Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600576714004907/rw5065sup1.cif | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LCTO_NPDsup2.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LCTO_SXRDsup3.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT10_NPDsup4.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT10_XRDsup5.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT20_NPDsup6.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT20_SXRDsup7.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT30_NPDsup8.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT30_SXRDsup9.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT50_NPDsup10.rtv | |
Rietveld powder data file (CIF format) https://doi.org/10.1107/S1600576714004907/rw5065LSCT50_SXRDsup11.rtv | |
Portable Document Format (PDF) file https://doi.org/10.1107/S1600576714004907/rw5065sup12.pdf |
CCDC references: 989515; 989516; 989517; 989518; 989519; 989520; 989521; 989522; 989523; 989524
Samples of compositions La2-xSrxCoTiO6 (0=x=0.5) were prepared by a modified Peccini method. About 10 grams of each sample was prepared solving stoichiometric amounts of high purity Co(CH3COO)2·4H2O (Aldrich, 99.99%), La2O3 (Aldrich, 99.9%)and SrCO3 (Aldrich 99.9%) in ca 20 ml of concentrated hot nitric acid (Panreac 66%)and ca 50 ml of distillate water was added. Under heating and vigorous stirring, citric acid was added in a molar ratio citric acid to metal ions of 3:1. Then, titanium was added as anatase (Aldrich, purity 99.9%) to obtain a homogeneous suspension, since TiO2 is not soluble. When the solution was concentrated to half of its initial volume, 3 ml of diethyleneglycol was added to promote polymerization. When a solid resin is formed it is allowed to cool down to room temperature and then milled in an agate mortar; the obtained powder was burn at 1073 K to remove organic matter. After milling and homogenization the resulted powder was heated at 1773 K for 24 h and cooled down (at a rate of 2 K/min) to room temperature to obtain well crystallized materials.
Co2La4O12Ti2 | Z = 2 |
Mr = 480.62 | ? _exptl_crystal_density_diffrn 6.556(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 422.0 |
Monoclinic, P21/n | Synchrotron radiation, λ = 0.621000 Å |
Hall symbol: -P 2yn | µ = 7.37 mm−1 |
a = 5.55510 (9) Å | T = 295 K |
b = 5.57813 (8) Å | Particle morphology: plate-like SEM |
c = 7.85718 (12) Å | black |
β = 90.005 (5)° | cylinder, 15 × 20 mm |
V = 243.47 (1) Å3 |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Scan method: step |
Radiation source: Synchrotron | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Si 111 monochromator | Tmin = ?, Tmax = ? |
Specimen mounting: Borosilicate 0.3 mm capillary | 2θmin = 7.989°, 2θmax = 46.991°, 2θstep = 0.010° |
Data collection mode: transmission |
Refinement on Inet | 3901 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.073 | 40 parameters |
Rwp = 0.100 | 0 restraints |
Rexp = 0.058 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.036 | (Δ/σ)max = 0.01 |
χ2 = 8.418 | Background function: Set of experimental background points |
Co2La4O12Ti2 | V = 243.47 (1) Å3 |
Mr = 480.62 | Z = 2 |
Monoclinic, P21/n | Synchrotron radiation, λ = 0.621000 Å |
a = 5.55510 (9) Å | µ = 7.37 mm−1 |
b = 5.57813 (8) Å | T = 295 K |
c = 7.85718 (12) Å | cylinder, 15 × 20 mm |
β = 90.005 (5)° |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Specimen mounting: Borosilicate 0.3 mm capillary | Tmin = ?, Tmax = ? |
Data collection mode: transmission | 2θmin = 7.989°, 2θmax = 46.991°, 2θstep = 0.010° |
Scan method: step |
Rp = 0.073 | χ2 = 8.418 |
Rwp = 0.100 | 3901 data points |
Rexp = 0.058 | 40 parameters |
RBragg = 0.036 | 0 restraints |
Experimental. Synchrotron source |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
La1 | 0.0059 (3) | −0.03335 (16) | 0.2494 (7) | 0.0055 (2)* | |
Ti1 | 0.00000 | 0.50000 | 0.00000 | 0.0038 (8)* | 0.90600 |
