1
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Lin Y, Chai C, Liu Z, Wang J, Jin S, Yang Y, Gao Y, Hao M, Li X, Hou Y, Ma X, Wang B, Wang Z, Kan Y, Zheng J, Bai Y, Chen Y, Sun J, Zhao T, Law JY, Franco V, Hu F, Shen B. Large low-field-driven electrocaloric effect in organic-inorganic hybrid TMCM-CdCl 3. Nat Commun 2025; 16:4009. [PMID: 40301308 PMCID: PMC12041295 DOI: 10.1038/s41467-025-58914-z] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/12/2024] [Accepted: 04/02/2025] [Indexed: 05/01/2025] Open
Abstract
Due to environmental-friendliness and high-efficiency, electrocaloric effect (ECE) is widely regarded as a refrigeration technology for tomorrow. Herein, utilizing organic-inorganic hybridization strategy, we achieve the largest low-field-driven ECE and highest directly-measured electrocaloric strength (ECS) via packing sphere-like organic cation (CH3)3NCH2Cl+ (TMCM+) into inorganic one-dimension (1-D) CdCl3 chain framework. Single-crystal X-ray (SC-XRD) diffraction combined with Raman Spectra reveals that the simultaneous order-disorder transition of organic cations and dramatic structure change of inorganic framework are responsible for the large ECE. Moreover, the measured P-E loops and density function theory (DFT) calculations convey that the distinctive electric-field-induced metastable phase and consequential two-step meta-electric transition could lower the transition energy barrier and account for the low driving field. This work shows that the low-symmetry interaction between inorganic framework and organic cations plays a key role in achieving large ECE under low-field, which provides a method for designing high-performance electrocaloric materials via organic-inorganic hybridization.
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Grants
- 52088101, 92263202, U23A20550,22361132534 National Natural Science Foundation of China (National Science Foundation of China)
- This work was supported by the National Key Research and Development Program of China (Grant Nos. 2020YFA0711500 (J.W. and Y.Y.), 2023YFA1406003 (F.H.), 2021YFB3501202 (F.H.)), the National Natural Sciences Foundation of China (Grant Nos. 52088101 (B.S.), 92263202 (F.H.), U23A20550 (F.H.), 22361132534 (J.W. and F.H.)), and the Strategic Priority Research Program (B) of the Chinese Academy of Sciences (XDB33030200 (B.S. and F.H.)). A portion of this work was carried out at the Synergetic Extreme Condition User Facility (SECUF). J.Y.L. and V.F. acknowledge the support of AEI/FEDER-UE (grants PID2019-105720RB-I00 (J.Y.L. and V.F.) and PID2023-146047OB-I00 (J.Y.L. and V.F.) from AEI/10.13039/501100011033), and of the Chinese Academy of Sciences President's International Fellowship Initiative (PIFI) for visiting scientists (Grants No. 2024VMC0006 (J.Y.L.), 2024VMA0021 (V.F.)). J.Y.L. acknowledges an EMERGIA 2021 Fellowship (EMC21_00418 (J.Y.L.)) from Junta de Andalucía.
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Affiliation(s)
- Yuan Lin
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
| | - Congcong Chai
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing, PR China
| | - Zhijie Liu
- National Laboratory of Solid State Microstructures and Collaborative Innovation Center of Advanced Microstructures, Department of Materials Science and Engineering, Nanjing University, Nanjing, PR China
| | - Jing Wang
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China.
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China.
| | - Shifeng Jin
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China.
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China.
| | - Yurong Yang
- National Laboratory of Solid State Microstructures and Collaborative Innovation Center of Advanced Microstructures, Department of Materials Science and Engineering, Nanjing University, Nanjing, PR China.
