Names | |
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IUPAC name
Dysprosium titanate | |
Identifiers | |
3D model (JSmol) |
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Properties | |
Dy2O7Ti2 | |
Molar mass | 532.727 g·mol−1 |
Density | 6.8 g/cm3[1] |
Structure[1] | |
Pyrochlore | |
Fd3m, cF88, No. 227 | |
a = 1.0136 nm | |
Formula units (Z) |
8 |
Related compounds | |
Other cations |
Holmium titanate |
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).
Infobox references |
Dysprosium titanate (Dy2Ti2O7) is an inorganic compound, a ceramic of the titanate family, with pyrochlore structure.
Dysprosium titanate, like holmium titanate and holmium stannate, is a spin ice material. In 2009, quasiparticles resembling magnetic monopoles were observed at low temperature and high magnetic field.[2][3]
Dysprosium titanate (Dy2TiO5) is used since 1995 as material for control rods of commercial nuclear reactor.[4]
References
- 1 2 Dolgikh V.A., Lavat E.A. (1991). "Preparation of new oxide nitrides with the pyrochlore structure". Russ. J. Inorg. Chem. 36: 1389–1392.
- ↑ "Magnetic Monopoles Detected In A Real Magnet For The First Time". Science Daily. 2009-09-04. Retrieved 2009-09-04.
- ↑ Morris, D. J. P.; Tennant, D. A.; Grigera, S. A.; Klemke, B.; Castelnovo, C.; Moessner, R.; Czternasty, C.; Meissner, M.; Rule, K. C.; Hoffmann, J.-U.; Kiefer, K.; Gerischer, S.; Slobinsky, D.; Perry, R. S. (2009-09-03). "Dirac Strings and Magnetic Monopoles in Spin Ice Dy2Ti2O7". Science. 326 (5951): 411–4. arXiv:1011.1174. Bibcode:2009Sci...326..411M. doi:10.1126/science.1178868. PMID 19729617. S2CID 206522398.
- ↑ Risovany, V.D.; Varlashova, E.E.; Suslov, D.N. (2000). "Dysprosium titanate as an absorber material for control rods". Journal of Nuclear Materials. 281 (1): 84–89. Bibcode:2000JNuM..281...84R. doi:10.1016/S0022-3115(00)00129-X.
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