Co2 | 0.00000 | 0.50000 | 0.00000 | 0.0038 (8)* | 0.09400 |
Co1 | 0.00000 | 0.50000 | 0.50000 | 0.0005 (8)* | 0.90600 |
Ti2 | 0.00000 | 0.50000 | 0.50000 | 0.0005 (8)* | 0.09400 |
O1 | −0.7229 (9) | 0.7041 (9) | 0.0381 (9) | 0.0058 (11)* | |
O1_2 | −0.2058 (9) | 0.7759 (9) | −0.0404 (9) | 0.0051 (11)* | |
O1_3 | −0.0740 (5) | 0.5143 (4) | 0.2473 (8) | 0.0083 (5)* |
La1—O1i | 2.678 (7) | Ti1—O1viii | 1.938 (5) |
La1—O1ii | 2.448 (7) | Ti1—O1iii | 1.938 (5) |
La1—O1iii | 3.309 (7) | Ti1—O1_2 | 1.943 (5) |
La1—O1iv | 2.769 (8) | Ti1—O1_2vi | 1.943 (5) |
La1—O1_2v | 2.775 (8) | Ti1—O1_3 | 1.988 (6) |
La1—O1_2ii | 3.314 (7) | Ti1—O1_3vi | 1.988 (6) |
La1—O1_2vi | 2.448 (7) | Co1—O1ii | 2.085 (5) |
La1—O1_2iv | 2.669 (7) | Co1—O1ix | 2.085 (5) |
La1—O1_3v | 2.562 (2) | Co1—O1_2ii | 2.082 (5) |
La1—O1_3 | 3.087 (2) | Co1—O1_2ix | 2.082 (5) |
La1—O1_3ii | 2.414 (3) | Co1—O1_3 | 2.029 (6) |
La1—O1_3vii | 3.167 (3) | Co1—O1_3x | 2.029 (6) |
O1—Co1—O1 | 180.0 (4) | O1—Ti1—O1 | 180.0 (5) |
O1—Co1—O1_2 | 90.7 (3) | O1—Ti1—O1_2 | 91.6 (4) |
O1—Co1—O1_2 | 89.3 (3) | O1—Ti1—O1_2 | 88.4 (4) |
O1—Co1—O1_3 | 90.6 (4) | O1—Ti1—O1_3 | 89.4 (4) |
O1—Co1—O1_3 | 89.4 (4) | O1—Ti1—O1_3 | 90.6 (4) |
O1—Co1—O1_2 | 89.3 (3) | O1—Ti1—O1_2 | 88.4 (4) |
O1—Co1—O1_2 | 90.7 (3) | O1—Ti1—O1_2 | 91.6 (4) |
O1—Co1—O1_3 | 89.4 (4) | O1—Ti1—O1_3 | 90.6 (4) |
O1—Co1—O1_3 | 90.6 (4) | O1—Ti1—O1_3 | 89.4 (4) |
O1_2—Co1—O1_2 | 180.0 (4) | O1_2—Ti1—O1_2 | 180.0 (5) |
O1_2—Co1—O1_3 | 90.8 (4) | O1_2—Ti1—O1_3 | 90.4 (4) |
O1_2—Co1—O1_3 | 89.2 (4) | O1_2—Ti1—O1_3 | 89.6 (4) |
O1_2—Co1—O1_3 | 89.2 (4) | O1_2—Ti1—O1_3 | 89.6 (4) |
O1_2—Co1—O1_3 | 90.8 (4) | O1_2—Ti1—O1_3 | 90.4 (4) |
O1_3—Co1—O1_3 | 180.0 (6) | O1_3—Ti1—O1_3 | 180.0 (6) |
Symmetry codes: (i) x+1, y−1, z; (ii) −x−1/2, y−1/2, −z+1/2; (iii) −x−1, −y+1, −z; (iv) x+1/2, −y+1/2, z+1/2; (v) x, y−1, z; (vi) −x, −y+1, −z; (vii) −x+1/2, y−1/2, −z+1/2; (viii) x+1, y, z; (ix) x+1/2, −y+3/2, z+1/2; (x) −x, −y+1, −z+1. |
Co2La4O12Ti2 | Z = 2 |
Mr = 480.62 | ? _exptl_crystal_density_diffrn 6.556(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 100.9 |
Monoclinic, P21/n | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
Hall symbol: -P 2yn | µ = 0.00 mm−1 |
a = 5.55510 (9) Å | T = 295 K |
b = 5.57813 (8) Å | Particle morphology: plate-like SEM |
c = 7.85718 (12) Å | black |
β = 90.005 (5)° | cylinder, 15 × 20 mm |
V = 243.47 (1) Å3 |
High-resolution two-axis diffractometer | Data collection mode: transmission |
Radiation source: nuclear reactor, D2B beamline ILL | Scan method: step |
Ge monochromator | 2θmin = 0.239°, 2θmax = 160.189°, 2θstep = 0.050° |
Specimen mounting: 'vanadium can' |
Refinement on Inet | 3901 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.046 | 40 parameters |
Rwp = 0.059 | 0 restraints |
Rexp = 0.039 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.032 | (Δ/σ)max = 0.01 |
χ2 = 5.505 | Background function: Set of experimental background points |
Co2La4O12Ti2 | V = 243.47 (1) Å3 |
Mr = 480.62 | Z = 2 |
Monoclinic, P21/n | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
a = 5.55510 (9) Å | µ = 0.00 mm−1 |
b = 5.57813 (8) Å | T = 295 K |
c = 7.85718 (12) Å | cylinder, 15 × 20 mm |
β = 90.005 (5)° |
High-resolution two-axis diffractometer | Scan method: step |
Specimen mounting: 'vanadium can' | 2θmin = 0.239°, 2θmax = 160.189°, 2θstep = 0.050° |
Data collection mode: transmission |
Rp = 0.046 | χ2 = 5.505 |
Rwp = 0.059 | 3901 data points |
Rexp = 0.039 | 40 parameters |
RBragg = 0.032 | 0 restraints |
Experimental. Neutron reactor |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
La1 | 0.0059 (3) | −0.03335 (16) | 0.2494 (7) | 0.0055 (2)* | |
Ti1 | 0.00000 | 0.50000 | 0.00000 | 0.0038 (8)* | 0.90600 |
Co2 | 0.00000 | 0.50000 | 0.00000 | 0.0038 (8)* | 0.09400 |
Co1 | 0.00000 | 0.50000 | 0.50000 | 0.0005 (8)* | 0.90600 |
Ti2 | 0.00000 | 0.50000 | 0.50000 | 0.0005 (8)* | 0.09400 |
