Journal Home > Volume 12 , Issue 9

Semiconductor materials with heterogeneous interfaces and twin structures generally demonstrate a higher concentration of carriers and better electrical stability. A variety of Cu-doped Co0.98CuxMn2.02−xO4 (0 ≤ x ≤ 0.5) negative temperature coefficient (NTC) ceramics with dual phases and twin structures were successfully prepared in this study. Rietveld refinement indicates that the content of a cubic spinel phase increases with increasing Cu content. The addition of Cu can promote grain growth and densification. Atomic-level structural characterization reveals the evolution of twin morphology from large lamellae with internal fine lamellae (LIT lamellae) to large lamellae without internal fine lamellae (L lamellae) and the distribution of twin boundary defects. First-principles calculations reveal that the dual phases and twin structures have lower oxygen-vacancy formation energy than those in the case of the pure tetragonal and cubic spinel, thereby enhancing the transmission of carriers. Additionally, the three-dimensional charge-density difference shows that metal ions at the interface lose electrons and dwell in high valence states, thereby enhancing electrical stability of the NTC ceramics. Furthermore, the additional Cu ions engage in electron-exchange interactions with Mn and Co ions, thereby reducing resistivity. In comparison to previous Cu-containing systems, the Co0.98CuxMn2.02−xO4 series exhibit superior stability (aging value ≤ 2.84%), tunable room-temperature resistivity (ρ), and material constant (B) value (17.5 Ω·cm ≤ ρ ≤ 7325 Ω·cm, 2836 K ≤ B ≤ 4315 K). These discoveries lay a foundation for designing and developing new NTC ceramics with ultra-high performance.


menu
Abstract
Full text
Outline
About this article

Enhanced conductivity and stability of Co0.98CuxMn2.02−xO4 ceramics with dual phases and twin structures

Show Author's information Chengjian Maa( )Longhua HebLei BicHong GaodJianxiang Dinge
Analytical and Testing Center, Yancheng Institute of Technology, Yancheng 224051, China
School of Materials Science and Engineering, Yancheng Institute of Technology, Yancheng 224051, China
School of Resource Environment and Safety Engineering, University of South China, Hengyang 421001, China
School of Mathematics and Physics, Yancheng Institute of Technology, Yancheng 224051, China
School of Materials Science and Engineering, Anhui University of Technology, Ma’anshan 243002, China

Abstract

Semiconductor materials with heterogeneous interfaces and twin structures generally demonstrate a higher concentration of carriers and better electrical stability. A variety of Cu-doped Co0.98CuxMn2.02−xO4 (0 ≤ x ≤ 0.5) negative temperature coefficient (NTC) ceramics with dual phases and twin structures were successfully prepared in this study. Rietveld refinement indicates that the content of a cubic spinel phase increases with increasing Cu content. The addition of Cu can promote grain growth and densification. Atomic-level structural characterization reveals the evolution of twin morphology from large lamellae with internal fine lamellae (LIT lamellae) to large lamellae without internal fine lamellae (L lamellae) and the distribution of twin boundary defects. First-principles calculations reveal that the dual phases and twin structures have lower oxygen-vacancy formation energy than those in the case of the pure tetragonal and cubic spinel, thereby enhancing the transmission of carriers. Additionally, the three-dimensional charge-density difference shows that metal ions at the interface lose electrons and dwell in high valence states, thereby enhancing electrical stability of the NTC ceramics. Furthermore, the additional Cu ions engage in electron-exchange interactions with Mn and Co ions, thereby reducing resistivity. In comparison to previous Cu-containing systems, the Co0.98CuxMn2.02−xO4 series exhibit superior stability (aging value ≤ 2.84%), tunable room-temperature resistivity (ρ), and material constant (B) value (17.5 Ω·cm ≤ ρ ≤ 7325 Ω·cm, 2836 K ≤ B ≤ 4315 K). These discoveries lay a foundation for designing and developing new NTC ceramics with ultra-high performance.

Keywords: negative temperature coefficient (NTC) ceramics, first-principles calculation, Cu-containing spinel, high electrical stability, twin structure, electron-exchange interaction

References(62)