| | - Yihong Gao
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
| | - Munan Hao
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing, PR China
| | - Xinyue Li
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- College of Materials Science and Opto-Electronic Technology, University of Chinese Academy of Sciences, Beijing, PR China
| | - Yuxuan Hou
- Beijing Advanced Innovation Center for Materials Genome Engineering, Institute for Advanced Materials and Technology, University of Science and Technology Beijing, Beijing, PR China
| | - Xingyue Ma
- National Laboratory of Solid State Microstructures and Collaborative Innovation Center of Advanced Microstructures, Department of Materials Science and Engineering, Nanjing University, Nanjing, PR China
| | - Bingjie Wang
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
| | - Zheng Wang
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
| | - Yue Kan
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
| | - Jie Zheng
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
| | - Yang Bai
- Beijing Advanced Innovation Center for Materials Genome Engineering, Institute for Advanced Materials and Technology, University of Science and Technology Beijing, Beijing, PR China
| | - Yunzhong Chen
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
| | - Jirong Sun
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
- Songshan Lake Materials Laboratory, Dongguan, Guangdong, PR China
| | - Tongyun Zhao
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- Ganjiang Innovation Academy, Chinese Academy of Sciences, Ganzhou, Jiangxi, PR China
| | - Jia Yan Law
- Multidisciplinary Unit for Energy Science, Dpto. Física de la Materia Condensada, ICMS-CSIC, Universidad de Sevilla, Sevilla, Spain
| | - Victorino Franco
- Multidisciplinary Unit for Energy Science, Dpto. Física de la Materia Condensada, ICMS-CSIC, Universidad de Sevilla, Sevilla, Spain.
| | - Fengxia Hu
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China.
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China.
- Songshan Lake Materials Laboratory, Dongguan, Guangdong, PR China.
| | - Baogen Shen
- Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China
- School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, PR China
- Ganjiang Innovation Academy, Chinese Academy of Sciences, Ganzhou, Jiangxi, PR China
- Ningbo Institute of Materials Technology & Engineering, Chinese Academy of Sciences, Ningbo, Zhejiang, PR China
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2
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Du F, Yang T, Hao H, Li S, Xu C, Yao T, Song Z, Shen J, Bai C, Luo R, Han D, Li Q, Zheng S, Zhang Y, Lin Y, Ma Z, Chen H, Guo C, Feng J, Zhong S, Mai R, Hou G, Qiu H, Xie M, Chen X, Yuan Y, Qian D, Xiang D, Chen X, Fu Z, Wang G, Liu H, Chen J, Meng G, Zhu X, Chen LQ, Zhang S, Qian X. Giant electrocaloric effect in high-polar-entropy perovskite oxides. Nature 2025; 640:924-930. [PMID: 40205056 DOI: 10.1038/s41586-025-08768-8] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/30/2024] [Accepted: 02/10/2025] [Indexed: 04/11/2025]
Abstract
Materials with a high electrocaloric effect (ECE)1,2 tend to favour a disordered yet easily tunable polar structure. Perovskite ferroelectrics3 stand out as ideal candidates owing to their high dielectric responses and reasonable thermal conductivity. The introduction of multielement atomic distortions induces a high-polar-entropy state4 that notably increases the ECE by effectively overcoming the constraints imposed by highly ordered, polar-correlated perovskite structures. Here we developed a lead-free relaxor ferroelectric with strong polar disorder through targeted multielement substitution at both the A and B sites of the perovskite, effectively distorting the lattice structure and inducing a variety of nanoscale polar configurations, polymorphic polar variants and non-polar regions. A combination of these multielement-induced features led to an increased density of interfaces, significantly enhancing the polar entropy. Remarkably, a high ECE for an entropy change of about 15 J kg-1 K-1 under a 10 MV m-1 field is observed for the material across a broad temperature range exceeding 60 °C. The formation of ultrafine, dispersed, multiphase lattice configurations leads to high-polar-entropy ferroelectric oxides with a high ECE and a long lifetime of over 1 million cycles that are suitable for manufacturing multilayer ceramic capacitors for practical electrocaloric refrigeration applications.
