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Barad C, Kimmel G, Opalińska A, Gierlotka S, Łojkowski W. Lattice variation as a function of concentration and grain size in MgO-NiO solid solution system. Heliyon 2024; 10:e31275. [PMID: 38803881 PMCID: PMC11129000 DOI: 10.1016/j.heliyon.2024.e31275] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/22/2023] [Revised: 03/01/2024] [Accepted: 05/14/2024] [Indexed: 05/29/2024] Open
Abstract
The study aimed to understand how changes in crystal's size affect the lattice parameters and crystal structure of Mg1-xNixO solid solution for six X values ranging from x = 0 to x = 1. Mg1-xNixO was synthesized via two different wet-chemical techniques: the sol-gel and the microwave hydrothermal method, both followed by calcination at different temperatures of 673, 873, 1073, 1273 and 1473 K. As annealing caused grain growth, the varied temperature range allowed to examine a wide range of grain sizes. The lattice parameters and x values were determined from XRD (X-ray diffraction) peak positions and intensities respectively. The grain size was evaluated by XRD line profile analysis and supported by SEM (scanning electron microscope) observations. At the temperatures of 673 and 873 K grain size was in the nanometric range and from 1073 K and above grain size was in the micrometric range. A non-monotonic lattice variation versus grain size was found for each concentration. When grain size decreased there was a slight contraction, however for grain size in the nanometric range there was a severe lattice expansion. Both lattice parameter changes were explained by two effects acting together: contraction due to surface stress and expansion due to weakening of the ionic bonding at nanocrystalline particles. In this current research study, the lattice parameter was mapped in two dimensions: concentration and grain size. The findings of this study provided valuable insights into the lattice variation in the MgO-NiO solid solution system.
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Affiliation(s)
- Chen Barad
- NRCN, P.O. Box 9001, Beer-Sheva, 84190, Israel
| | - Giora Kimmel
- Department of Materials Engineering, Ben-Gurion University of the Negev, Beer-Sheva, 84105, Israel
| | - Agnieszka Opalińska
- Institute of High Pressure Physics, Polish Academic of Sciences (PAS), Warszawa, Poland
| | - Stanislaw Gierlotka
- Institute of High Pressure Physics, Polish Academic of Sciences (PAS), Warszawa, Poland
| | - Witold Łojkowski
- Institute of High Pressure Physics, Polish Academic of Sciences (PAS), Warszawa, Poland
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Mazzucco A, Dematteis EM, Gulino V, Corno M, Sgroi MF, Palumbo M, Baricco M. Experimental and theoretical studies of the LiBH 4-LiI phase diagram. RSC Adv 2024; 14:12038-12048. [PMID: 38623301 PMCID: PMC11018216 DOI: 10.1039/d4ra01642d] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/02/2024] [Accepted: 04/08/2024] [Indexed: 04/17/2024] Open
Abstract
The hexagonal structure of LiBH4 at room temperature can be stabilised by substituting the BH4- anion with I-, leading to high Li-ion conductive materials. A thermodynamic description of the pseudo-binary LiBH4-LiI system is presented. The system has been explored investigating several compositions, synthetized by ball milling and subsequently annealed. X-ray diffraction and Differential Scanning Calorimetry have been exploited to determine structural and thermodynamic features of various samples. The monophasic zone of the hexagonal Li(BH4)1-x(I)x solid solution has been experimentally defined equal to 0.18 ≤ x ≤ 0.60 at 25 °C. In order to establish the formation of the hexagonal solid solution, the enthalpy of mixing was experimentally determined, converging to a value of 1800 ± 410 J mol-1. Additionally, the enthalpy of melting was acquired for samples that differ in molar fraction. By merging experimental results, literature data and ab initio theoretical calculations, the pseudo-binary LiBH4-LiI phase diagram has been assessed and evaluated across all compositions and temperature ranges by applying the CALPHAD method.