O1 | −0.7229 (9) | 0.7041 (9) | 0.0381 (9) | 0.0058 (11)* | |
O1_2 | −0.2058 (9) | 0.7759 (9) | −0.0404 (9) | 0.0051 (11)* | |
O1_3 | −0.0740 (5) | 0.5143 (4) | 0.2473 (8) | 0.0083 (5)* |
La1—O1i | 2.678 (7) | Ti1—O1viii | 1.938 (5) |
La1—O1ii | 2.448 (7) | Ti1—O1iii | 1.938 (5) |
La1—O1iii | 3.309 (7) | Ti1—O1_2 | 1.943 (5) |
La1—O1iv | 2.769 (8) | Ti1—O1_2vi | 1.943 (5) |
La1—O1_2v | 2.775 (8) | Ti1—O1_3 | 1.988 (6) |
La1—O1_2ii | 3.314 (7) | Ti1—O1_3vi | 1.988 (6) |
La1—O1_2vi | 2.448 (7) | Co1—O1ii | 2.085 (5) |
La1—O1_2iv | 2.669 (7) | Co1—O1ix | 2.085 (5) |
La1—O1_3v | 2.562 (2) | Co1—O1_2ii | 2.082 (5) |
La1—O1_3 | 3.087 (2) | Co1—O1_2ix | 2.082 (5) |
La1—O1_3ii | 2.414 (3) | Co1—O1_3 | 2.029 (6) |
La1—O1_3vii | 3.167 (3) | Co1—O1_3x | 2.029 (6) |
O1—Co1—O1 | 180.0 (4) | O1—Ti1—O1 | 180.0 (5) |
O1—Co1—O1_2 | 90.7 (3) | O1—Ti1—O1_2 | 91.6 (4) |
O1—Co1—O1_2 | 89.3 (3) | O1—Ti1—O1_2 | 88.4 (4) |
O1—Co1—O1_3 | 90.6 (4) | O1—Ti1—O1_3 | 89.4 (4) |
O1—Co1—O1_3 | 89.4 (4) | O1—Ti1—O1_3 | 90.6 (4) |
O1—Co1—O1_2 | 89.3 (3) | O1—Ti1—O1_2 | 88.4 (4) |
O1—Co1—O1_2 | 90.7 (3) | O1—Ti1—O1_2 | 91.6 (4) |
O1—Co1—O1_3 | 89.4 (4) | O1—Ti1—O1_3 | 90.6 (4) |
O1—Co1—O1_3 | 90.6 (4) | O1—Ti1—O1_3 | 89.4 (4) |
O1_2—Co1—O1_2 | 180.0 (4) | O1_2—Ti1—O1_2 | 180.0 (5) |
O1_2—Co1—O1_3 | 90.8 (4) | O1_2—Ti1—O1_3 | 90.4 (4) |
O1_2—Co1—O1_3 | 89.2 (4) | O1_2—Ti1—O1_3 | 89.6 (4) |
O1_2—Co1—O1_3 | 89.2 (4) | O1_2—Ti1—O1_3 | 89.6 (4) |
O1_2—Co1—O1_3 | 90.8 (4) | O1_2—Ti1—O1_3 | 90.4 (4) |
O1_3—Co1—O1_3 | 180.0 (6) | O1_3—Ti1—O1_3 | 180.0 (6) |
Symmetry codes: (i) x+1, y−1, z; (ii) −x−1/2, y−1/2, −z+1/2; (iii) −x−1, −y+1, −z; (iv) x+1/2, −y+1/2, z+1/2; (v) x, y−1, z; (vi) −x, −y+1, −z; (vii) −x+1/2, y−1/2, −z+1/2; (viii) x+1, y, z; (ix) x+1/2, −y+3/2, z+1/2; (x) −x, −y+1, −z+1. |
CoLa1.9O6Sr0.1Ti | Z = 2 |
Mr = 475.52 | ? _exptl_crystal_density_diffrn 6.483(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 418.2 |
Monoclinic, P21/n | Cu Kα1 radiation, λ = 1.540560 Å |
Hall symbol: -P 2yn | T = 295 K |
a = 5.55318 (8) Å | Particle morphology: plate-like SEM |
b = 5.56557 (7) Å | black |
c = 7.84995 (10) Å | flat sheet, 20 × 20 mm |
β = 90.007 (5)° | Specimen preparation: Cooled at 2 K min−1 |
V = 242.62 (1) Å3 |
Bruker D8 Advance diffractometer | Data collection mode: reflexion |
Radiation source: sealed X-ray tube | Scan method: step |
Ge (111) monochromator | 2θmin = 19.880°, 2θmax = 99.882°, 2θstep = 0.020° |
Specimen mounting: Aluminium Sample holder |
Refinement on Inet | 4061 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.036 | 34 parameters |
Rwp = 0.047 | 0 restraints |
Rexp = 0.035 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.083 | (Δ/σ)max = 0.01 |
χ2 = 3.147 | Background function: Set of experimental background points |
CoLa1.9O6Sr0.1Ti | β = 90.007 (5)° |
Mr = 475.52 | V = 242.62 (1) Å3 |
Monoclinic, P21/n | Z = 2 |
a = 5.55318 (8) Å | Cu Kα1 radiation, λ = 1.540560 Å |
b = 5.56557 (7) Å | T = 295 K |
c = 7.84995 (10) Å | flat sheet, 20 × 20 mm |
Bruker D8 Advance diffractometer | Scan method: step |
Specimen mounting: Aluminium Sample holder | 2θmin = 19.880°, 2θmax = 99.882°, 2θstep = 0.020° |
Data collection mode: reflexion |
Rp = 0.036 | χ2 = 3.147 |
Rwp = 0.047 | 4061 data points |
Rexp = 0.035 | 34 parameters |
RBragg = 0.083 | 0 restraints |
Experimental. Conventional X-Ray source |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
La1 | 0.0056 (4) | −0.03105 (18) | 0.2494 (10) | 0.0066 (2)* | 0.95000 |
Sr1 | 0.0056 (4) | −0.03105 (18) | 0.2494 (10) | 0.0066 (2)* | 0.05000 |
Ti1 | 0.00000 | 0.50000 | 0.00000 | 0.0069 (12)* | 0.82690 |
Co2 | 0.00000 | 0.50000 | 0.00000 | 0.0069 (12)* | 0.17312 |
O1 | −0.7234 (8) | 0.7081 (8) | 0.0375 (10) | 0.0062 (11)* | |
O1_2 | −0.2102 (8) | 0.7757 (8) | −0.0390 (10) | 0.0082 (12)* | |
O1_3 | −0.0725 (4) | 0.5128 (3) | 0.2475 (3) | 0.0076 (4)* | |
Co1 | 0.00000 | 0.50000 | 0.50000 | 0.0036 (18)* | 0.82690 |