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Affiliation(s)
- Feihong Du
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Tiannan Yang
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Hua Hao
- State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, International School of Material Science and Engineering, Wuhan University of Technology, Wuhan, China
- Foshan Xianhu Laboratory of the Advanced Energy Science and Technology Guangdong Laboratory, Xianhu Hydrogen Valley, Foshan, China
| | - Shangshu Li
- State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, International School of Material Science and Engineering, Wuhan University of Technology, Wuhan, China
- Foshan Xianhu Laboratory of the Advanced Energy Science and Technology Guangdong Laboratory, Xianhu Hydrogen Valley, Foshan, China
| | - Chenhang Xu
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai, China
| | - Tian Yao
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Zhiwu Song
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Jiahe Shen
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Chenyun Bai
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Ruhong Luo
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Donglin Han
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Qiang Li
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Shanyu Zheng
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Yingjing Zhang
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Yezhan Lin
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Zhenhua Ma
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Haotian Chen
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Chenyu Guo
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Jiawang Feng
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Shengyi Zhong
- SJTU Paris Elite Institute of Technology and School of Materials Science and Engineering, Shanghai Jiao Tong University, Shanghai, China
- School of Materials Science and Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Ruilin Mai
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
- School of Materials Science and Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Guodong Hou
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Haixin Qiu
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Meng Xie
- State Key Laboratory of High Performance Ceramics and Superfine Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, China
| | - Xin Chen
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Yakun Yuan
- Future Material Innovation Center, School of Materials Science and Engineering, and Zhangjiang Institute for Advanced Study, Shanghai Jiao Tong University, Shanghai, China
| | - Dong Qian
- Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai, China
| | - Dao Xiang
- Future Material Innovation Center, School of Materials Science and Engineering, and Zhangjiang Institute for Advanced Study, Shanghai Jiao Tong University, Shanghai, China
- Key Laboratory for Laser Plasmas (Ministry of Education), School of Physics and Astronomy, Collaborative Innovation Center of IFSA (CICIFSA), and Tsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai, China
| | - Xuefeng Chen
- State Key Laboratory of High Performance Ceramics and Superfine Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, China
| | - Zhengqian Fu
- State Key Laboratory of High Performance Ceramics and Superfine Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, China
| | - Genshui Wang
- State Key Laboratory of High Performance Ceramics and Superfine Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, China
| | - Hanxing Liu
- State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, International School of Material Science and Engineering, Wuhan University of Technology, Wuhan, China
| | - Jiangping Chen
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Guang Meng
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Xiangyang Zhu
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Long-Qing Chen
- Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA
| | - Shujun Zhang
- Institute for Superconducting and Electronic Materials, Faculty of Engineering and Information Science, University of Wollongong, Wollongong, New South Wales, Australia.
| | - Xiaoshi Qian
- State Key Laboratory of Mechanical System and Vibration, MOE Key Laboratory for Power Machinery and Engineering, and Interdisciplinary Research Center, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China.
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3
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Wang F, Wang ZY, Luo YR, Li MD, Yang YR, Li W, Wang XL, Yang T, Shen QD. Two dimensional confinement induced discontinuous chain transitions for augmented electrocaloric cooling. Nat Commun 2025; 16:675. [PMID: 39809741 PMCID: PMC11733110 DOI: 10.1038/s41467-024-55726-5] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/26/2023] [Accepted: 12/23/2024] [Indexed: 01/16/2025] Open
Abstract
Overheating remains a major barrier to chip miniaturization, leading to device malfunction. Addressing the urgent need for thermal management promotes the development of solid-state electrocaloric cooling. However, enhancing passive heat dissipation through two-dimensional materials in electrocaloric polymers typically compromises the electrocaloric effect. In this work, we utilize two-dimensional polyamide with porous structure and hydrogen bonding to achieve multiple polar conformations with short-range order in the electrocaloric composite polymers. The structure minimizes intermolecular interactions while reducing energy barriers for field-driven polar-nonpolar conformational transitions. The electrocaloric polymer exhibits doubled cooling efficiency at electric fields as low as 40 MV m-1. Additionally, the electrode design achieves a vertical deformation of 2 millimeters, demonstrating the feasibility of self-driven electric refrigeration devices. This porous organic two-dimensional material resolves cooling efficiency limitations from spatial confinement, advancing the integration of two-dimensional materials in flexible electronics.