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Affiliation(s)
- Asya Mazzucco
- Department of Chemistry, Inter-departmental Center NIS and INSTM, University of Turin Via Pietro Giuria 7 10125 Torino Italy
| | - Erika Michela Dematteis
- Department of Chemistry, Inter-departmental Center NIS and INSTM, University of Turin Via Pietro Giuria 7 10125 Torino Italy
| | - Valerio Gulino
- Department of Chemistry, Inter-departmental Center NIS and INSTM, University of Turin Via Pietro Giuria 7 10125 Torino Italy
- Materials Chemistry and Catalysis, Debye Institute for Nanomaterials Science, Utrecht University Universiteitsweg 99 3584 CG Utrecht The Netherlands
| | - Marta Corno
- Department of Chemistry, Inter-departmental Center NIS and INSTM, University of Turin Via Pietro Giuria 7 10125 Torino Italy
| | - Mauro Francesco Sgroi
- Department of Chemistry, Inter-departmental Center NIS and INSTM, University of Turin Via Pietro Giuria 7 10125 Torino Italy
| | - Mauro Palumbo
- Department of Chemistry, Inter-departmental Center NIS and INSTM, University of Turin Via Pietro Giuria 7 10125 Torino Italy
| | - Marcello Baricco
- Department of Chemistry, Inter-departmental Center NIS and INSTM, University of Turin Via Pietro Giuria 7 10125 Torino Italy
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3
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Wei Y, Li Z, Chen Z, Gao P, Ma Q, Gao M, Yan C, Chen J, Wu Z, Jiang Y, Yu X, Zhang X, Liu Y, Yang Y, Gao M, Sun W, Pan H. Polymeric Electronic Shielding Layer Enabling Superior Dendrite Suppression for All-Solid-State Lithium Batteries. ACS NANO 2024. [PMID: 38334290 DOI: 10.1021/acsnano.4c00279] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 02/10/2024]
Abstract
LiBH4 is one of the most promising candidates for use in all-solid-state lithium batteries. However, the main challenges of LiBH4 are the poor Li-ion conductivity at room temperature, excessive dendrite formation, and the narrow voltage window, which hamper practical application. Herein, we fabricate a flexible polymeric electronic shielding layer on the particle surfaces of LiBH4. The electronic conductivity of the primary LiBH4 is reduced by 2 orders of magnitude, to 1.15 × 10-9 S cm-1 at 25 °C, due to the high electron affinity of the electronic shielding layer; this localizes the electrons around the BH4- anions, which eliminates electronic leakage from the anionic framework and leads to a 68-fold higher critical electrical bias for dendrite growth on the particle surfaces. Contrary to the previously reported work, the shielding layer also ensures fast Li-ion conduction due to the fast-rotational dynamics of the BH4- species and the high Li-ion (carrier) concentration on the particle surfaces. In addition, the flexibility of the layer guarantees its structural integrity during Li plating and stripping. Therefore, our LiBH4-based solid-state electrolyte exhibits a high critical current density (11.43 mA cm-2) and long cycling stability of 5000 h (5.70 mA cm-2) at 25 °C. More importantly, the electrolyte had a wide operational temperature window (-30-150 °C). We believe that our findings provide a perspective with which to avoid dendrite formation in hydride solid-state electrolytes and provide high-performance all-solid-state lithium batteries.
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Affiliation(s)
- Yiqi Wei
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an 710021, China
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Zhenglong Li
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an 710021, China
| | - Zichong Chen
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Panyu Gao
- Department of Materials Science, Fudan University, Shanghai 200433, China
| | - Qihang Ma
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Mingxi Gao
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Chenhui Yan
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Jian Chen
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an 710021, China
| | - Zhijun Wu
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an 710021, China
| | - Yinzhu Jiang
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Xuebin Yu
- Department of Materials Science, Fudan University, Shanghai 200433, China
| | - Xin Zhang
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Yongfeng Liu
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Yaxiong Yang
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an 710021, China
| | - Mingxia Gao
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Wenping Sun
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
| | - Hongge Pan
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an 710021, China
- State Key Laboratory of Silicon and Advanced Semiconductor Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, China
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Shu L, Gao C, Liu Y, Zhou X, Ma H, Zhang X, Shen X, Dai S, Lin C, Jiao Q. Enhancing interface stability and ionic conductivity in the designed Na 3SbP 0.4xS 4-xO x sulfide solid electrolyte through bridging oxygen. J Colloid Interface Sci 2023; 652:2042-2053. [PMID: 37696058 DOI: 10.1016/j.jcis.2023.09.013] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/10/2023] [Revised: 08/26/2023] [Accepted: 09/02/2023] [Indexed: 09/13/2023]
Abstract
The all-solid-state sodium battery has emerged as a promising candidate for energy storage. However, the limited electrochemical stability of the solid electrolyte, particularly in the presence of Na metal at the anode, along with low ionic conductivity, hinders its widespread application. In this work, the design of P and O elements in Na3SbS4 solid electrolyte was investigated through a series of structural tests and characterizations. The electrochemical stability was remarkably improved in the Na/Na3SbP0.16S3.6O0.4/Na battery, exhibiting a stability of 260 h under a current of 0.1 mA cm-2. Additionally, the room temperature conductivity of Na3SbP0.16S3.6O0.4 was enhanced to 3.82 mS cm-1, maintaining a value comparable to commercial standards. The proposed design strategy provides an approach for developing sodium ion solid-state batteries with high energy density and long lifespan. The stability of the solid electrolyte interface at the Na | solid electrolyte interface proves critical for the successful assembly of all-solid-state sodium ion batteries.
