A search for disorder in the spin glass double perovskites Sr2CaReO6 and Sr2MgReO6 using neutron diffraction and neutron pair distribution function analysis
暂无分享,去创建一个
[1] C. Bridges,et al. Structure and magnetic properties of the S = 1 geometrically frustrated double perovskites La 2 LiReO 6 and Ba 2 YReO 6 , 2010 .
[2] V. Michaelis,et al. Magnetic properties of the geometrically frustrated S=(1)/(2) antiferromagnets, La 2 LiMoO 6 and Ba 2 YMoO 6 , with the B-site ordered double perovskite structure: Evidence for a collective spin-singlet ground state , 2010, 1001.1665.
[3] M. Gingras,et al. Magnetic Pyrochlore Oxides , 2009, 0906.3661.
[4] V. Michaelis,et al. Magnetic properties of the S = 3 2 geometrically frustrated double perovskites La 2 LiRuO 6 and Ba 2 YRuO 6 , 2009 .
[5] A. D. Lozano-Gorrín,et al. Local and average structures of the spin-glass pyrochlore Y2Mo2O7 from neutron diffraction and neutron pair distribution function analysis , 2009 .
[6] W. Bisson,et al. Anisotropy-driven spin glass transition in the kagome antiferromagnet hydronium jarosite, (H3O)Fe3(SO4)2(OH)6 , 2008 .
[7] W. Kockelmann,et al. Magnetic ground state of an experimental S=1/2 kagome antiferromagnet. , 2007, Physical review letters.
[8] J. Trombe,et al. (17) O NMR study of the intrinsic magnetic susceptibility and spin dynamics of the quantum kagome antiferromagnet ZnCu3(OH)(6)Cl(2). , 2007, Physical review letters.
[9] S J L Billinge,et al. PDFfit2 and PDFgui: computer programs for studying nanostructure in crystals , 2007, Journal of physics. Condensed matter : an Institute of Physics journal.
[10] Q. Huang,et al. Quantum-spin-liquid states in the two-dimensional kagome antiferromagnets ZnxCu4-x(OD)6Cl2. , 2007, Nature materials.
[11] D. Nocera,et al. A structurally perfect S = (1/2) kagomé antiferromagnet. , 2005, Journal of the American Chemical Society.
[12] J. Bouchaud,et al. Transitions and Spin Dynamics at Very Low Temperature in the Pyrochlores Yb2Ti2O7 and Gd2Sn2O7 , 2003, cond-mat/0306470.
[13] S. Billinge. The atomic pair distribution function: past and present , 2004 .
[14] A. Savici,et al. Frustration-driven spin freezing in the S=1/2 fcc perovskite Sr 2 MgReO 6 , 2003 .
[15] C. Grey,et al. Structural chemistry and magnetic properties of La2LiRuO6 , 2003 .
[16] P. Woodward,et al. Ordered double perovskites -- a group-theoretical analysis. , 2003, Acta crystallographica. Section B, Structural science.
[17] D. Nocera,et al. Magnetism of pure iron jarosites , 2003 .
[18] A. Cheetham,et al. Building a high resolution total scattering powder diffractometer – upgrade of NPD at MLNSC , 2002 .
[19] J. Gardner,et al. Spin-glass behavior in the S = 1 / 2 fcc ordered perovskite Sr 2 CaReO 6 , 2002 .
[20] Mark D. Smith,et al. Crystal growth of Ba2MOsO6 (M=Li, Na) from reactive hydroxide fluxes , 2002 .
[21] M. Gingras,et al. Spin Ice State in Frustrated Magnetic Pyrochlore Materials , 2001, Science.
[22] H. Okumura,et al. Nature of spin freezing transition of geometrically frustrated pyrochlore system R2Ru2O7 (R=rare earth elements and Y) , 2001 .
[23] M. Gingras,et al. Thermodynamic and single-ion properties of Tb3+ within the collective paramagnetic-spin liquid state of the frustrated pyrochlore antiferromagnet Tb2Ti2O7 , 2000 .
[24] A. Harrison,et al. μSR studies of the kagomé antiferromagnet (H3O)Fe3(OH)6(SO4)2 , 2000 .
[25] Ronald I. Smith,et al. Magnetic properties of pure and diamagnetically doped jarosites: Model kagome antiferromagnets with variable coverage of the magnetic lattice , 2000 .
[26] M. Itoh,et al. Structure and magnetic properties of Sr2NiAO6 (A = W, Te) , 2000 .
[27] K. H. Andersen,et al. A polarised neutron scattering study of the magnetic correlations in the kagome antiferromagnet , 1999 .
[28] R. Siddharthan,et al. Zero-point entropy in ‘spin ice’ , 1999, Nature.
[29] Y. Hinatsu,et al. Magnetic Properties of Ruthenium Pyrochlores Y2Ru2O7and Lu2Ru2O7 , 1999 .
[30] A. Harrison,et al. Long-range order induced by diamagnetic dilution of jarosites, model Kagomé antiferromagnets , 1997 .
[31] S. Bramwell,et al. GEOMETRICAL FRUSTRATION IN THE FERROMAGNETIC PYROCHLORE HO2TI2O7 , 1997 .
[32] M. Gingras,et al. Static Critical Behavior of the Spin-Freezing Transition in the Geometrically Frustrated Pyrochlore Antiferromagnet Y 2 Mo 2 O 7 , 1996, cond-mat/9611121.
[33] T. Mason,et al. Magnetic correlations in deuteronium jarosite, a model S = 5/2 Kagomé antiferromagnet , 1996, cond-mat/9607106.
[34] A. Harrison,et al. Structure and magnetism of hydronium jarosite, a model Kagomé antiferromagnet , 1996 .
[35] I. Brown,et al. The chemical bond and atomic displacements in SrTiO3 from X‐ray diffraction analysis , 1995 .
[36] Mark T. Anderson,et al. B-cation arrangements in double perovskites , 1993 .
[37] Mason,et al. Spin freezing in the geometrically frustrated pyrochlore antiferromagnet Tb2Mo2O7. , 1992, Physical review letters.
[38] A. S. Cooper,et al. Broken spin rotation symmetry without magnetic Bragg peaks in Kagomé antiferromagnets , 1990 .
[39] J. N. Reimers,et al. Short‐range ordering in a three‐dimensionally frustrated magnet, Tb2Mo2O7, by wide‐ and small‐angle neutron diffraction , 1990 .
[40] N. Ali,et al. Magnetic and electrical properties of R2Mo2O7 pyrochlore compounds , 1989 .
[41] Mineo Sato,et al. Magnetic properties and magnetic ordering in the rare earth molybdenum(IV) pyrochlores: R2Mo2O7 , 1986 .
[42] J. Greedan,et al. Spin-glass-like behavior in Y2Mo2O7, a concentrated, crystalline system with negligible apparent disorder , 1986 .
[43] L. Soderholm,et al. Ferromagnetic semiconductors: Magnetic properties of the pyrochlores, (YxLu1−x)2V2O7 and (ScxLu1−x)2V2O7 , 1979 .
[44] G. Adachi,et al. On the pyrochlore type Ln2V2O7 (Ln: Rare-earth elements) , 1977 .