Ti2 | 0.00000 | 0.50000 | 0.50000 | 0.0036 (18)* | 0.17312 |
La1—O1i | 2.676 (8) | Ti1—O1viii | 1.949 (5) |
La1—O1ii | 2.459 (8) | Ti1—O1iii | 1.949 (5) |
La1—O1iii | 3.284 (8) | Ti1—O1_2 | 1.955 (5) |
La1—O1iv | 2.779 (9) | Ti1—O1_2vi | 1.955 (5) |
La1—O1_2v | 2.782 (9) | Ti1—O1_3 | 1.988 (2) |
La1—O1_2ii | 3.287 (8) | Ti1—O1_3vi | 1.988 (2) |
La1—O1_2vi | 2.461 (8) | Co1—O1ii | 2.068 (5) |
La1—O1_2iv | 2.669 (8) | Co1—O1ix | 2.068 (5) |
La1—O1_3v | 2.577 (2) | Co1—O1_2ii | 2.062 (5) |
La1—O1_3 | 3.060 (2) | Co1—O1_2ix | 2.062 (5) |
La1—O1_3ii | 2.421 (3) | Co1—O1_3 | 2.026 (2) |
La1—O1_3vii | 3.160 (3) | Co1—O1_3x | 2.026 (2) |
O1—Ti1—O1 | 180.0 (4) | O1—Co1—O1 | 180.0 (4) |
O1—Ti1—O1_2 | 91.6 (3) | O1—Co1—O1_2 | 90.8 (3) |
O1—Ti1—O1_2 | 88.4 (3) | O1—Co1—O1_2 | 89.2 (3) |
O1—Ti1—O1_3 | 89.5 (3) | O1—Co1—O1_3 | 90.4 (3) |
O1—Ti1—O1_3 | 90.5 (3) | O1—Co1—O1_3 | 89.6 (3) |
O1—Ti1—O1_2 | 88.4 (3) | O1—Co1—O1_2 | 89.2 (3) |
O1—Ti1—O1_2 | 91.6 (3) | O1—Co1—O1_2 | 90.8 (3) |
O1—Ti1—O1_3 | 90.5 (3) | O1—Co1—O1_3 | 89.6 (3) |
O1—Ti1—O1_3 | 89.5 (3) | O1—Co1—O1_3 | 90.4 (3) |
O1_2—Ti1—O1_2 | 180.0 (4) | O1_2—Co1—O1_2 | 180.0 (4) |
O1_2—Ti1—O1_3 | 90.2 (3) | O1_2—Co1—O1_3 | 90.7 (3) |
O1_2—Ti1—O1_3 | 89.8 (3) | O1_2—Co1—O1_3 | 89.3 (3) |
O1_2—Ti1—O1_3 | 89.8 (3) | O1_2—Co1—O1_3 | 89.3 (3) |
O1_2—Ti1—O1_3 | 90.2 (3) | O1_2—Co1—O1_3 | 90.7 (3) |
O1_3—Ti1—O1_3 | 180.0 (2) | O1_3—Co1—O1_3 | 180.0 (2) |
Symmetry codes: (i) x+1, y−1, z; (ii) −x−1/2, y−1/2, −z+1/2; (iii) −x−1, −y+1, −z; (iv) x+1/2, −y+1/2, z+1/2; (v) x, y−1, z; (vi) −x, −y+1, −z; (vii) −x+1/2, y−1/2, −z+1/2; (viii) x+1, y, z; (ix) x+1/2, −y+3/2, z+1/2; (x) −x, −y+1, −z+1. |
CoLa1.9O6Sr0.1Ti | Z = 2 |
Mr = 475.52 | ? _exptl_crystal_density_diffrn 6.483(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 100.6 |
Monoclinic, P21/n | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
Hall symbol: -P 2yn | µ = 0.00 mm−1 |
a = 5.55318 (8) Å | T = 295 K |
b = 5.56557 (7) Å | Particle morphology: plate-like SEM |
c = 7.84995 (10) Å | black |
β = 90.007 (5)° | cylinder, 15 × 20 mm |
V = 242.62 (1) Å3 |
High-resolution two-axis diffractometer | Data collection mode: transmission |
Radiation source: nuclear reactor, D2B beamline ILL | Scan method: step |
Ge monochromator | 2θmin = 0.245°, 2θmax = 160.195°, 2θstep = 0.050° |
Specimen mounting: 'vanadium can' |
Refinement on Inet | 4061 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.364 | 34 parameters |
Rwp = 0.047 | 0 restraints |
Rexp = 0.027 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.023 | (Δ/σ)max = 0.01 |
χ2 = 9.624 | Background function: Set of experimental background points |
CoLa1.9O6Sr0.1Ti | V = 242.62 (1) Å3 |
Mr = 475.52 | Z = 2 |
Monoclinic, P21/n | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
a = 5.55318 (8) Å | µ = 0.00 mm−1 |
b = 5.56557 (7) Å | T = 295 K |
c = 7.84995 (10) Å | cylinder, 15 × 20 mm |
β = 90.007 (5)° |
High-resolution two-axis diffractometer | Scan method: step |
Specimen mounting: 'vanadium can' | 2θmin = 0.245°, 2θmax = 160.195°, 2θstep = 0.050° |
Data collection mode: transmission |
Rp = 0.364 | χ2 = 9.624 |
Rwp = 0.047 | 4061 data points |
Rexp = 0.027 | 34 parameters |
RBragg = 0.023 | 0 restraints |
Experimental. Neutron reactor |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
La1 | 0.0056 (4) | −0.03105 (18) | 0.2494 (10) | 0.0066 (2)* | 0.95000 |
Sr1 | 0.0056 (4) | −0.03105 (18) | 0.2494 (10) | 0.0066 (2)* | 0.05000 |
Ti1 | 0.00000 | 0.50000 | 0.00000 | 0.0069 (12)* | 0.82690 |
Co2 | 0.00000 | 0.50000 | 0.00000 | 0.0069 (12)* | 0.17312 |
O1 | −0.7234 (8) | 0.7081 (8) | 0.0375 (10) | 0.0062 (11)* | |
O1_2 | −0.2102 (8) | 0.7757 (8) | −0.0390 (10) | 0.0082 (12)* | |
O1_3 | −0.0725 (4) | 0.5128 (3) | 0.2475 (3) | 0.0076 (4)* | |
Co1 | 0.00000 | 0.50000 | 0.50000 | 0.0036 (18)* | 0.82690 |
Ti2 | 0.00000 | 0.50000 | 0.50000 | 0.0036 (18)* | 0.17312 |
La1—O1i | 2.676 (8) | Ti1—O1viii | 1.949 (5) |
La1—O1ii | 2.459 (8) | Ti1—O1iii | 1.949 (5) |