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Affiliation(s)
- Lingjun Shu
- Laboratory of Infrared Material and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China; Faculty of Information Science and Engineering, Ningbo University, Ningbo 315211, China
| | - Chengwei Gao
- Laboratory of Infrared Material and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China; Faculty of Information Science and Engineering, Ningbo University, Ningbo 315211, China
| | - Yongxing Liu
- Laboratory of Infrared Material and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China; Engineering Research Center for Advanced Infrared Photoelectric Materials and Devices of Zhejiang Province, Ningbo 315211, China
| | - Xiaolong Zhou
- Faculty of Materials Science and Engineering, Kunming University of Science and Technology, Kunming 650093, China
| | - Hongli Ma
- Laboratory of Glasses and Ceramics, Institute of Chemical Science, University of Rennes 1, UMR CNRS 6226, Rennes, France
| | - Xianghua Zhang
- Laboratory of Glasses and Ceramics, Institute of Chemical Science, University of Rennes 1, UMR CNRS 6226, Rennes, France
| | - Xiang Shen
- Laboratory of Infrared Material and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China; Faculty of Information Science and Engineering, Ningbo University, Ningbo 315211, China; Engineering Research Center for Advanced Infrared Photoelectric Materials and Devices of Zhejiang Province, Ningbo 315211, China; Ningbo Institute of Oceanography, Ningbo 315832, China
| | - Shixun Dai
- Laboratory of Infrared Material and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China
| | - Changgui Lin
- Laboratory of Infrared Material and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China; Engineering Research Center for Advanced Infrared Photoelectric Materials and Devices of Zhejiang Province, Ningbo 315211, China.
| | - Qing Jiao
- Laboratory of Infrared Material and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China; Engineering Research Center for Advanced Infrared Photoelectric Materials and Devices of Zhejiang Province, Ningbo 315211, China.
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5
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Wei Y, Yang Y, Chen Z, Gao P, Ma Q, Gao M, Yan C, Wu Z, Jiang Y, Chen J, Yu X, Li Z, Zhang X, Liu Y, Gao M, Sun W, Pan H. In-Situ-Generated Electron-Blocking LiH Enabling an Unprecedented Critical Current Density of Over 15 mA cm -2 for Solid-State Hydride Electrolytes. ADVANCED MATERIALS (DEERFIELD BEACH, FLA.) 2023; 35:e2304285. [PMID: 37487246 DOI: 10.1002/adma.202304285] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/08/2023] [Revised: 07/03/2023] [Indexed: 07/26/2023]
Abstract
LiBH4 is a promising solid-state electrolyte (SE) due to its thermodynamic stability to Li. However, poor Li-ion conductivities at room temperature, low oxidative stabilities, and severe dendrite growth hamper its application. In this work, a partial dehydrogenation strategy is adopted to in situ generate an electronic blocking layer dispersed of LiH, addressing the above three issues simultaneously. The electrically insulated LiH reduces the electronic conductivity by two orders of magnitude, leading to a 32.0-times higher critical electrical bias for dendrite growth on the particle surfaces than that of the counterpart. Additionally, this layer not only promotes the Li-ion conductance by stimulating coordinated rotations of BH4 - and B12 H12 2- , contributing to a Li-ion conductivity of 1.38 × 10-3 S cm-1 at 25 °C, but also greatly enhances oxidation stability by localizing the electron density on BH4 - , extending its voltage window to 6.0 V. Consequently, this electrolyte exhibits an unprecedented critical current density (CCD) of 15.12 mA cm-2 at 25 °C, long-term Li plating and stripping stability for 2700 h, and a wide temperature window for dendrite inhibition from -30 to 150 °C. Its Li-LiCoO2 cell displays high reversibility within 3.0-5.0 V. It is believed that this work provides a clear direction for solid-state hydride electrolytes.