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Affiliation(s)
- Fang Wang
- Department of Polymer Science and Engineering, Key Laboratory of High-Performance Polymer Materials and Technology of MOE, State Key Laboratory of Analytical Chemistry for Life Science, School of Chemistry & Chemical Engineering, Nanjing University, Nanjing, China
| | - Zhong-Ye Wang
- Key Laboratory of Mesoscopic Chemistry of Ministry of Education, Institute of Theoretical and Computational Chemistry, Nanjing University, Nanjing, China
| | - Yao-Rong Luo
- National Laboratory of Solid Microstructures and Collaborative Innovation Center of Advanced Microstructures, College of Engineering and Applied Science, Nanjing University, Nanjing, China
| | - Ming-Ding Li
- Department of Polymer Science and Engineering, Key Laboratory of High-Performance Polymer Materials and Technology of MOE, State Key Laboratory of Analytical Chemistry for Life Science, School of Chemistry & Chemical Engineering, Nanjing University, Nanjing, China
- MOE Key Laboratory of Materials and Surface Technology, School of Materials Science and Engineering, Xihua University, Chengdu, China
| | - Yu-Rong Yang
- National Laboratory of Solid Microstructures and Collaborative Innovation Center of Advanced Microstructures, College of Engineering and Applied Science, Nanjing University, Nanjing, China
| | - Wei Li
- Key Laboratory of Mesoscopic Chemistry of Ministry of Education, Institute of Theoretical and Computational Chemistry, Nanjing University, Nanjing, China
| | - Xiao-Liang Wang
- Department of Polymer Science and Engineering, Key Laboratory of High-Performance Polymer Materials and Technology of MOE, State Key Laboratory of Analytical Chemistry for Life Science, School of Chemistry & Chemical Engineering, Nanjing University, Nanjing, China
| | - Tiannan Yang
- Interdisciplinary Research Centre, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China.
| | - Qun-Dong Shen
- Department of Polymer Science and Engineering, Key Laboratory of High-Performance Polymer Materials and Technology of MOE, State Key Laboratory of Analytical Chemistry for Life Science, School of Chemistry & Chemical Engineering, Nanjing University, Nanjing, China.
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4
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Jiang H, Peng R, Zhu Y, Jeong DY, Chu B. Enhanced Electrocaloric Effect of PVDF-based Polymer Composite with Surface Modified AlN. ACS APPLIED MATERIALS & INTERFACES 2024; 16:65436-65445. [PMID: 39532680 DOI: 10.1021/acsami.4c11206] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/16/2024]
Abstract
Poly(vinylidenefluoride-trifluoroethylene-chlorotrifluoroethylene) (P(VDF-TrFE-CTFE)) relaxor ferroelectric polymer exhibits a modest electrocaloric effect (ECE) at a low electric field near room temperature and a low thermal conductivity. The low thermal conductivity causes poor heat transfer when the terpolymer is used as a cooling device, even when the ECE of the polymer is substantial. By incorporating aluminum nitride (AlN) nanoparticles, which possess high thermal conductivity and good electrical insulation properties, into polymer matrices, we can enhance both the thermal conductivity and the ECE. However, weak bonding at the AlN-polymer interface can lead to a reduced breakdown electric field. Therefore, surface modification of AlN nanoparticles is performed to strengthen the chemical bonding between AlN and the terpolymer, thereby increasing the breakdown electric field. Following the addition of surface-modified nanoparticles, the breakdown electric field of the composite films remained around 240 MV/m, which is comparable to that of the pristine polymer film. Furthermore, the ECE and thermal conductivity were improved by 44% and 55%, respectively. We found three factors influencing the ECE, including the interface effect, the change in ferroelectric-paraelectric phase transition behavior, and the Joule heating effect. To assess the interfacial effect on the ECE, composite films with AlN particles of four different sizes were prepared. It was found that as the size of the nanoparticles increased, which resulted in a decreased interface area, the ECE decreased correspondingly. This finding further confirms the significant impact of the interface area in the composites on the ECE.