[1]
Shin J, Jeong B, Kim J, et al. Sensitive wearable temperature sensor with seamless monolithic integration. Adv Mater 2020, 32: e1905527.
[2]
Katerinopoulou D, Zalar P, Sweelssen J, et al. Large-area all-printed temperature sensing surfaces using novel composite thermistor materials. Adv Electron Mater 2019, 5: 1800605.
[3]
Feteira A. Negative temperature coefficient resistance (NTCR) ceramic thermistors: An industrial perspective. J Am Ceram Soc 2009, 92: 967983.10.1111/j.1551-2916.2009.02990.x
[4]
Moulson AJ, Herbert JM. Electroceramics: Materials, Properties, Applications, 2nd edn. Wiley, 2003.
DOI
[5]
Larson EG, Arnott RJ, Wickham DG. Preparation, semiconduction and low-temperature magnetization of the system Ni1−xMn12+xO4. J Phys Chem Solids 1962, 23: 1771–1781.
[6]
Kshirsagar ST. Electrical and crystallographic studies of the system CuxNi1–xMn2O4. J Phys Soc Jpn 1969, 27: 1164–1170.
[7]
Rousset A, Tenailleau C, Dufour P, et al. Electrical properties of Mn3–xCoxO4 (0 ≤ x ≤ 3) ceramics: An interesting system for negative temperature coefficient thermistors. Int J Appl Ceram Technol 2013, 10: 175185.10.1111/j.1744-7402.2011.02723.x
[8]
Gillot B, Kharroubi M, Metz R, et al. Electrical properties and cationic distribution in cubic nickel manganite spinels NixMn3−xO4, 0.5 < x < 1. Solid State Ion 1991, 44: 275–280.
[9]
Vila E, Rojas RM, Martin De Vidales JL, et al. Structural and thermal properties of the tetragonal cobalt manganese spinels MnxCo3–xO4 (1.4 < x < 2.0). Chem Mater 1996, 8: 1078−1083.
[10]
Bordeneuve H, Guillemet-Fritsch S, Rousset A, et al. Structure and electrical properties of single-phase cobalt manganese oxide spinels Mn3−xCoxO4 sintered classically and by spark plasma sintering (SPS). J Solid State Chem 2009, 182: 396–401.
[11]
Park K, Lee JK. Mn–Ni–Co–Cu–Zn–O NTC thermistors with high thermal stability for low resistance applications. Scripta Mater 2007, 57: 329–332.
[12]
Dinger J, Reimann T, Ovodok E, et al. Cation distribution in NiMn2O4 spinel probed by high temperature thermopower measurements. J Alloys Compd 2021, 865: 158909.
[13]
Dojcinovic MP, Vasiljevic ZZ, Krstic JB, et al. Electrospun nickel manganite (NiMn2O4) nanocrystalline fibers for humidity and temperature sensing. Sensors 2021, 21: 4357.
[14]
Li HB, Zhang HM, Thayil S, et al. Enhanced aging and thermal shock performance of Mn1.95–xCO0.21Ni0.84SrxO4 NTC ceramics. J Adv Ceram 2021, 10: 258–270.
[15]
Vakiv M, Shpotyuk O, Mrooz O, et al. Controlled thermistor effect in the system CuxNi1–xyCo2yMn2–yO4. J Eur Ceram Soc 2001, 21: 17831785.10.1016/S0955-2219(01)00115-7
[16]
Wang ZB, Li ZB, Zhang Y, et al. Preparation and electrical properties of Ni0.6Mn2.4−xSnxO4 NTC ceramics. Ceram Int 2014, 40: 4875–4878.
[17]
Yao JC, Wang JH, Zhao Q, et al. Effect of La2O3 addition on copper–nickel manganese thermistors for low-temperature applications. Int J Appl Ceram Technol 2013, 10: E106–E112.
[18]
Zhao CH, Wang BY, Yang PH, et al. Effects of Cu and Zn co-doping on the electrical properties of Ni0.5Mn2.5O4 NTC ceramics. J Eur Ceram Soc 2008, 28: 35–40.
[19]
Zhao C, Zhao Y. The investigation of Zn content on the structure and electrical properties of ZnxCu0.2Ni0.66Mn2.14−xO4 negative temperature coefficient ceramics. J Mater Sci Mater Electron 2012, 23: 1788–1792.
[20]
Ma CJ, Liu YF, Lu YN, et al. Effect of Zn substitution on the phase, microstructure and electrical properties of Ni0.6Cu0.5ZnxMn1.9–xO4 (0 ≤ x ≤ 1) NTC ceramics. Mater Sci Eng B 2014, 188: 66–71.
[21]
Le DT, Cho JH, Ju H. Electrical properties and stability of low temperature annealed (Zn,Cu) co-doped (Ni,Mn)3O4 spinel thin films. J Asian Ceram Soc 2021, 9: 838–850.
[22]
Legros R, Metz R, Rousset A. The preparation, characterization and electrical properties of electroceramics made of copper—Cobalt manganite spinel: Mn2.6−xCo0.4CuxO4, 0 ≤ x ≤ 1. J Eur Ceram Soc 1995, 15: 463468.10.1016/0955-2219(95)00007-H