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Affiliation(s)
- Yiqi Wei
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Yaxiong Yang
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an, 710021, China
| | - Zichong Chen
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Panyu Gao
- Department of Materials Science, Fudan University, Shanghai, 200433, China
| | - Qihang Ma
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Mingxi Gao
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Chenhui Yan
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Zhijun Wu
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an, 710021, China
| | - Yinzhu Jiang
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Jian Chen
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an, 710021, China
| | - Xuebin Yu
- Department of Materials Science, Fudan University, Shanghai, 200433, China
| | - Zhenglong Li
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an, 710021, China
| | - Xin Zhang
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Yongfeng Liu
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Mingxia Gao
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Wenping Sun
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
| | - Hongge Pan
- State Key Laboratory of Silicon Materials and School of Materials Science and Engineering, Zhejiang University, Hangzhou, 310027, China
- Institute of Science and Technology for New Energy, Xi'an Technological University, Xi'an, 710021, China
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6
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Nakagawa Y, Sendo T, Shibayama T. Enhanced Li-ion conductivity in LiBH 4-ZrO 2 nanocomposites and nanoscale Li imaging by energy-filtered transmission electron microscopy. Chem Commun (Camb) 2023; 59:10912-10915. [PMID: 37594117 DOI: 10.1039/d3cc02860g] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 08/19/2023]
Abstract
A complementary solid-state nuclear magnetic resonance and transmission electron microscopy (TEM) analysis was performed for LiBH4-ZrO2 nanocomposites. As a result, amorphous LiBH4 films with thicknesses of less than 30 nm were observed covering the ZrO2 particles. Li imaging by energy-filtered TEM is useful for the real-space characterization of nanoscale LiBH4.
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Affiliation(s)
- Yuki Nakagawa
- Faculty of Engineering, Hokkaido University, N-13, W-8, Sapporo 060-8628, Japan.
| | - Tsubasa Sendo
- Graduate School of Engineering, Hokkaido University, N-13, W-8, Sapporo 060-8628, Japan
| | - Tamaki Shibayama
- Faculty of Engineering, Hokkaido University, N-13, W-8, Sapporo 060-8628, Japan.
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Lu P, Xia Y, Sun G, Wu D, Wu S, Yan W, Zhu X, Lu J, Niu Q, Shi S, Sha Z, Chen L, Li H, Wu F. Realizing long-cycling all-solid-state Li-In||TiS 2 batteries using Li 6+xM xAs 1-xS 5I (M=Si, Sn) sulfide solid electrolytes. Nat Commun 2023; 14:4077. [PMID: 37429864 DOI: 10.1038/s41467-023-39686-w] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/06/2022] [Accepted: 06/26/2023] [Indexed: 07/12/2023] Open
Abstract
Inorganic sulfide solid-state electrolytes, especially Li6PS5X (X = Cl, Br, I), are considered viable materials for developing all-solid-state batteries because of their high ionic conductivity and low cost. However, this class of solid-state electrolytes suffers from structural and chemical instability in humid air environments and a lack of compatibility with layered oxide positive electrode active materials. To circumvent these issues, here, we propose Li6+xMxAs1-xS5I (M=Si, Sn) as sulfide solid electrolytes. When the Li6+xSixAs1-xS5I (x = 0.8) is tested in combination with a Li-In negative electrode and Ti2S-based positive electrode at 30 °C and 30 MPa, the Li-ion lab-scale Swagelok cells demonstrate long cycle life of almost 62500 cycles at 2.44 mA cm-2, decent power performance (up to 24.45 mA cm-2) and areal capacity of 9.26 mAh cm-2 at 0.53 mA cm-2.
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Affiliation(s)
- Pushun Lu
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Yu Xia
- Beijing ByteDance Technology Co Ltd, Beijing, 100098, China
| | - Guochen Sun
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Dengxu Wu
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Siyuan Wu
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Wenlin Yan
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Xiang Zhu
- Nano Science and Technology Institute, University of Science and Technology of China, Suzhou, 215123, China
- Tianmu Lake Institute of Advanced Energy Storage Technologies, Liyang, 213300, Jiangsu, China
| | - Jiaze Lu
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China
| | - Quanhai Niu
- Tianmu Lake Institute of Advanced Energy Storage Technologies, Liyang, 213300, Jiangsu, China
| | - Shaochen Shi
- Beijing ByteDance Technology Co Ltd, Beijing, 100098, China
| | - Zhengju Sha
- Beijing ByteDance Technology Co Ltd, Beijing, 100098, China
| | - Liquan Chen
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China
- Tianmu Lake Institute of Advanced Energy Storage Technologies, Liyang, 213300, Jiangsu, China
- Yangtze River Delta Physics Research Center, Liyang, 213300, Jiangsu, China
| | - Hong Li
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
- Nano Science and Technology Institute, University of Science and Technology of China, Suzhou, 215123, China.
