High-entropy oxide ceramics for detecting the ionic conductivity component in electron conductors

A. V. Shlyakhtina , E. D. Baldin , N. V. Gorshkov , D. N. Stolbov , N. V. Lyskov

International Journal of Minerals, Metallurgy, and Materials ›› 2025, Vol. 32 ›› Issue (11) : 2666 -2675.

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International Journal of Minerals, Metallurgy, and Materials ›› 2025, Vol. 32 ›› Issue (11) :2666 -2675. DOI: 10.1007/s12613-025-3206-7
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High-entropy oxide ceramics for detecting the ionic conductivity component in electron conductors

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Abstract

A series of solid solutions with high content of Tb2O3–(TbxTi1−x)4O8−2x (x = 0.667–0.830) are synthesized in the Tb2O3–TiO2 system via co-precipitation and/or mechanical activation. This is followed by high-temperature annealing for 4–22 h. The X-ray diffraction method showed that the fluorite structure was realized for (TbxTi1−x)4O8−2x (x = 0.75–0.817). The solid solution Tb3.12Ti0.88O6.44 (64mol% Tb2O3 (x = 0.78)) with a fluorite structure exhibited a maximum hole conductivity of ∼22 S/cm at 600°C. To separate the ionic component of the conductivity in the electronic conductor Tb3.12Ti0.88O6.44, its high entropy analogue, (La0.2Gd0.2Tm0.2Lu0.2Y0.2)3.12Ti0.88O6.44, was synthesized in which all rare-earth elements (REE) cations exhibited valency of +3. Consequently, the contribution of ionic (proton) conductivity (∼7 × 10−6 S/cm at 600°C) was revealed with respect to the background of dominant hole conductivity. The proton conductivity of high-entropy oxide (HEO) (La0.2Gd0.2Tm0.2Lu0.2Y0.2)3.12Ti0.88O6.44 was confirmed by the detection of the isotope effect, where the mobility of the heavier O–D ions was lower than that of the O–H hydroxyls, resulting in lower conductivity in D2O vapors when compared to H2O.

Keywords

co-precipitation / mechanical activation / fluorite / (TbxTi1−x)4O8−2x / hole conductivity / proton conductivity / HEO (La0.2Gd0.2Tm0.2Lu0.2Y0.2)3.12Ti0.88O6.44

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A. V. Shlyakhtina, E. D. Baldin, N. V. Gorshkov, D. N. Stolbov, N. V. Lyskov. High-entropy oxide ceramics for detecting the ionic conductivity component in electron conductors. International Journal of Minerals, Metallurgy, and Materials, 2025, 32(11): 2666-2675 DOI:10.1007/s12613-025-3206-7

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References

[1]

Brisse A, Schefold J, Zahid M. High temperature water electrolysis in solid oxide cells. Int. J. Hydrogen Energy, 2008, 33(205375

[2]

Ni M, Leung MKH, Leung DYC. Technological development of hydrogen production by solid oxide electrolyzer cell (SOEC). Int. J. Hydrogen Energy, 2008, 33(92337

[3]

Holladay JD, Hu J, King DL, Wang Y. An overview of hydrogen production technologies. Catal. Today, 2009, 139(4244

[4]

Lyskov NV, Kolchina LM, Galin MZ, Mazo GN. Development of lanthanum-doped praseodymium cuprates as cathode materials for intermediate-temperature solid oxide fuel cells. Solid State Ion., 2018, 319: 156

[5]

Lyskov NV, Galin MZ, Napol’skii KS, Roslyakov IV, Mazo GN. Increasing the electrochemical activity of the interface Pr1.95La0.05CuO4/porous Ce0.9Gd0.1O1.95 layer by infiltrating Pr6O11. Russ. J. Electrochem., 2021, 57(111070

[6]

Kolchina LM, Lyskov NV, Pestrikov PP, Istomin SY, Mazo GN, Antipov EV. Evaluation of La18−xPrxSr0.2CuO4−δ oxides as cathode materials for IT-SOFCs. Mater. Chem. Phys., 2015, 165: 91

[7]

Lyskov NV, Kotova AI, Petukhov DI, Istomin SY, Mazo GN. A new electroactive and stable electrode based on praseodymium molybdate for symmetrical SOFCs. Russ. J. Electrochem., 2022, 58(11989

[8]

Yeh TH, Hsu WC, Chou CC. Mechanical and electrical properties of ZrO2 (3Y) doped with RENbO4 (RE = Yb, Er, Y, Dy, YNd, Sm, Nd). J. Phys. IV France, 2005, 128: 213

[9]

Yoon S, Noh T, Kim W, Choi J, Lee H. Structural parameters and oxygen ion conductivity of Y2O3–ZrO2 and MgO–ZrO2 at high temperature. Ceram. Int., 2013, 39(89247

[10]

Lee DS, Kim WS, Choi SH, Kim J, Lee HW, Lee JH. Characterization of ZrO2 co-doped with Sc2O3 and CeO2 electrolyte for the application of intermediate temperature SOFCs. Solid State Ion., 2005, 176(1–233