[23]
Metz R, Caffin JP, Legros R, et al. The preparation, characterization and electrical properties of copper manganite spinels, CuxMn3−xO4, 0 ≤ x ≤ 1. J Mater Sci 1989, 24: 8387.10.1007/BF00660936
[24]
Metz R. Electrical properties of N.T.C. thermistors made of manganite ceramics of general spinel structure: Mn3–xxMxNxO4 (0 ≤ x + x′ ≤ 1; M and N being Ni, Co or Cu). Aging phenomenon study. J Mater Sci 2000, 35: 47054711.
[25]
Li DF, Zhao SX, Xiong K, et al. Aging improvement in Cu-containing NTC ceramics prepared by co-precipitation method. J Alloys Compd 2014, 582: 283–288.
[26]
Aleksic OS, Nikolic MV, Lukovic MD, et al. Preparation and characterization of Cu and Zn modified nickel manganite NTC powders and thick film thermistors. Mater Sci Eng B 2013, 178: 202–210.
[27]
Zhao CH, Wang ZB, Wang SM, et al. Preparation and characterization of negative temperature coefficient (Ni,Mn)3O4–La(Mn,Ni)O3 composite. J Electroceram 2008, 20: 113–117.
[28]
Guan F, Zhang HM, Chang AM, et al. Effect of CaO-doped in NiMn2O4–LaMnO3 composite ceramics on microstructure and electrical properties. J Mater Sci Mater Electron 2012, 23: 1728–1733.
[29]
Jagtap S, Rane S, Gosavi S, et al. Preparation, characterization and electrical properties of spinel-type environment friendly thick film NTC thermistors. J Eur Ceram Soc 2008, 28: 2501–2507.
[30]
Jagtap S, Rane S, Gosavi S, et al. Ruthenium dioxide doped manganite-based NTC thermistors for low-resistance applications. Microelectron Int 2009, 26: 19–23.
[31]
Jagtap S, Rane S, Aiyer R, et al. Study of microstructure, impedance and dc electrical properties of RuO2-spinel based screen printed ‘green’ NTC thermistor. Curr Appl Phys 2010, 10: 1156–1163.
[32]
Ma CJ, Li N, Gao H, et al. Effect of Ag addition on the microstructure and electrical properties of Ni0.6CoMn1.4O4/Ag composite ceramics. J Alloys Compd 2022, 900: 163528.
[33]
Yang BW, Feng YF, Deng XQ, et al. RuO2 doping and its influence on phase structure, cations state, and electrical properties of Mn1.6Co0.4CuO4 ceramics. Ceram Int 2021, 47: 2107–2114.
[34]
Sun J, Xue H, Zhang YF, et al. Unraveling the synergistic effect of heteroatomic substitution and vacancy engineering in CoFe2O4 for superior electrocatalysis performance. Nano Lett 2022, 22: 3503–3511.
[35]
Wang R, Chen X, Huang ZY, et al. Twin boundary defect engineering improves lithium-ion diffusion for fast-charging spinel cathode materials. Nat Commun 2021, 12: 3085.
[36]
Brieu M, Couderc JJ, Rousset A, et al. TEM characterization of nickel and nickel–cobalt manganite ceramics. J Eur Ceram Soc 1993, 11: 171–177.
[37]
Metzmacher C, Groen WA, Reaaney IM. Microstructure and electrical properties of Mn–Ni–In spinels. Phys Stat Sol A 2000, 181: 369–386.
DOI
[38]
Groen WA, Metzmacher C, Zaspalis V, et al. Aging of NTC ceramics in the system Mn–Ni–Fe–O. J Eur Ceram Soc 2001, 21: 1793–1796.
[39]
El Horr N, Guillemet-Fritsch S, Rousset A, et al. Microstructure of single-phase cobalt and manganese oxide spinel Mn3−xCoxO4 ceramics. J Eur Ceram Soc 2014, 34: 317–326.
[40]
Ma CJ, Liu YF, Lyu YN. Investigation of multiply twins in Mn2.02Co0.98O4 ceramic by means of transmission electron microscopy. J Am Ceram Soc 2016, 99: 3458–3466.
[41]
Ma CJ, Gao H. TEM and electrical properties characterizations of Co0.98Mn2.02O4 NTC ceramic. J Alloys Compd 2018, 749: 853–858.
[42]
Kukuruznyak DA, Moyer JG, Prowse MS, et al. Relationship between electronic and crystal structure in Cu–Ni–Co–Mn–O spinels. J Electron Spectrosc Relat Phenom 2006, 150: 282–287.
[43]
Jeon JE, Park KR, Kim KM, et al. Effect of Cu/Fe addition on the microstructures and electrical performances of Ni–Co–Mn oxides. J Alloys Compd 2021, 859: 157769.
[44]
Li HQ, Liu JS, Yu HT, et al. Relaxor behavior and Raman spectra of CuO-doped Pb(Mg1/3Nb2/3)O3–PbTiO3 ferroelectric ceramics. J Adv Ceram 2014, 3: 177–183.
[45]