- Tianmu Lake Institute of Advanced Energy Storage Technologies, Liyang, 213300, Jiangsu, China.
- Yangtze River Delta Physics Research Center, Liyang, 213300, Jiangsu, China.
| | - Fan Wu
- Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China.
- Nano Science and Technology Institute, University of Science and Technology of China, Suzhou, 215123, China.
- Tianmu Lake Institute of Advanced Energy Storage Technologies, Liyang, 213300, Jiangsu, China.
- Yangtze River Delta Physics Research Center, Liyang, 213300, Jiangsu, China.
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Yu Y, Zhang W, Cao H, He T, Chen P. Ion migration in hydride materials. TRENDS IN CHEMISTRY 2022. [DOI: 10.1016/j.trechm.2022.07.006] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
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9
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Suwarno S, Nale A, Suwarta P, Wijayanti ID, Ismail M. Designing Nanoconfined LiBH4 for Solid-State Electrolytes. Front Chem 2022; 10:866959. [PMID: 35464216 PMCID: PMC9024324 DOI: 10.3389/fchem.2022.866959] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/31/2022] [Accepted: 03/07/2022] [Indexed: 12/02/2022] Open
Abstract
Solid-state electrolytes are necessary for high-density and safe lithium-ion batteries. Lithium borohydride (LiBH4) is one of the hydride compounds that shows promising candidates for solid-state electrolytes and enables all-solid-state batteries. LiBH4 has good wetting properties and preferable mechanical properties when used in battery cells. The Li-ion conduction in LiBH4 can be modified with nanoconfinement as a result of distinct properties on the interfaces. The ion conductivities can be modified further by choosing property support materials, i.e., composition, textural properties, and surface chemistry. The present work briefly reviews the Li-ion conduction in nanoconfined LiBH4. A future perspective on the development of LiBH4 as a solid-state electrolyte is further elaborated in the last section.
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Affiliation(s)
- Suwarno Suwarno
- Department of Mechanical Engineering, Institut Teknologi Sepuluh Nopember (ITS), Surabaya, Indonesia
- *Correspondence: Suwarno Suwarno,
| | - Angeloclaudio Nale
- “Section of Chemistry for Technologies”, Department of Industrial Engineering, University of Padova, Padova, Italy
| | - Putu Suwarta
- Department of Mechanical Engineering, Institut Teknologi Sepuluh Nopember (ITS), Surabaya, Indonesia
| | - Ika Dewi Wijayanti
- Department of Mechanical Engineering, Institut Teknologi Sepuluh Nopember (ITS), Surabaya, Indonesia
| | - Mohammad Ismail
- Energy Storage Research Group, Faculty of Ocean Engineering Technology and Informatics, Universiti Malaysia Terengganu, Kuala Terengganu, Malaysia
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Effects of LiBF4 Addition on the Lithium-Ion Conductivity of LiBH4. Molecules 2022; 27:molecules27072187. [PMID: 35408587 PMCID: PMC9000853 DOI: 10.3390/molecules27072187] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/02/2022] [Revised: 03/10/2022] [Accepted: 03/22/2022] [Indexed: 12/03/2022] Open
Abstract
Complex hydrides, such as LiBH4, are a promising class of ion conductors for all-solid-state batteries, but their application is constrained by low ion mobility at room temperature. Mixing with halides or complex hydride anions, i.e., other complex hydrides, is an effective approach to improving the ionic conductivity. In the present study, we report on the reaction of LiBH4 with LiBF4, resulting in the formation of conductive composites consisting of LiBH4, LiF and lithium closo-borates. It is believed that the in-situ formation of closo-borate related species gives rise to highly conductive interfaces in the decomposed LiBH4 matrix. As a result, the ionic conductivity is improved by orders of magnitude with respect to the Li-ion conductivity of the LiBH4, up to 0.9 × 10−5 S cm−1 at 30 °C. The insights gained in this work show that the incorporation of a second compound is a versatile method to improve the ionic conductivity of complex metal hydrides, opening novel synthesis pathways not limited to conventional substituents.