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Affiliation(s)
- Haitao Jiang
- CAS Key Laboratory of Materials for Energy Conversion and Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, 230026, China
| | - Rui Peng
- CAS Key Laboratory of Materials for Energy Conversion and Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, 230026, China
| | - Yuhong Zhu
- CAS Key Laboratory of Materials for Energy Conversion and Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, 230026, China
| | - Dae-Yong Jeong
- Department of Materials Science and Engineering, Inha University, Incheon, 22212, South Korea
| | - Baojin Chu
- CAS Key Laboratory of Materials for Energy Conversion and Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, 230026, China
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5
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Zhou X, Shen Q, Wang Y, Dai Y, Chen Y, Wu K. Surface and interfacial sciences for future technologies. Natl Sci Rev 2024; 11:nwae272. [PMID: 39280082 PMCID: PMC11394106 DOI: 10.1093/nsr/nwae272] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/09/2024] [Revised: 07/15/2024] [Accepted: 08/01/2024] [Indexed: 09/18/2024] Open
Abstract
Physical science has undergone an evolutional transition in research focus from solid bulks to surfaces, culminating in numerous prominent achievements. Currently, it is experiencing a new exploratory phase-interfacial science. Many a technology with a tremendous impact is closely associated with a functional interface which delineates the boundary between disparate materials or phases, evokes complexities that surpass its pristine comprising surfaces, and thereby unveils a plethora of distinctive properties. Such an interface may generate completely new or significantly enhanced properties. These specific properties are closely related to the interfacial states formed at the interfaces. Therefore, establishing a quantitative relationship between the interfacial states and their functionalities has become a key scientific issue in interfacial science. However, interfacial science also faces several challenges such as invisibility in characterization, inaccuracy in calculation, and difficulty in precise construction. To tackle these challenges, people must develop new strategies for precise detection, accurate computation, and meticulous construction of functional interfaces. Such strategies are anticipated to provide a comprehensive toolbox tailored for future interfacial science explorations and thereby lay a solid scientific foundation for several key future technologies.
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Affiliation(s)
- Xiong Zhou
- College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China
| | - Qian Shen
- Department of Interdisciplinary Sciences, National Natural Science Foundation of China, Beijing 100085, China
| | - Yongfeng Wang
- School of Electronics, Peking University, Beijing 100871, China
| | - Yafei Dai
- Department of Interdisciplinary Sciences, National Natural Science Foundation of China, Beijing 100085, China
| | - Yongjun Chen
- Department of Interdisciplinary Sciences, National Natural Science Foundation of China, Beijing 100085, China
| | - Kai Wu
- College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China
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6
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Guo J, Geng Z, Wen L, Zheng N, Yuan M, Wang K, Zhang ST. Evolution of Ferroelectricity in Sr 0.6Ba 0.4Nb 2O 6-BaTiO 3 Solid Solution with a Strong Electrocaloric Effect. ACS APPLIED MATERIALS & INTERFACES 2024; 16:43704-43712. [PMID: 39135214 DOI: 10.1021/acsami.4c06103] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 08/23/2024]
Abstract
In conventional knowledge, ferroelectric solid solutions were formed between members belonging to the same crystal structure family. Since both tungsten bronze and perovskite structures are constructed by connecting the corner-sharing oxygen octahedra, it offers a possibility for formatting an unusual solid solution between these two families. Herein, (1 - x)Sr0.6Ba0.4Nb2O6-xBaTiO3, (1 - x)SBN-xBT, solid solutions were synthesized and the solution mechanism was resolved from a structure viewpoint. With increasing BT content, the solid solution persists of tetragonal tungsten bronze structure, but the lattice parameter a (= b) decreases whereas c increases, resulting in the significant reduction of grains anisotropy. The ferroelectric-relaxor phase transition temperature shows a monotonic increase as x increases. However, the ferroelectricity evolution is not monotonous as a function of BT content because of the competitive effects of Ba and Ti on the property. As a result, the x = 0.10 ceramic shows the strongest ferroelectricity and a remarkable electrocaloric effect of 1.4 K near room temperature. This work challenges the traditional view of solid solution formation and provides an alternative way to modulate the structure and properties of ferroelectrics.