La1—O1iii | 3.284 (8) | Ti1—O1_2 | 1.955 (5) |
La1—O1iv | 2.779 (9) | Ti1—O1_2vi | 1.955 (5) |
La1—O1_2v | 2.782 (9) | Ti1—O1_3 | 1.988 (2) |
La1—O1_2ii | 3.287 (8) | Ti1—O1_3vi | 1.988 (2) |
La1—O1_2vi | 2.461 (8) | Co1—O1ii | 2.068 (5) |
La1—O1_2iv | 2.669 (8) | Co1—O1ix | 2.068 (5) |
La1—O1_3v | 2.577 (2) | Co1—O1_2ii | 2.062 (5) |
La1—O1_3 | 3.060 (2) | Co1—O1_2ix | 2.062 (5) |
La1—O1_3ii | 2.421 (3) | Co1—O1_3 | 2.026 (2) |
La1—O1_3vii | 3.160 (3) | Co1—O1_3x | 2.026 (2) |
O1—Ti1—O1 | 180.0 (4) | O1—Co1—O1 | 180.0 (4) |
O1—Ti1—O1_2 | 91.6 (3) | O1—Co1—O1_2 | 90.8 (3) |
O1—Ti1—O1_2 | 88.4 (3) | O1—Co1—O1_2 | 89.2 (3) |
O1—Ti1—O1_3 | 89.5 (3) | O1—Co1—O1_3 | 90.4 (3) |
O1—Ti1—O1_3 | 90.5 (3) | O1—Co1—O1_3 | 89.6 (3) |
O1—Ti1—O1_2 | 88.4 (3) | O1—Co1—O1_2 | 89.2 (3) |
O1—Ti1—O1_2 | 91.6 (3) | O1—Co1—O1_2 | 90.8 (3) |
O1—Ti1—O1_3 | 90.5 (3) | O1—Co1—O1_3 | 89.6 (3) |
O1—Ti1—O1_3 | 89.5 (3) | O1—Co1—O1_3 | 90.4 (3) |
O1_2—Ti1—O1_2 | 180.0 (4) | O1_2—Co1—O1_2 | 180.0 (4) |
O1_2—Ti1—O1_3 | 90.2 (3) | O1_2—Co1—O1_3 | 90.7 (3) |
O1_2—Ti1—O1_3 | 89.8 (3) | O1_2—Co1—O1_3 | 89.3 (3) |
O1_2—Ti1—O1_3 | 89.8 (3) | O1_2—Co1—O1_3 | 89.3 (3) |
O1_2—Ti1—O1_3 | 90.2 (3) | O1_2—Co1—O1_3 | 90.7 (3) |
O1_3—Ti1—O1_3 | 180.0 (2) | O1_3—Co1—O1_3 | 180.0 (2) |
Symmetry codes: (i) x+1, y−1, z; (ii) −x−1/2, y−1/2, −z+1/2; (iii) −x−1, −y+1, −z; (iv) x+1/2, −y+1/2, z+1/2; (v) x, y−1, z; (vi) −x, −y+1, −z; (vii) −x+1/2, y−1/2, −z+1/2; (viii) x+1, y, z; (ix) x+1/2, −y+3/2, z+1/2; (x) −x, −y+1, −z+1. |
CoLa1.8O6Sr0.2Ti | Z = 2 |
Mr = 470.39 | ? _exptl_crystal_density_diffrn 6.452(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 414.4 |
Monoclinic, P21/n | Synchrotron radiation, λ = 0.621000 Å |
Hall symbol: -P 2yn | µ = 7.73 mm−1 |
a = 5.55020 (11) Å | T = 295 K |
b = 5.54838 (9) Å | Particle morphology: plate-like SEM |
c = 7.83763 (10) Å | black |
β = 90.014 (7)° | cylinder, 15 × 20 mm |
V = 241.36 (1) Å3 |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Scan method: step |
Radiation source: Synchrotron | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Si 111 monochromator | Tmin = ?, Tmax = ? |
Specimen mounting: Borosilicate 0.3 mm capillary | 2θmin = 7.011°, 2θmax = 37.302°, 2θstep = 0.010° |
Data collection mode: transmission |
Refinement on Inet | 3030 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.156 | 40 parameters |
Rwp = 0.239 | 0 restraints |
Rexp = 0.213 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.079 | (Δ/σ)max = 0.01 |
χ2 = 1.573 | Background function: Set of experimental background points |
CoLa1.8O6Sr0.2Ti | V = 241.36 (1) Å3 |
Mr = 470.39 | Z = 2 |
Monoclinic, P21/n | Synchrotron radiation, λ = 0.621000 Å |
a = 5.55020 (11) Å | µ = 7.73 mm−1 |
b = 5.54838 (9) Å | T = 295 K |
c = 7.83763 (10) Å | cylinder, 15 × 20 mm |
β = 90.014 (7)° |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Specimen mounting: Borosilicate 0.3 mm capillary | Tmin = ?, Tmax = ? |
Data collection mode: transmission | 2θmin = 7.011°, 2θmax = 37.302°, 2θstep = 0.010° |
Scan method: step |
Rp = 0.156 | χ2 = 1.573 |
Rwp = 0.239 | 3030 data points |
Rexp = 0.213 | 40 parameters |
RBragg = 0.079 | 0 restraints |
Experimental. Synchrotron source |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
La1 | 0.0048 (4) | −0.0271 (2) | 0.2503 (16) | 0.0075 (2)* | 0.90000 |
Sr1 | 0.0048 (4) | −0.0271 (2) | 0.2503 (16) | 0.0075 (2)* | 0.10000 |
Ti1 | 0.00000 | 0.50000 | 0.00000 | 0.007 (3)* | 0.56308 |
Co2 | 0.00000 | 0.50000 | 0.00000 | 0.007 (3)* | 0.43694 |
O1 | −0.7219 (11) | 0.7228 (11) | 0.0387 (10) | 0.014 (2)* | |
O1_2 | −0.2173 (11) | 0.7849 (11) | −0.0351 (10) | 0.0049 (16)* | |
O1_3 | −0.0689 (4) | 0.51043 (5) | 0.2510 (15) | 0.0072 (4)* | |
Co1 | 0.00000 | 0.50000 | 0.50000 | 0.007 (8)* | 0.56308 |
Ti2 | 0.00000 | 0.50000 | 0.50000 | 0.007 (8)* | 0.43694 |
La1—O1i | 2.642 (11) | Ti1—O1viii | 2.001 (6) |
La1—O1ii | 2.471 (11) | Ti1—O1iii | 2.001 (6) |