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11
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Zhang R, Li H, Wang Q, Wei S, Yan Y, Chen Y. Size Effect of MgO on the Ionic Conduction Properties of a LiBH 4·1/2NH 3-MgO Nanocomposite. ACS APPLIED MATERIALS & INTERFACES 2022; 14:8947-8954. [PMID: 35142501 DOI: 10.1021/acsami.1c20976] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/14/2023]
Abstract
A solid-state electrolyte (SSE) is the core component for fabricating solid-state batteries competitive with the currently commercial Li-ion batteries. In the present study, a LiBH4·1/2NH3-MgO nanocomposite has been developed as a fast Li-ion conductor. The conductive properties depend strongly on the size of MgO nanopowders. By adding MgO nanoparticles, the first-order transition at 55 °C observed in the crystalline LiBH4·1/2NH3 is suppressed due to the conversion of LiBH4·1/2NH3 into the amorphous state. When the size of MgO decreases from 163.6 to 13.9 nm, the MgO amount required for the phase-transition suppression of LiBH4·1/2NH3 decreases linearly from 92 to 75 wt %, accompanied by a significant enhancement of ionic conductivity. The optimized nanocomposite with 75 wt % MgO of size 13.9 nm exhibits a pronouncedly high conductivity of 4.0 × 10-3 S cm-1 at room temperature, which is 20 times higher than that of the crystalline LiBH4·1/2NH3. Furthermore, a smaller size MgO contributes to a higher electrochemical stability window (ESW) owing to the stronger interfacial interaction via B-O bonds, i.e., an ESW of 4.0 V is achieved with the addition of 75 wt % MgO of size 13.9 nm.
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Affiliation(s)
- Ruixue Zhang
- Institute of New Energy and Low-Carbon Technology, Sichuan University, Chengdu 610065, China
| | - Hongjiao Li
- School of Chemical Engineering, Sichuan University, Chengdu 610065, China
| | - Qian Wang
- College of Materials Science and Engineering, Sichuan University, Chengdu 610065, China
| | - Shanghai Wei
- Department of Chemical & Materials Engineering, Faculty of Engineering, The University of Auckland, Auckland 1142, New Zealand
| | - Yigang Yan
- Institute of New Energy and Low-Carbon Technology, Sichuan University, Chengdu 610065, China
- Engineering Research Center of Alternative Energy Materials and Devices, Ministry of Education, Chengdu 610207, China
| | - Yungui Chen
- Institute of New Energy and Low-Carbon Technology, Sichuan University, Chengdu 610065, China
- Engineering Research Center of Alternative Energy Materials and Devices, Ministry of Education, Chengdu 610207, China
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12
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Murgia F, Brighi M, Piveteau L, Avalos CE, Gulino V, Nierstenhöfer MC, Ngene P, de Jongh P, Černý R. Enhanced Room-Temperature Ionic Conductivity of NaCB 11H 12 via High-Energy Mechanical Milling. ACS APPLIED MATERIALS & INTERFACES 2021; 13:61346-61356. [PMID: 34927409 DOI: 10.1021/acsami.1c21113] [Citation(s) in RCA: 6] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/14/2023]
Abstract
The body-centered cubic (bcc) polymorph of NaCB11H12 has been stabilized at room temperature by high-energy mechanical milling. Temperature-dependent electrochemical impedance spectroscopy shows an optimum at 45-min milling time, leading to an rt conductivity of 4 mS cm-1. Mechanical milling suppresses an order-disorder phase transition in the investigated temperature range. Nevertheless, two main regimes can be identified, with two clearly distinct activation energies. Powder X-ray diffraction and 23Na solid-state NMR reveal two different Na+ environments, which are partially occupied, in the bcc polymorph. The increased number of available sodium sites w.r.t. ccp polymorph raises the configurational entropy of the bcc phase, contributing to a higher ionic conductivity. Mechanical treatment does not alter the oxidative stability of NaCB11H12. Electrochemical test on a symmetric cell (Na|NaCB11H12|Na) without control of the stack pressure provides a critical current density of 0.12 mA cm-2, able to fully charge/discharge a 120 mA h g-1 specific capacity positive electrode at the rate of C/2.
