | - Kinson C Kam
- ¶Haldor Topsøe A/S, Nymø llevej 55, 2800 Kongens Lyngby, Denmark
| | - Mark Asta
- †Materials Science and Engineering Department, University of California Berkeley, Berkeley, California 94720, United States
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Sun K, Wei TS, Ahn BY, Seo JY, Dillon SJ, Lewis JA. 3D printing of interdigitated Li-ion microbattery architectures. Adv Mater 2013; 25:4539-4543. [PMID: 23776158 DOI: 10.1002/adma.201301036] [Citation(s) in RCA: 387] [Impact Index Per Article: 35.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/07/2013] [Revised: 05/07/2013] [Indexed: 06/02/2023]
Abstract
3D interdigitated microbattery architectures (3D-IMA) are fabricated by printing concentrated lithium oxide-based inks. The microbatteries are composed of interdigitated, high-aspect ratio cathode and anode structures. Our 3D-IMA, which exhibit high areal energy and power densities, may find potential application in autonomously powered microdevices.
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Affiliation(s)
- Ke Sun
- Department of Materials Science and Engineering, University of Illinois, Urbana, IL 61801, USA
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