La1—O1iii | 3.232 (11) | Ti1—O1_2 | 2.007 (6) |
La1—O1iv | 2.806 (12) | Ti1—O1_2vi | 2.007 (6) |
La1—O1_2v | 2.759 (13) | Ti1—O1_3 | 2.005 (12) |
La1—O1_2ii | 3.245 (11) | Ti1—O1_3vi | 2.005 (12) |
La1—O1_2vi | 2.458 (11) | Co1—O1ii | 1.994 (6) |
La1—O1_2iv | 2.693 (10) | Co1—O1ix | 1.994 (6) |
La1—O1_3v | 2.5984 (12) | Co1—O1_2ii | 1.991 (6) |
La1—O1_3 | 3.0103 (12) | Co1—O1_2ix | 1.991 (6) |
La1—O1_3ii | 2.428 (3) | Co1—O1_3 | 1.989 (12) |
La1—O1_3vii | 3.138 (3) | Co1—O1_3x | 1.989 (12) |
O1—Ti1—O1 | 180.0 (6) | O1—Co1—O1 | 180.0 (6) |
O1—Ti1—O1_2 | 89.9 (4) | O1—Co1—O1_2 | 92.6 (4) |
O1—Ti1—O1_2 | 90.1 (4) | O1—Co1—O1_2 | 87.4 (4) |
O1—Ti1—O1_3 | 88.9 (5) | O1—Co1—O1_3 | 89.5 (5) |
O1—Ti1—O1_3 | 91.1 (6) | O1—Co1—O1_3 | 90.5 (6) |
O1—Ti1—O1_2 | 90.1 (4) | O1—Co1—O1_2 | 87.4 (4) |
O1—Ti1—O1_2 | 89.9 (4) | O1—Co1—O1_2 | 92.6 (4) |
O1—Ti1—O1_3 | 91.1 (6) | O1—Co1—O1_3 | 90.5 (6) |
O1—Ti1—O1_3 | 88.9 (5) | O1—Co1—O1_3 | 89.5 (5) |
O1_2—Ti1—O1_2 | 180.0 (6) | O1_2—Co1—O1_2 | 180.0 (6) |
O1_2—Ti1—O1_3 | 89.8 (6) | O1_2—Co1—O1_3 | 90.1 (6) |
O1_2—Ti1—O1_3 | 90.2 (5) | O1_2—Co1—O1_3 | 89.9 (6) |
O1_2—Ti1—O1_3 | 90.2 (5) | O1_2—Co1—O1_3 | 89.9 (6) |
O1_2—Ti1—O1_3 | 89.8 (6) | O1_2—Co1—O1_3 | 90.1 (6) |
O1_3—Ti1—O1_3 | 180.0 (10) | O1_3—Co1—O1_3 | 180.0 (11) |
Symmetry codes: (i) x+1, y−1, z; (ii) −x−1/2, y−1/2, −z+1/2; (iii) −x−1, −y+1, −z; (iv) x+1/2, −y+1/2, z+1/2; (v) x, y−1, z; (vi) −x, −y+1, −z; (vii) −x+1/2, y−1/2, −z+1/2; (viii) x+1, y, z; (ix) x+1/2, −y+3/2, z+1/2; (x) −x, −y+1, −z+1. |
CoLa1.8O6Sr0.2Ti | Z = 2 |
Mr = 470.39 | ? _exptl_crystal_density_diffrn 6.452(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 100.4 |
Monoclinic, P21/n | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
Hall symbol: -P 2yn | µ = 0.00 mm−1 |
a = 5.55020 (11) Å | T = 295 K |
b = 5.54838 (9) Å | Particle morphology: plate-like SEM |
c = 7.83763 (10) Å | black |
β = 90.014 (7)° | cylinder, 15 × 20 mm |
V = 241.36 (1) Å3 |
High-resolution two-axis diffractometer | Data collection mode: transmission |
Radiation source: nuclear reactor, D2B beamline ILL | Scan method: step |
Ge monochromator | 2θmin = 0.241°, 2θmax = 160.191°, 2θstep = 0.050° |
Specimen mounting: 'vanadium can' |
Refinement on Inet | 3901 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.035 | 40 parameters |
Rwp = 0.045 | 0 restraints |
Rexp = 0.026 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.025 | (Δ/σ)max = 0.01 |
χ2 = 8.804 | Background function: Set of experimental background points |
CoLa1.8O6Sr0.2Ti | V = 241.36 (1) Å3 |
Mr = 470.39 | Z = 2 |
Monoclinic, P21/n | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
a = 5.55020 (11) Å | µ = 0.00 mm−1 |
b = 5.54838 (9) Å | T = 295 K |
c = 7.83763 (10) Å | cylinder, 15 × 20 mm |
β = 90.014 (7)° |
High-resolution two-axis diffractometer | Scan method: step |
Specimen mounting: 'vanadium can' | 2θmin = 0.241°, 2θmax = 160.191°, 2θstep = 0.050° |
Data collection mode: transmission |
Rp = 0.035 | χ2 = 8.804 |
Rwp = 0.045 | 3901 data points |
Rexp = 0.026 | 40 parameters |
RBragg = 0.025 | 0 restraints |
Experimental. Neutron reactor |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
La1 | 0.0048 (4) | −0.0271 (2) | 0.2503 (16) | 0.0075 (2)* | 0.90000 |
Sr1 | 0.0048 (4) | −0.0271 (2) | 0.2503 (16) | 0.0075 (2)* | 0.10000 |
Ti1 | 0.00000 | 0.50000 | 0.00000 | 0.007 (3)* | 0.56308 |
Co2 | 0.00000 | 0.50000 | 0.00000 | 0.007 (3)* | 0.43694 |
O1 | −0.7219 (11) | 0.7228 (11) | 0.0387 (10) | 0.014 (2)* | |
O1_2 | −0.2173 (11) | 0.7849 (11) | −0.0351 (10) | 0.0049 (16)* | |
O1_3 | −0.0689 (4) | 0.51043 (5) | 0.2510 (15) | 0.0072 (4)* | |
Co1 | 0.00000 | 0.50000 | 0.50000 | 0.007 (8)* | 0.56308 |
Ti2 | 0.00000 | 0.50000 | 0.50000 | 0.007 (8)* | 0.43694 |
La1—O1i | 2.642 (11) | Ti1—O1viii | 2.001 (6) |
La1—O1ii | 2.471 (11) | Ti1—O1iii | 2.001 (6) |
La1—O1iii | 3.232 (11) | Ti1—O1_2 | 2.007 (6) |
La1—O1iv | 2.806 (12) | Ti1—O1_2vi | 2.007 (6) |
