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High-resolution synchrotron radiation powder diffraction patterns of α-Fe2O3 measured between room temperature and 1100 K, i.e. above the Néel temperature TN = 950 K, have been analyzed. The integral breadths of the Bragg peaks show a hkl-dependent anisotropy, both below and above TN. This anisotropy can be quantitatively described by using a statistical peak-broadening model [Stephens (1999). J. Appl. Cryst. 32, 281]. Model calculations show that the rhombohedral α-Fe2O3 lattice is deformed and the deformation leads to a monoclinic lattice with the unique monoclinic axis along the hexagonal [110] direction both below and above TN. The monoclinic symmetry of bulk α-Fe2O3 is compatible with α-Fe2O3 nanowire growth along the [110] direction reported in Fu et al. [Chem. Phys. Lett. (2001), 350, 491].
Supporting information
CCDC references: 1515808; 1515809
Crystal data top
Fe2O3 | β = 162.4043 (3)° |
Mr = 159.7 | V = 201.35 (1) Å3 |
Monoclinic, C2/c | Z = 4 |
Hall symbol: -C 2yc | F(000) = 304 |
a = 9.61865 (9) Å | Dx = 5.268 Mg m−3 |
b = 5.03554 (3) Å | Synchrotron radiation |
c = 13.75158 (13) Å | T = 293 K |
Data collection top
2θmin = 5°, 2θmax = 29.999°, 2θstep = 0.001° | |
Refinement top
Rp = 0.097 | 21 parameters |
Rwp = 0.129 | 0 restraints |
Rexp = 0.094 | 0 constraints |
R(F) = 0.032 | Weighting scheme based on measured s.u.'s |
43005 data points | (Δ/σ)max = 0.025 |
Excluded region(s): from 30 to 100.000 | Background function: 5 Legendre polynoms |
Profile function: Pseudo-Voigt | Preferred orientation correction: none |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Fe1 | 0 | 0 | 0.14473 (3) | 0.0033* | |
O1 | 0 | 0.309 (3) | 0.25 | 0.0005* | |
O2 | −0.449 (2) | −0.156 (2) | −0.050 (2) | 0.0005* | |
Crystal data top
Fe2O3 | β = 162.3508 (2)° |
Mr = 159.7 | V = 206.97 (1) Å3 |
Monoclinic, C2/c | Z = 4 |
Hall symbol: -C 2yc | F(000) = 304 |
a = 9.68920 (8) Å | Dx = 5.125 Mg m−3 |
b = 5.08737 (2) Å | Synchrotron radiation |
c = 13.84868 (11) Å | T = 1053 K |
Data collection top
2θmin = 5°, 2θmax = 29.999°, 2θstep = 0.001° | |
Refinement top
Rp = 0.099 | 21 parameters |
Rwp = 0.128 | 0 restraints |
Rexp = 0.086 | 0 constraints |
R(F) = 0.044 | Weighting scheme based on measured s.u.'s |
43003 data points | (Δ/σ)max = 0.036 |
Excluded region(s): from 30 to 100.000 | Background function: 5 Legendre polynoms |
Profile function: Pseudo-Voigt | Preferred orientation correction: none |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Fe1 | 0 | 0 | 0.14425 (3) | 0.0131* | |
O1 | 0 | 0.313 (3) | 0.25 | 0.0102* | |
O2 | −0.449 (3) | −0.155 (3) | −0.049 (2) | 0.0102* | |
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