Mechanochemical synthesis, crystal structure and ion conduction in the Gd2Hf2−x Ti x O7 system
Source abstract
Abstract
This work describes the mechanochemical synthesis, structural characterization and electrical properties of an interesting group of novel ionic conductors, with general formula Gd2(Hf2−x Ti x )2O7. Different compositions in this system (x = 0, 0.4, 0.8, 1.2, 1.6 and 2) were obtained at room temperature, via a mechanochemical reaction between the corresponding elemental oxides, and characterized by using XRD, Raman spectroscopy and SEM. The XRD structural analysis by the Rietveld method revealed that all the Hf-containing compositions show a disordered fluorite-like structure instead of the expected pyrochlore-like atomic ordering, and the cation size mismatch criteria for pyrochlore stability. Increasing Ti content promotes a phase transformation to the pyrochlore structure with post-milling thermal treatments, which takes place in all samples on annealing at 1200 °C, except for Gd2Hf2O7. These results were confirmed by Raman spectroscopy, which also suggests that the x = 0.4 sample has the highest degree of oxygen disorder in the system and that this disorder decreases with increasing Ti4+ content. Finally, all samples show the pyrochlore structure on firing at 1500 °C. Activation energies E dc for oxygen migration were determined by using impedance spectroscopy and found to be within the ~0.9–1.2 eV range, whereas conductivity σ dc values at 700 °C vary from 1.12 × 10−6 to 2.75 × 10−4 S cm−1, with decreasing conductivity as Ti4+ content increases.
Source: openaire · Quality: candidate unverified · Source record ↗
Research context
OpenAlex topics: Nuclear materials and radiation effects · Advanced Condensed Matter Physics · Microwave Dielectric Ceramics Synthesis
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (44)
Show source-provided references
1. Gardner JS, Gingras MJP, Greedan JE (2010) Magnetic pyrochlore oxides. Rev Mod Phys 82:53–10710.1103/RevModPhys.82.53 ↗
2. Ramirez AP, Hayashi A, Cava RJ, Siddharthan R, Sastry BS (1999) Zero-point entropy in “spin-ice”. Nature 399:333–33510.1038/20619 ↗
3. Levi CG (2004) Emerging materials and processes for thermal barrier systems. Curr Opin Solid State Mat Sci 8:77–9110.1016/j.cossms.2004.03.009 ↗
4. Sickafus KE, Minervini L, Grimes RW, Valdez JA, Ishimaru M, Li F, McClellan KJ, Hartmann T (2000) Radiation tolerance of complex oxides. Science 289:748–75110.1126/science.289.5480.748 ↗
5. Van Dijk T, de Vries KJ, Burggraaf AJ (1980) Electrical conductivity of fluorite and pyrochlore LnxZr1-xO2−x/2 (Ln = Gd, Nd) solid solutions. Phys Stat Sol A 58:115–12510.1002/pssa.2210580114 ↗
6. Burggraaf AJ, van Dijk T, Verkerk MJ (1981) Structure and conductivity of pyrochlore and fluorite type solid solutions. Solid State Ion 5:519–52210.1016/0167-2738(81)90306-4 ↗
7. Van Dijk MP, de Vries KJ, Burggraaf AJ (1985) Electrical conductivity and defect chemistry in the system (Tb x Gd1-x )2Zr2O7+y , (0 ≤ x ≤ 1; 0 ≤ y ≤ 0.25). Solid State Ion 16:211–22410.1016/0167-2738(85)90045-1 ↗
8. Subbarao EC, Maiti HS (1982) Solid electrolytes with oxygen ion conduction. Solid State Ion 11:317–33810.1016/0167-2738(84)90024-9 ↗
9. Shlyakhtina AV, Fedtke P, Busch A, Kolbanev IV, Barfels T, Wienecke M, Sokolov AE, Ulianov VA, Trounov VA, Shcherbakova LG (2008) Effect of the Ca-doping on the electrical conductivity of oxide ion conductor Yb2Ti2O7. Solid State Ion 179:1004–100810.1016/j.ssi.2007.12.098 ↗
10. Xia XL, Ouyang JH, Liu ZG (2010) Electrical properties of gadolinium-europium zirconate ceramics. J Am Ceram Soc 93:1074–108010.1111/j.1551-2916.2009.03505.x ↗