La1—O1_2v | 2.759 (13) | Ti1—O1_3 | 2.005 (12) |
La1—O1_2ii | 3.245 (11) | Ti1—O1_3vi | 2.005 (12) |
La1—O1_2vi | 2.458 (11) | Co1—O1ii | 1.994 (6) |
La1—O1_2iv | 2.693 (10) | Co1—O1ix | 1.994 (6) |
La1—O1_3v | 2.5984 (12) | Co1—O1_2ii | 1.991 (6) |
La1—O1_3 | 3.0103 (12) | Co1—O1_2ix | 1.991 (6) |
La1—O1_3ii | 2.428 (3) | Co1—O1_3 | 1.989 (12) |
La1—O1_3vii | 3.138 (3) | Co1—O1_3x | 1.989 (12) |
O1—Ti1—O1 | 180.0 (6) | O1—Co1—O1 | 180.0 (6) |
O1—Ti1—O1_2 | 89.9 (4) | O1—Co1—O1_2 | 92.6 (4) |
O1—Ti1—O1_2 | 90.1 (4) | O1—Co1—O1_2 | 87.4 (4) |
O1—Ti1—O1_3 | 88.9 (5) | O1—Co1—O1_3 | 89.5 (5) |
O1—Ti1—O1_3 | 91.1 (6) | O1—Co1—O1_3 | 90.5 (6) |
O1—Ti1—O1_2 | 90.1 (4) | O1—Co1—O1_2 | 87.4 (4) |
O1—Ti1—O1_2 | 89.9 (4) | O1—Co1—O1_2 | 92.6 (4) |
O1—Ti1—O1_3 | 91.1 (6) | O1—Co1—O1_3 | 90.5 (6) |
O1—Ti1—O1_3 | 88.9 (5) | O1—Co1—O1_3 | 89.5 (5) |
O1_2—Ti1—O1_2 | 180.0 (6) | O1_2—Co1—O1_2 | 180.0 (6) |
O1_2—Ti1—O1_3 | 89.8 (6) | O1_2—Co1—O1_3 | 90.1 (6) |
O1_2—Ti1—O1_3 | 90.2 (5) | O1_2—Co1—O1_3 | 89.9 (6) |
O1_2—Ti1—O1_3 | 90.2 (5) | O1_2—Co1—O1_3 | 89.9 (6) |
O1_2—Ti1—O1_3 | 89.8 (6) | O1_2—Co1—O1_3 | 90.1 (6) |
O1_3—Ti1—O1_3 | 180.0 (10) | O1_3—Co1—O1_3 | 180.0 (11) |
Symmetry codes: (i) x+1, y−1, z; (ii) −x−1/2, y−1/2, −z+1/2; (iii) −x−1, −y+1, −z; (iv) x+1/2, −y+1/2, z+1/2; (v) x, y−1, z; (vi) −x, −y+1, −z; (vii) −x+1/2, y−1/2, −z+1/2; (viii) x+1, y, z; (ix) x+1/2, −y+3/2, z+1/2; (x) −x, −y+1, −z+1. |
CoLa1.7O6Sr0.3Ti | Z = 2 |
Mr = 465.26 | ? _exptl_crystal_density_diffrn 6.443(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 410.4 |
Orthorhombic, Pnma | Synchrotron radiation, λ = 0.621000 Å |
Hall symbol: -P 2ac 2n | µ = 7.92 mm−1 |
a = 5.52939 (10) Å | T = 295 K |
b = 7.81873 (13) Å | Particle morphology: plate-like SEM |
c = 5.54331 (9) Å | black |
V = 239.65 (1) Å3 | cylinder, 15 × 20 mm |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Scan method: step |
Radiation source: Synchrotron | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Si 111 monochromator | Tmin = ?, Tmax = ? |
Specimen mounting: Borosilicate 0.3 mm capillary | 2θmin = 8.056°, 2θmax = 46.996°, 2θstep = 0.010° |
Data collection mode: transmission |
Refinement on Inet | 3895 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.059 | 30 parameters |
Rwp = 0.077 | 0 restraints |
Rexp = 0.058 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.042 | (Δ/σ)max = 0.01 |
χ2 = 3.082 | Background function: Set of experimental background points |
CoLa1.7O6Sr0.3Ti | V = 239.65 (1) Å3 |
Mr = 465.26 | Z = 2 |
Orthorhombic, Pnma | Synchrotron radiation, λ = 0.621000 Å |
a = 5.52939 (10) Å | µ = 7.92 mm−1 |
b = 7.81873 (13) Å | T = 295 K |
c = 5.54331 (9) Å | cylinder, 15 × 20 mm |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Specimen mounting: Borosilicate 0.3 mm capillary | Tmin = ?, Tmax = ? |
Data collection mode: transmission | 2θmin = 8.056°, 2θmax = 46.996°, 2θstep = 0.010° |
Scan method: step |
Rp = 0.059 | χ2 = 3.082 |
Rwp = 0.077 | 3895 data points |
Rexp = 0.058 | 30 parameters |
RBragg = 0.042 | 0 restraints |
Experimental. Synchrotron source |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Co1 | 0.50000 | 0.00000 | 0.00000 | 0.0014 (5)* | 0.50000 |
Ti1 | 0.50000 | 0.00000 | 0.00000 | 0.0014 (5)* | 0.50000 |
La1 | 0.02348 (16) | 0.25000 | 0.0037 (4) | 0.00622 (17)* | 0.84700 |
Sr1 | 0.02348 (16) | 0.25000 | 0.0037 (4) | 0.00622 (17)* | 0.15300 |
O1 | 0.7774 (3) | 0.0348 (2) | 0.2228 (3) | 0.0076 (3)* | |
O1_2 | 0.0084 (4) | 0.75000 | 0.4341 (4) | 0.0078 (4)* |
La1—O1i | 2.482 (2) | La1—O1_2x | 3.121 (3) |
La1—O1ii | 2.665 (2) | La1—O1_2xi | 2.966 (2) |
La1—O1iii | 2.7833 (19) | La1—O1_2xii | 2.617 (2) |
La1—O1iv | 3.186 (2) | Co1—O1 | 1.9880 (17) |
La1—O1v | 2.7833 (19) | Co1—O1xiii | 1.9875 (17) |
La1—O1vi | 3.186 (2) | Co1—O1v | 1.9880 (17) |
La1—O1vii | 2.482 (2) | Co1—O1viii | 1.9875 (17) |
La1—O1viii | 2.665 (2) | Co1—O1_2xiv | 1.9891 (4) |