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Affiliation(s)
- Jian Guo
- National Laboratory of Solid State Microstructures, College of Engineering and Applied Sciences & Jiangsu Key Laboratory of Artificial Functional Materials & Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
- State Key Laboratory of New Ceramics and Fine Processing, School of Materials Science and Engineering, Tsinghua University, Beijing 100084, China
| | - Zhiming Geng
- National Laboratory of Solid State Microstructures, College of Engineering and Applied Sciences & Jiangsu Key Laboratory of Artificial Functional Materials & Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Lanji Wen
- College of Materials Science and Engineering, Sichuan University, Chengdu 610064, China
| | - Ningchong Zheng
- National Laboratory of Solid State Microstructures, College of Engineering and Applied Sciences & Jiangsu Key Laboratory of Artificial Functional Materials & Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Mingqian Yuan
- National Laboratory of Solid State Microstructures, College of Engineering and Applied Sciences & Jiangsu Key Laboratory of Artificial Functional Materials & Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Ke Wang
- State Key Laboratory of New Ceramics and Fine Processing, School of Materials Science and Engineering, Tsinghua University, Beijing 100084, China
| | - Shan-Tao Zhang
- National Laboratory of Solid State Microstructures, College of Engineering and Applied Sciences & Jiangsu Key Laboratory of Artificial Functional Materials & Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
- Nanjing University (Suzhou) High-tech Institute, Suzhou Industrial Park, Suzhou 215123, China
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7
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Zou K, Bai P, Li K, Luo F, Liang J, Lin L, Ma R, Li Q, Jiang S, Wang Q, Zhang G. Electronic cooling and energy harvesting using ferroelectric polymer composites. Nat Commun 2024; 15:6670. [PMID: 39107311 PMCID: PMC11303521 DOI: 10.1038/s41467-024-51147-6] [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: 02/27/2024] [Accepted: 07/29/2024] [Indexed: 08/10/2024] Open
Abstract
Thermal management emerges as a grand challenge of next-generation electronics. Efforts to develop compact, solid-state cooling devices have led to the exploration of the electrocaloric effect of ferroelectric polymers. Despite recent advances, the applications of electrocaloric polymers on electronics operating at elevated temperatures remain essentially unexplored. Here, we report that the ferroelectric polymer composite composed of highly-polarized barium strontium titanate nanofibers and electron-accepting [6,6] phenyl-C61-butyric acid methyl ester retains fast electrocaloric responses and stable cyclability at elevated temperatures. We demonstrate the effectiveness of electrocaloric cooling in a polymer composite for a pyroelectric energy harvesting device. The device utilizes a simulated central processing unit (CPU) as the heat source. Our results show that the device remains operational even when the CPU is overheated. Furthermore, we show that the composite functions simultaneously as a pyroelectric energy converter to harvest thermal energy from an overheated chip into electricity in the electrocaloric process. This work suggests a distinct approach for overheating protection and recycling waste heat of microelectronics.
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Affiliation(s)
- Kailun Zou
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, China
| | - Peijia Bai
- School of Materials Science and Engineering, National Institute for Advanced Materials, Nankai University, Tianjin, China
| | - Kanghua Li
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, China
| | - Fangyuan Luo
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, China
| | - Jiajie Liang
- State Key Laboratory of Power System, Department of Electrical Engineering, Tsinghua University, Beijing, China
| | - Ling Lin
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, China
| | - Rujun Ma
- School of Materials Science and Engineering, National Institute for Advanced Materials, Nankai University, Tianjin, China.
| | - Qi Li
- State Key Laboratory of Power System, Department of Electrical Engineering, Tsinghua University, Beijing, China.
| | - Shenglin Jiang
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, China
| | - Qing Wang
- Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA.
| | - Guangzu Zhang
- School of Integrated Circuits, Huazhong University of Science and Technology, Wuhan, China.
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Han D, Zhang Y, Huang C, Zheng S, Wu D, Li Q, Du F, Duan H, Chen W, Shi J, Chen J, Liu G, Chen X, Qian X. Self-oscillating polymeric refrigerator with high energy efficiency. Nature 2024; 629:1041-1046. [PMID: 38720078 DOI: 10.1038/s41586-024-07375-3] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/29/2023] [Accepted: 04/02/2024] [Indexed: 05/31/2024]
Abstract
Electrocaloric1,2 and electrostrictive3,4 effects concurrently exist in dielectric materials. Combining these two effects could achieve the lightweight, compact localized thermal management that is promised by electrocaloric refrigeration5. Despite a handful of numerical models and schematic presentations6,7, current electrocaloric refrigerators still rely on external accessories to drive the working bodies8-10 and hence result in a low device-level cooling power density and coefficient of performance (COP). Here we report an electrocaloric thin-film device that uses the electro-thermomechanical synergy provided by polymeric ferroelectrics. Under one-time a.c. electric stimulation, the device is thermally and mechanically cycled by the working body itself, resulting in an external-driver-free, self-cycling, soft refrigerator. The prototype offers a directly measured cooling power density of 6.5 W g-1 and a peak COP exceeding 58 under a zero temperature span. Being merely a 30-µm-thick polymer film, the device achieved a COP close to 24 under a 4 K temperature span in an open ambient environment (32% thermodynamic efficiency). Compared with passive cooling, the thin-film refrigerator could immediately induce an additional 17.5 K temperature drop against an electronic chip. The soft, polymeric refrigerator can sense, actuate and pump heat to provide automatic localized thermal management.