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Affiliation(s)
- Fabrizio Murgia
- Laboratory of Crystallography, Department of Quantum Matter Physics, University of Geneva, Quai Ernest-Ansermet 24, CH-1211 Geneva, Switzerland
| | - Matteo Brighi
- Laboratory of Crystallography, Department of Quantum Matter Physics, University of Geneva, Quai Ernest-Ansermet 24, CH-1211 Geneva, Switzerland
| | - Laura Piveteau
- Institute of Chemical Sciences and Engineering, NMR Platform, Ecole Polytechnique Fédérale de Lausanne, Station 6, CH-1015 Lausanne, Switzerland
| | - Claudia E Avalos
- Institute of Chemical Sciences and Engineering, NMR Platform, Ecole Polytechnique Fédérale de Lausanne, Station 6, CH-1015 Lausanne, Switzerland
| | - Valerio Gulino
- Materials Chemistry and Catalysis, Debye Institute for Nanomaterials Science, Utrecht University, 3584 CG Utrecht, The Netherlands
| | - Marc C Nierstenhöfer
- Fakultät für Mathematik und Naturwissenschaften, Anorganische Chemie, Bergische Universität Wuppertal, Gaußstr. 20, 42119 Wuppertal, Germany
| | - Peter Ngene
- Materials Chemistry and Catalysis, Debye Institute for Nanomaterials Science, Utrecht University, 3584 CG Utrecht, The Netherlands
| | - Petra de Jongh
- Materials Chemistry and Catalysis, Debye Institute for Nanomaterials Science, Utrecht University, 3584 CG Utrecht, The Netherlands
| | - Radovan Černý
- Laboratory of Crystallography, Department of Quantum Matter Physics, University of Geneva, Quai Ernest-Ansermet 24, CH-1211 Geneva, Switzerland
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13
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Zettl R, Hogrefe K, Gadermaier B, Hanzu I, Ngene P, de Jongh PE, Wilkening HMR. Conductor-Insulator Interfaces in Solid Electrolytes: A Design Strategy to Enhance Li-Ion Dynamics in Nanoconfined LiBH 4/Al 2O 3. THE JOURNAL OF PHYSICAL CHEMISTRY. C, NANOMATERIALS AND INTERFACES 2021; 125:15052-15060. [PMID: 34295449 PMCID: PMC8287566 DOI: 10.1021/acs.jpcc.1c03789] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 04/28/2021] [Revised: 06/22/2021] [Indexed: 06/13/2023]
Abstract
Synthesizing Li-ion-conducting solid electrolytes with application-relevant properties for new energy storage devices is a challenging task that relies on a few design principles to tune ionic conductivity. When starting with originally poor ionic compounds, in many cases, a combination of several strategies, such as doping or substitution, is needed to achieve sufficiently high ionic conductivities. For nanostructured materials, the introduction of conductor-insulator interfacial regions represents another important design strategy. Unfortunately, for most of the two-phase nanostructured ceramics studied so far, the lower limiting conductivity values needed for applications could not be reached. Here, we show that in nanoconfined LiBH4/Al2O3 prepared by melt infiltration, a percolating network of fast conductor-insulator Li+ diffusion pathways could be realized. These heterocontacts provide regions with extremely rapid 7Li NMR spin fluctuations giving direct evidence for very fast Li+ jump processes in both nanoconfined LiBH4/Al2O3 and LiBH4-LiI/Al2O3. Compared to the nanocrystalline, Al2O3-free reference system LiBH4-LiI, nanoconfinement leads to a strongly enhanced recovery of the 7Li NMR longitudinal magnetization. The fact that almost no difference is seen between LiBH4-LiI/Al2O3 and LiBH4/Al2O3 unequivocally reveals that the overall 7Li NMR spin-lattice relaxation rates are solely controlled by the spin fluctuations near or in the conductor-insulator interfacial regions. Thus, the conductor-insulator nanoeffect, which in the ideal case relies on a percolation network of space charge regions, is independent of the choice of the bulk crystal structure of LiBH4, either being orthorhombic (LiBH4/Al2O3) or hexagonal (LiBH4-LiI/Al2O3). 7Li (and 1H) NMR shows that rapid local interfacial Li-ion dynamics is corroborated by rather small activation energies on the order of only 0.1 eV. In addition, the LiI-stabilized layer-structured form of LiBH4 guarantees fast two-dimensional (2D) bulk ion dynamics and contributes to facilitating fast long-range ion transport.