11. Porat O, Heremans C, Tuller HL (1997) Stability and mixed ionic electronic conduction in Gd2(Ti1-x Mo x )2O7 under anodic conditions. Solid State Ion 94:75–8310.1016/S0167-2738(96)00586-3 ↗
12. Díaz-Guillén MR, Moreno KJ, Díaz-Guillén JA, Fuentes AF, Ngai KL, García-Barriocanal J, Santamaría J, León C (2008) Cation size effects in oxygen ion dynamics of highly disordered pyrochlore-type ionic conductors. Phys Rev B 78:10430410.1103/PhysRevB.78.104304 ↗
13. Díaz-Guillén JA, Fuentes AF, Díaz-Guillén MR, Almanza JM, Santamaría J, León C (2009) The effect of homovalent A-site substitutions on the ionic conductivity of pyrochlore-type Gd2Zr2O7. J Power Sources 186:349–35210.1016/j.jpowsour.2008.09.106 ↗
14. Shlyaktina AV, Shcherbakova LG (2012) New solid electrolytes of the pyrochlore family. Russ J Electrochem 48:1–2510.1134/S1023193512010144 ↗
15. Kumar S, Gupta HC (2012) First principles study of dielectric and vibrational properties of pyrochlore hafnates. Solid State Sci 14:1405–141110.1016/j.solidstatesciences.2012.08.003 ↗
16. Kong L, Zhang Z, de los Reyes M, Karatchevtseva I, Lumpkin GR, Triani G, Aughterson RD (2015) Soft chemical synthesis and structural characterization of Y2Hf x Ti2−x O7. Ceram Inter 41:5309–531710.1016/j.ceramint.2014.12.074 ↗
17. Anand VK, Bera AK, Xu J, Herrmannsdörfer T, Ritter C, Lake B (2015) Observation of long-range magnetic ordering in pyrohafnate Nd2Hf2O7: a neutron diffraction study. Phys Rev B 92:18441810.1103/PhysRevB.92.184418 ↗
18. Blanchard PER, Liu S, Kennedy BJ, Ling CD (2013) Investigating the local structure of lanthanoid hafnates Ln2Hf2O7 via diffraction and spectroscopy. J Phys Chem C 117:2266–227310.1021/jp311329q ↗
19. Shlyakhtina AV, Shcherbakova LG (2011) Polymorphism and high-temperature conductivity of Ln2M2O7 (Ln = Sm–Lu; M = Ti, Zr, Hf) pyrochlores. Solid State Ion 192:200–20410.1016/j.ssi.2010.07.013 ↗
20. Brixner LH (1984) Structural and luminescent properties of the Ln2Hf2O7-type rare earth hafnates. Mat Res Bull 19:143–14910.1016/0025-5408(84)90084-9 ↗
21. Shlyakhtina AV, Knotko AV, Boguslavskii MV, Stefanovich SY, Kolbanev IV, Larina LL, Shcherbakova LG (2007) Effect of non-stoichiometry and synthesis temperature on the structure and conductivity of Ln(2+x)M(2−x)O(7-x/2) (Ln = Sm–Gd; M = Zr, Hf, x = 0-0.286). Solid State Ion 178:59–6610.1016/j.ssi.2006.11.001 ↗
22. Shannon R (1976) Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides. Acta Cryst A32:751–76710.1107/S0567739476001551 ↗
23. Zyryanov VV (2008) Mechanochemical synthesis of complex oxides. Russ Chem Rev 77:105–13510.1070/RC2008v077n02ABEH003709 ↗
24. Fuentes AF, Takacs L (2013) Preparation of multicomponent oxides by mechanochemical methods. J Mater Sci 48:598–611. doi: 10.1007/s10853-012-6909-x10.1007/s10853-012-6909-x ↗
25. Subramanian MA, Aravamudan G, Subba Rao GV (1985) Oxide pyrochlores—a review. Prog Solid State Chem 15:55–143.10.1016/0079-6786(83)90001-8 ↗
26. Van Dijk MP, Burggraaf AJ, Cormack AN, Catlow CRA (1985) Defect structures and migration mechanisms in oxide pyrochlores. Solid State Ion 17:159–16710.1016/0167-2738(85)90067-0 ↗
27. Wilde PJ, Catlow CRA (1998) Defects and diffusion in pyrochlore structured oxides. Solid State Ion 112:173–18310.1016/S0167-2738(98)00190-8 ↗
28. Rodríguez-Carvajal J (1993) Recent advances in magnetic structure determination by neutron powder diffraction, Phys B 19:55–69; See also a report in CPD of IUCr, Newsletter 2001, 26, 12; available at http://www.iucr.org/iucr-top/comm/cpd/Newsletters . The program and manual can be found at http://www-llb.cea.fr/fullweb/powder.htm10.1016/0921-4526(93)90108-I ↗