Chen T, Liang RH, Jiang K, et al. Low-temperature sintering and electrical properties of Sr2Nb2O7 piezoceramics by CuO addition. J Am Ceram Soc 2017, 100: 2397–2401.
[46]
Couderc JJ, Fritsch S, Brieu M, et al. A transmission electron microscopy study of lattice defects in Mn3O4 hausmannite. Philos Mag B 1994, 70: 1077–1094.
[47]
Nesbitt HW, Banerjee D. Interpretation of XPS Mn(2p) spectra of Mn oxyhydroxides and constraints on the mechanism of MnO2 precipitation. Am Mineral 1998, 83: 305–315.
[48]
Beyreuther E, Grafström S, Eng LM, et al. XPS investigation of Mn valence in lanthanum manganite thin films under variation of oxygen content. Phys Rev B 2006, 73: 155425.
[49]
Drouet C, Laberty C, Fierro JLG, et al. X-ray photoelectron spectroscopic study of non-stoichiometric nickel and nickel–copper spinel manganites. Int J Inorg Mater 2000, 2: 419–426.
[50]
Gillot B, Buguet S, Kester E, et al. Cation valencies and distribution in the spinels CoxCuyMnzFeuO4+δ (δ ≥ 0) thin films studied by X-ray photoelectron spectroscopy. Thin Solid Films 1999, 357: 223–231.
[51]
Töpfer J, Feltz A, Gräf D, et al. Cation valencies and distribution in the spinels NiMn2O4 and MzNiMn2–zO4 (M = Li, Cu) studied by XPS. Phys Stat Sol (a) 1992, 134: 405415.10.1002/pssa.2211340211
[52]
Chen XY, Li XH, Gao B, et al. A novel NTC ceramic based on La2Zr2O7 for high-temperature thermistor. J Eur Ceram Soc 2022, 42: 2561–2564.
[53]
Li RF, Fu QY, Zou XH, et al. Mn–Co–Ni–O thin films prepared by sputtering with alloy target. J Adv Ceram 2020, 9: 64–71.
[54]
Vandenberghe RE, Robbrect GG, Brabers VAM. Structure and ionic configuration of oxidic copper-manganese spinels (CuxMn3–xO4). Phys Stat Sol (a) 1976, 34: 583–592.
[55]
Suzuki M. AC hopping conduction in Mn–Co–Ni–Cu complex oxide semiconductors with spinel structure. J Phys Chem Solids 1980, 41: 12531260.10.1016/0022-3697(80)90160-2
[56]
Elbadraoui E, Baudour JL, Bouree F, et al. Cation distribution and mechanism of electrical conduction in nickel-copper manganite spinels. Solid State Ion 1997, 93: 219–225.
[57]
Dorris SE, Mason TO. Electrical properties and cation valencies in Mn3O4. J Am Ceram Soc 1988, 71: 379–385.
[58]
He ZL, Li ZC, Xiang QH, et al. Electrical properties of Y/Mg modified NiO simple oxides for negative temperature coefficient thermistors. Int J Appl Ceram Technol 2019, 16: 160–169.
[59]
Muralidharan MN, Rohini PR, Sunny EK, et al. Effect of Cu and Fe addition on electrical properties of Ni–Mn–Co–O NTC thermistor compositions. Ceram Int 2012, 38: 6481–6486.
[60]
Guan MY, Yao JC, Kong WW, et al. Effects of Zn-doped on the microstructure and electrical properties of Mn1.5−xCo1.2Cu0.3ZnxO4 (0 ≤  x ≤  0.5) NTC ceramics. J Mater Sci Mater Electron 2018, 29: 50825086.10.1007/s10854-017-8471-4
[61]
Xiong K, Zhao SX, Li DF, et al. Structure and electrical performance of Mn1.5−0.5xCo0.9−0.3xNi0.6−0.2xCuxO4 NTC ceramics prepared by heterogeneous precipitation. J Alloys Compd 2014, 606: 273–277.
[62]
Battault T, Legros R, Brieu M, et al. Correlation between microstructure and ageing of iron manganite thermistors. J Phys III France 1997, 7: 979–992.
Publication history
Copyright
Acknowledgements
Rights and permissions

Publication history

Received: 09 April 2023
Revised: 07 June 2023
Accepted: 26 June 2023
Published: 05 September 2023
Issue date: September 2023

Copyright

© The Author(s) 2023.

Acknowledgements

This work was supported by the National Natural Science Foundation of China (Grant No. 52002347), and Natural Science Foundation of the Jiangsu Higher Education Institutions of China (Grant No. 19KJB430039). The authors would like to thank Shiyanjia Lab (www.shiyanjia. com) for the language editing service.

Rights and permissions

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made.

The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder.

To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.

Return