[11]

Shimazu M, Isobe T, Ando S, et al.. Stability of Sc2O3 and CeO2 co-doped ZrO2 electrolyte during the operation of solid oxide fuel cells. Solid State Ion., 2011, 182(1120

[12]

Shimazu M, Yamaji K, Kishimoto H, et al.. Stability of Sc2O3 and CeO2 co-doped ZrO2 electrolyte during the operation of solid oxide fuel cells: Part III. Detailed mechanism of the decomposition. Solid State Ion., 2012, 224: 6

[13]

Clarke DR, Oechsner M, Padture NP. Thermal-barrier coatings for more efficient gas-turbine engines. MRS Bull., 2012, 37(10891

[14]

Trubelja MF, Stubican VS. Ionic conductivity in the hafnia-R2O3 systems. Solid State Ion., 1991, 49: 89

[15]

Kharton VV, Naumovich EN, Yaremchenko AA, Marques FMB. Research on the electrochemistry of oxygen ion conductors in the former Soviet Union. J. Solid State Electrochem., 2001, 5(3160

[16]

T. Omata and S. Otsuka-Yao-Matsuo, Electrical properties of proton-conducting Ca2+-doped La2Zr2O7 with a pyrochlore-type structure, J. Electrochem. Soc., 148(2001), No. 6, art. No. E252.

[17]

Gorshkov N, Baldin E, Stolbov D, Vorobieva G, Shatov A, Shlyakhtina A. Proton conductivity of fluorite based rare earth titanates (LnxTi1−x)4O8−2x (Ln = Yb, Er, Ho, 0.667 ≤ x ≤ 0.765). Dalton Trans., 2024, 53(3514752

[18]

Shlyakhtina AV, Lyskov NV, Konysheva EY, et al.. Gastight proton-conducting Nd2−xCaxZr2O7−δ (x = 0, 0.05) ceramics. J. Solid State Electrochem., 2020, 24(71475

[19]

A.V. Shlyakhtina, N.V. Lyskov, G.E. Nikiforova, et al., Proton conductivity of La2(Hf2−xLax)O7−x/2 “stuffed” pyrochlores, Appl. Sci., 12(2022), No. 9, art. No. 4342.

[20]

Shlyakhtina AV, Lyskov NV, Kolbanev IV, Baldin ED, Kasyanova AV, Medvedev DA. Proton and oxygen-ion conductivity of the pure and lanthanide-doped hafnates with pyrochlore structure. Russ. J. Electrochem., 2023, 59(6449

[21]

Shlyakhtina AV, Lyskov NV, Shchegolikhin AN, et al.. Structure evolution, ionic and proton conductivity of solid solutions based on Nd2Hf2O7. Ceram. Int., 2020, 46(1117383

[22]

Shlyakhtina AV, Shcherbakova LG. New solid electrolytes of the pyrochlore family. Russ. J. Electrochem., 2012, 48(11

[23]

Shlyakhtina AV. Morphotropy, isomorphism, and polymorphism of Ln2M2O7-based (Ln = La–Lu, Y, Sc; M = Ti, Zr, Hf, Sn) oxides. Crystallogr. Rep., 2013, 58(4548

[24]

Antonova EP, Ananyev MV, Farlenkov AS, Tropin ES, Khodimchuk AV, Porotnikova NM. Phase equilibria, water dissolution, and peculiarities of charge transfer in Ca-doped La2Zr2O7−α. Russ. J. Electrochem., 2017, 53(6651

[25]

Vorotnikov VA, Belyakov SA, Plekhanov MS, et al.. Proton transfer in La2−xCa,Zr2O7−δ pyrochlores: Reasons for limited water uptake and high grain boundary conductivity. Ceram. Int., 2022, 48(2335166

[26]

Mullens BG, Zhang ZM, Avdeev M, Brand HEA, Cowie BCC, Saura Múzquiz M, Kennedy BJ. Effect of long-and short-range disorder on the oxygen ionic conductivity of Tm2(Ti2−xTmx)O7−x/2 “stuffed” pyrochlores. Inorg. Chem., 2021, 60(74517

[27]

B.G. Mullens, Z.M. Zhang, M. Avdeev, et al., Average and local ordering of Yb2(Ti2−xYbx)O7−x/2 ‘stuffed’ pyrochlores: The development of a robust structural model, J. Solid State Chem., 302(2021), art. No. 122412.