29. Langford JI (1992) The use of the Voigt function in determining microstructural properties from diffraction data by means of pattern decomposition. In: Prince E, Stalick JK (eds) Proceedings of the international conference “Accuracy in Powder Diffraction II”. NIST Special Publication 846 Gaithersburg, MD, USA, pp 110–126
30. Langford JI (1999) Use of pattern decomposition or simulation to study microstructure: theoretical considerations. In: Snyder RL, Fiala J, Bunge HJ (eds) Defect and microstructure analysis by diffraction, IUCr Monographs on Crystallography 10. Oxford University Press, Oxford, pp 59–81
31. Louër D (1999) Use of pattern decomposition to study microstructure: practical aspects and applications. In: Snyder RL, Fiala J, Bunge HJ (eds) Defect and microstructure analysis by diffraction, IUCr Monographs on Crystallography 10. Oxford University Press, Oxford, pp 671–697
32. Halder NC, Wagner CNJ (1966) Analysis of the broadening of powder pattern peaks using variance, integral breadth, and Fourier coefficients on the line profile. Adv X-Ray Anal 9:91–102
33. Heremans C, Wuensch BJ, Stalick JK, Prince E (1995) Fast-ion conducting Y2(ZryTi1-y)2O7 pyrochlores: neutron Rietveld analysis of disorder induced by Zr substitution. J Solid State Chem 117:108–12110.1006/jssc.1995.1253 ↗
34. Wuensch BJ, Eberman KW, Heremans C, Ku EM, Onnerud P, Yeo EME, Haile SM, Stalick JK, Jorgensen JD (2000) Connection between oxygen-ion conductivity of pyrochlore fuel-cell materials and structural change with composition and temperature. Solid State Ion 129:111–13310.1016/S0167-2738(99)00320-3 ↗
35. Fuentes AF, Boulahya K, Maczka M, Hanuza J, Amador U (2005) Synthesis of disordered pyrochlores, A2Ti2O7 (A = Y, Gd and Dy), by mechanical milling of constituent oxides. Solid State Sci 7:343–35310.1016/j.solidstatesciences.2005.01.002 ↗
36. Moreno KJ, Fuentes AF, Maczka M, Hanuza J, Amador U, Santamaria J, Leon C (2007) Influence of thermally induced oxygen order on mobile ion dynamics in Gd2(Ti0.65Zr0.35)2O7. Phys Rev B 75:18430310.1103/PhysRevB.75.184303 ↗
37. Maczka M, Hanuza J, Hermanowicz K, Fuentes AF, Matsuhira K, Hiroi ZJ (2008) Temperature-dependent Raman scattering studies of the geometrically frustrated Dy2Ti2O7, Gd2Ti2O7 and Er2Ti2O7. J Raman Spectrosc 39:537–54410.1002/jrs.1875 ↗
38. Garg N, Pandey KK, Murli C, Shanavas KV, Mandal BP, Tyagi AK, Sharma SM (2008) Decomposition of lanthanum hafnate at high pressures. Phys Rev B 77:21410510.1103/PhysRevB.77.214105 ↗
39. Mandal BP, Garg N, Sharma SM, Tyagi AK (2006) Preparation, XRD and Raman spectroscopic studies on new compounds RE2Hf2O7 (RE = Dy, Ho, Er, Tm, Lu, Y): pyrochlores or defect fluorite? J Solid State Chem 179:1990–199410.1016/j.jssc.2006.03.036 ↗
40. Glerup M, Nielsen OF, Poulsen FW (2001) The structural transformation from the pyrochlore structure, A2B2O7, to the fluorite structure, AO2, studied by Raman spectroscopy and defect chemistry modeling. J Solid State Chem 160:25–3210.1006/jssc.2000.9142 ↗
41. Sanjuán ML, Guglieri C, Diaz-Moreno S, Aquilanti G, Fuentes AF, Olivi L, Chaboy J (2011) Raman and x-ray absorption spectroscopy of the phase evolution induced by mechanical milling and thermal treatments in R2Ti2O7 pyrochlores. Phys Rev B 84:10420710.1103/PhysRevB.84.104207 ↗
42. Jonscher AK (1984) Dielectric relaxation in solids. Chelsea Dielectric Press, London
43. Moreno KJ, Fuentes AF, Amador U, Santamaría J, León C (2007) Influence of structural disorder on the dynamics of mobile oxygen ions in Dy2(Ti1-yZry)2O7. J Non-Cryst Solids 353:3947–395510.1016/j.jnoncrysol.2007.04.037 ↗
44. Aguadero A, Fawcett L, Taub S, Woolley R, Wu K-T, Xu N, Kilner JA, Skinner SJ (2012) Materials development for intermediate-temperature solid oxide electrochemical devices. J Mater Sci 47:3925–3938. doi: 10.1007/s10853-011-6213-110.1007/s10853-011-6213-1 ↗