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Affiliation(s)
- Donglin Han
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Yingjing Zhang
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Cenling Huang
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Shanyu Zheng
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Dongyuan Wu
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Qiang Li
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Feihong Du
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Hongxiao Duan
- School of Electronic Information and Electrical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Weilin Chen
- School of Electronic Information and Electrical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Junye Shi
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Jiangping Chen
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Gang Liu
- School of Electronic Information and Electrical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Xin Chen
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China
| | - Xiaoshi Qian
- State Key Laboratory of Mechanical System and Vibration, Interdisciplinary Research Center, Institute of Refrigeration and Cryogenics, and MOE Key Laboratory for Power Machinery and Engineering, School of Mechanical Engineering, Shanghai Jiao Tong University, Shanghai, China.
- Shanghai Jiao Tong University Zhongguancun Research Institute, Liyang, China.
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Wei XH, Wu ZP, Peng A, Zhang XA, Merlitz H, Forest MG, Wu CX, Cao XZ. Depletion Strategies for Crystallized Layers of Two-Dimensional Nanosheets to Enhance Lithium-Ion Conductivity in Polymer Nanocomposites. ACS Macro Lett 2024; 13:453-460. [PMID: 38552169 DOI: 10.1021/acsmacrolett.3c00756] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 04/17/2024]
Abstract
The assembly of long-range aligned structures of two-dimensional nanosheets (2DNSs) in polymer nanocomposites (PNCs) is in urgent need for the design of nanoelectronics and lightweight energy-storage materials of high conductivity for electricity or heat. These 2DNS are thin and exhibit thermal fluctuations, leading to an intricate interplay with polymers in which entropic effects can be exploited to facilitate a range of different assemblies. In molecular dynamics simulations of experimentally studied 2DNSs, we show that the layer-forming crystallization of 2DNSs is programmable by regulating the strengths and ranges of polymer-induced entropic depletion attractions between pairs of 2DNSs, as well as between single 2DNSs and a substrate surface, by exclusively tuning the temperature and size of the 2DNS. Enhancing the temperature supports the 2DNS-substrate depletion rather than crystallization of 2DNSs in the bulk, leading to crystallized layers of 2DNSs on the substrate surfaces. On the other hand, the interaction range of the 2DNS-2DNS depletion attraction extends further than the 2DNS-substrate attraction whenever the 2DNS size is well above the correlation length of the polymers, which results in a nonmonotonic dependence of the crystallization layer on the 2DNS size. It is demonstrated that the depletion-tuned crystallization layers of 2DNSs contribute to a conductive channel in which individual lithium ions (Li ions) migrate efficiently through the PNCs. This work provides statistical and dynamical insights into the balance between the 2DNS-2DNS and 2DNS-substrate depletion interactions in polymer-2DNS composites and highlights the possibilities to exploit depletion strategies in order to engineer crystallization processes of 2DNSs and thus to control electrical conductivity.
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Affiliation(s)
- Xiao-Han Wei
- Department of Physics, Xiamen University, Xiamen 361005, People's Republic of China
| | - Zong-Pei Wu
- Department of Physics, Xiamen University, Xiamen 361005, People's Republic of China
| | - Ao Peng
- School of Informatics, Xiamen University, Xiamen 361005, People's Republic of China
| | - Xue-Ao Zhang
- Department of Physics, Xiamen University, Xiamen 361005, People's Republic of China
| | - Holger Merlitz
- Leibniz-Institut für Polymerforschung Dresden, 01069 Dresden, Germany
| | - M Gregory Forest
- Departments of Mathematics, Applied Physical Sciences and Biomedical Engineering, University of North Carolina at Chapel Hill, Chapel Hill, North Carolina 27599-3250, United States
| | - Chen-Xu Wu
- Department of Physics, Xiamen University, Xiamen 361005, People's Republic of China
| | - Xue-Zheng Cao
- Department of Physics, Xiamen University, Xiamen 361005, People's Republic of China
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