[28]

Lyskov N, Baldin E, Borunova A, Vorobieva G, Stolbov D, Shlyakhtina A. Proton conductivity in the Gd2O3–HfO2 system. New J. Chem., 2025, 49(93606

[29]

Shlyakhtina AV, Baldin ED, Vorobieva GA, Stolbov DN, Lyskov NV. Successful synthesis of proton-conducting high-entropy (La0.2Nd0.2Ho0.2Lu0.2Y0.2)2ZrO5 ceramics. Ceram. Int., 2024, 50(2040330

[30]

Lyashenko LP, Shcherbakova LG, Tartakovskii II, Maksimov AA, Svetogorov RD, Zubavichus YV. Order-disorder structural transformations in nanocrystalline highly imperfect Gd2MO5 (M = Zr and Hf) fluorite derivatives. Inorg. Mater., 2018, 54(3245

[31]

Aughterson RD, Lumpkin GR, Zhang ZM, Avdeev M, Kong LG. Crystal chemistry and ion-irradiation resistance of Ln2ZrO5 compounds with Ln = Sm, Eu, Gd, and Tb. J. Am. Ceram. Soc., 2022, 105(53521

[32]

Newman R, Aughterson RD, Lumpkin GR. Synthesis and structure of novel A2BO5 compounds containing A = Y, Yb, Gd, Sm, and La and B = Zr, Ti, and Sn. MRS Adv., 2018, 3(201117

[33]

Aughterson RD, Newman R, Ionescu M, Lumpkin GR. The ion irradiation tolerance of the fluorite RE2MO5 (RE = Sm, and Yb, M = Ti, Zr, and Sn) system. J. Aust. Ceram. Soc., 2022, 58(1287

[34]

Yusupova SG, Glushkova VB, Tikhonov PA, Mosevich AN, Kalinina MV. Variable valence of terbium and electrical properties of solid solutions (TbOx)y(YO1.5)1−y. Russ. J. Phys. Chem., 1988, 12: 2534

[35]

Tikhonov PA, Kuznetsov AK, Kravchinskaya MV, Merezhinsky KY, Zhikhareva EF. Phase relationships in the YO1.5–PrOx system and physicochemical properties of solid solutions. Izv. Akad. Nauk SSSR, Neorg. Mater., 1977, 22: 1862

[36]

Tikhonov PA, Kravchinskaya MV, Kuznetsov AK, Safonov AA, Zhikhareva EF. Physico-chemical properties of solid solutions in the YO1.5–PrOx–CaO system. Izv. Akad. Nauk SSSR, Neorg. Mater., 1983, 19(111887

[37]

Shlyakhtina AV, Abrantes JCC, Gomes E, et al.. Effect of Pr3+/Pr4+ ratio on the oxygen ion transport and thermomechanical properties of the pyrochlore and fluorite phases in the ZrO2–Pr2O3 system. Int. J. Hydrogen Energy, 2016, 41(239982

[38]

J.C.C. Abrantes, E. Gomes, and A.V. Shlyakhtina, Defect chemistry of pyrochlore Pr2O3–ZrO2 system: The relevant thermodynamic parameters. J. Solid State Electrochem., (2024). https://doi.org/10.1007/s10008-024-05995-3.

[39]

L. Grima, J.I. Pena, and M.L. Sanjuán, Pyrochlore-like ZrO2–PrOx compounds: The role of the processing atmosphere in the stoichiometry, microstructure and oxidation state, J. Alloy. Compd., 923(2022), art. No. 166449.

[40]

Komissarova LN, Shatskii VM, Pushkina GY, Shcherbakova LG, Mamsurova LG, Sukhanova GE. Soedineniya redkozemel’nykh elementov. Karbonaty, Oksalaty, Nitraty, Titanaty (Rare-Earth Compounds: Carbonates, Oxalates, Nitrates, and Titanates), 1984, Moscow, Nauka

[41]

German RM. Sintering Theory and Practice, 1996, Weinheim, Wiley-VCH

[42]

Rakhaman MN. Ceramic Processing and Sintering, 2022

[43]

Haneda M, Kintaichi Y, Hamada H. Surface reactivity of prereduced rare earth oxides with nitric oxide: New approach for NO decomposition. Phys. Chem. Chem. Phys., 2002, 4(133146

[44]

Korona DV, Partin GS, Neiman AY. Conductivity of fluorite-type Pr6−xWO12−1.5x tungstates (x = 0.5; 0.75; 1; 1.25). Russ. J. Electrochem., 2015, 51(10925

[45]

Colomban P, Slodczyk A. The structural and dynamics neutron study of proton conductors: Difficulties and improvement procedures in protonated perovskite. Eur. Phys. J. Spec. Top., 2012, 213(1171

[46]

Scherban T, Baikov Y, Shalkova E. H+/D+ isotope effect in Y-doped BaCeO3 crystals. Solid State Ion., 1993, 66(1–2159

[47]

Eurenius KEJ, Ahlberg E, Ahmed I, Eriksson SG, Knee CS. Investigation of proton conductivity in Sm1.92Ca0.08Ti2O7−δ and Sm2Ti1.92Y0.08O7−δ pyrochlores. Solid State Ion., 2010, 181(3–4148

[48]

Bonanos N, Huijser A, Poulsen FW. H/D isotope effects in high temperature proton conductors. Solid State Ion., 2015, 275: 9

[49]

M.K. Hossain, K. Kawaguchi, and K. Hashizume, Isotopic effect of proton conductivity in gadolinium sesquioxide, Fusion Eng. Des., 171(2021), art. No. 112555.

[50]

Nowick AS, Vaysleyb AV. Isotope effect and proton hopping in high-temperature protonic conductors. Solid State Ion., 1997, 97(1–417

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