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Affiliation(s)
- Roman Zettl
- Institute
for Chemistry and Technology of Materials, Christian-Doppler-Laboratory
for Lithium Batteries, Graz University of
Technology (NAWI Graz), Stremayrgasse 9, 8010 Graz, Austria
- Materials
Chemistry and Catalysis, Debye Institute for Nanomaterials Science, Utrecht University, 3584 Utrecht, Netherlands
| | - Katharina Hogrefe
- Institute
for Chemistry and Technology of Materials, Christian-Doppler-Laboratory
for Lithium Batteries, Graz University of
Technology (NAWI Graz), Stremayrgasse 9, 8010 Graz, Austria
| | - Bernhard Gadermaier
- Institute
for Chemistry and Technology of Materials, Christian-Doppler-Laboratory
for Lithium Batteries, Graz University of
Technology (NAWI Graz), Stremayrgasse 9, 8010 Graz, Austria
| | - Ilie Hanzu
- Institute
for Chemistry and Technology of Materials, Christian-Doppler-Laboratory
for Lithium Batteries, Graz University of
Technology (NAWI Graz), Stremayrgasse 9, 8010 Graz, Austria
| | - Peter Ngene
- Materials
Chemistry and Catalysis, Debye Institute for Nanomaterials Science, Utrecht University, 3584 Utrecht, Netherlands
| | - Petra E. de Jongh
- Materials
Chemistry and Catalysis, Debye Institute for Nanomaterials Science, Utrecht University, 3584 Utrecht, Netherlands
| | - H. Martin R. Wilkening
- Institute
for Chemistry and Technology of Materials, Christian-Doppler-Laboratory
for Lithium Batteries, Graz University of
Technology (NAWI Graz), Stremayrgasse 9, 8010 Graz, Austria
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14
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Synthesis and Characterization of Lithium-Ion Conductive LATP-LaPO 4 Composites Using La 2O 3 Nano-Powder. MATERIALS 2021; 14:ma14133502. [PMID: 34201690 PMCID: PMC8269504 DOI: 10.3390/ma14133502] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 05/31/2021] [Revised: 06/17/2021] [Accepted: 06/21/2021] [Indexed: 11/17/2022]
Abstract
LATP-based composite electrolytes were prepared by sintering the mixtures of LATP precursor and La2O3 nano-powder. Powder X-ray diffraction and scanning electron microscopy suggest that La2O3 can react with LATP during sintering to form fine LaPO4 particles that are dispersed in the LATP matrix. The room temperature conductivity initially increases with La2O3 nano-powder addition showing the maximum of 0.69 mS∙cm-1 at 6 wt.%, above which, conductivity decreases with the introduction of La2O3. The activation energy of conductivity is not largely varied with the La2O3 content, suggesting that the conduction mechanism is essentially preserved despite LaPO4 dispersion. In comparison with the previously reported LATP-LLTO system, although some unidentified impurity slightly reduces the conductivity maximum, the fine dispersion of LaPO4 particles can be achieved in the LATP-La2O3 system.
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15
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Yang Q, Lu F, Liu Y, Zhang Y, Wang X, Pang Y, Zheng S. Li 2(BH 4)(NH 2) Nanoconfined in SBA-15 as Solid-State Electrolyte for Lithium Batteries. NANOMATERIALS 2021; 11:nano11040946. [PMID: 33917809 PMCID: PMC8068180 DOI: 10.3390/nano11040946] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 03/19/2021] [Revised: 04/04/2021] [Accepted: 04/06/2021] [Indexed: 12/26/2022]
Abstract
Solid electrolytes with high Li-ion conductivity and electrochemical stability are very important for developing high-performance all-solid-state batteries. In this work, Li2(BH4)(NH2) is nanoconfined in the mesoporous silica molecule sieve (SBA-15) using a melting–infiltration approach. This electrolyte exhibits excellent Li-ion conduction properties, achieving a Li-ion conductivity of 5.0 × 10−3 S cm−1 at 55 °C, an electrochemical stability window of 0 to 3.2 V and a Li-ion transference number of 0.97. In addition, this electrolyte can enable the stable cycling of Li|Li2(BH4)(NH2)@SBA-15|TiS2 cells, which exhibit a reversible specific capacity of 150 mAh g−1 with a Coulombic efficiency of 96% after 55 cycles.
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