La1—O1_2ix | 2.433 (3) | Co1—O1_2xii | 1.9891 (4) |
O1—Co1—O1 | 91.22 (12) | O1—Co1—O1_2 | 90.40 (10) |
O1—Co1—O1 | 180.00 (15) | O1—Co1—O1 | 91.22 (12) |
O1—Co1—O1 | 88.78 (12) | O1—Co1—O1_2 | 89.87 (11) |
O1—Co1—O1_2 | 90.13 (10) | O1—Co1—O1_2 | 90.13 (10) |
O1—Co1—O1_2 | 89.87 (11) | O1—Co1—O1_2 | 90.40 (10) |
O1—Co1—O1 | 88.78 (12) | O1—Co1—O1_2 | 89.60 (11) |
O1—Co1—O1 | 180.00 (15) | O1_2—Co1—O1_2 | 180.00 (4) |
O1—Co1—O1_2 | 89.60 (11) |
Symmetry codes: (i) x−1, y, z; (ii) x−1/2, −y+1/2, −z+1/2; (iii) −x+1, y+1/2, −z; (iv) −x+1/2, −y, z−1/2; (v) −x+1, −y, −z; (vi) −x+1/2, y+1/2, z−1/2; (vii) x−1, −y+1/2, z; (viii) x−1/2, y, −z+1/2; (ix) −x, y−1/2, −z; (x) −x, y−1/2, −z+1; (xi) −x−1/2, −y+1, z−1/2; (xii) −x+1/2, −y+1, z−1/2; (xiii) −x+3/2, −y, z−1/2; (xiv) x+1/2, −y+1/2, −z+1/2. |
CoLa1.7O6Sr0.3Ti | Z = 2 |
Mr = 465.26 | ? _exptl_crystal_density_diffrn 6.443(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 100.1 |
Orthorhombic, Pnma | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
Hall symbol: -P 2ac 2n | µ = 0.00 mm−1 |
a = 5.52939 (10) Å | T = 295 K |
b = 7.81873 (13) Å | Particle morphology: plate-like SEM |
c = 5.54331 (9) Å | black |
V = 239.65 (1) Å3 | cylinder, 15 × 20 mm |
High-resolution two-axis diffractometer | Data collection mode: transmission |
Radiation source: nuclear reactor, D2B beamline ILL | Scan method: step |
Ge monochromator | 2θmin = 0.309°, 2θmax = 160.220°, 2θstep = 0.050° |
Specimen mounting: 'vanadium can' |
Refinement on Inet | 4061 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.036 | 30 parameters |
Rwp = 0.045 | 0 restraints |
Rexp = 0.027 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.021 | (Δ/σ)max = 0.01 |
χ2 = 6.965 | Background function: Set of experimental background points |
CoLa1.7O6Sr0.3Ti | V = 239.65 (1) Å3 |
Mr = 465.26 | Z = 2 |
Orthorhombic, Pnma | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
a = 5.52939 (10) Å | µ = 0.00 mm−1 |
b = 7.81873 (13) Å | T = 295 K |
c = 5.54331 (9) Å | cylinder, 15 × 20 mm |
High-resolution two-axis diffractometer | Scan method: step |
Specimen mounting: 'vanadium can' | 2θmin = 0.309°, 2θmax = 160.220°, 2θstep = 0.050° |
Data collection mode: transmission |
Rp = 0.036 | χ2 = 6.965 |
Rwp = 0.045 | 4061 data points |
Rexp = 0.027 | 30 parameters |
RBragg = 0.021 | 0 restraints |
Experimental. Neutron reactor |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Co1 | 0.50000 | 0.00000 | 0.00000 | 0.0014 (5)* | 0.50000 |
Ti1 | 0.50000 | 0.00000 | 0.00000 | 0.0014 (5)* | 0.50000 |
La1 | 0.02348 (16) | 0.25000 | 0.0037 (4) | 0.00622 (17)* | 0.84700 |
Sr1 | 0.02348 (16) | 0.25000 | 0.0037 (4) | 0.00622 (17)* | 0.15300 |
O1 | 0.7774 (3) | 0.0348 (2) | 0.2228 (3) | 0.0076 (3)* | |
O1_2 | 0.0084 (4) | 0.75000 | 0.4341 (4) | 0.0078 (4)* |
La1—O1i | 2.482 (2) | La1—O1_2x | 3.121 (3) |
La1—O1ii | 2.665 (2) | La1—O1_2xi | 2.966 (2) |
La1—O1iii | 2.7833 (19) | La1—O1_2xii | 2.617 (2) |
La1—O1iv | 3.186 (2) | Co1—O1 | 1.9880 (17) |
La1—O1v | 2.7833 (19) | Co1—O1xiii | 1.9875 (17) |
La1—O1vi | 3.186 (2) | Co1—O1v | 1.9880 (17) |
La1—O1vii | 2.482 (2) | Co1—O1viii | 1.9875 (17) |
La1—O1viii | 2.665 (2) | Co1—O1_2xiv | 1.9891 (4) |
La1—O1_2ix | 2.433 (3) | Co1—O1_2xii | 1.9891 (4) |
O1—Co1—O1 | 91.22 (12) | O1—Co1—O1_2 | 90.40 (10) |
O1—Co1—O1 | 180.00 (15) | O1—Co1—O1 | 91.22 (12) |
O1—Co1—O1 | 88.78 (12) | O1—Co1—O1_2 | 89.87 (11) |
O1—Co1—O1_2 | 90.13 (10) | O1—Co1—O1_2 | 90.13 (10) |
O1—Co1—O1_2 | 89.87 (11) | O1—Co1—O1_2 | 90.40 (10) |
O1—Co1—O1 | 88.78 (12) | O1—Co1—O1_2 | 89.60 (11) |
O1—Co1—O1 | 180.00 (15) | O1_2—Co1—O1_2 | 180.00 (4) |
O1—Co1—O1_2 | 89.60 (11) |
Symmetry codes: (i) x−1, y, z; (ii) x−1/2, −y+1/2, −z+1/2; (iii) −x+1, y+1/2, −z; (iv) −x+1/2, −y, z−1/2; (v) −x+1, −y, −z; (vi) −x+1/2, y+1/2, z−1/2; (vii) x−1, −y+1/2, z; (viii) x−1/2, y, −z+1/2; (ix) −x, y−1/2, −z; (x) −x, y−1/2, −z+1; (xi) −x−1/2, −y+1, z−1/2; (xii) −x+1/2, −y+1, z−1/2; (xiii) −x+3/2, −y, z−1/2; (xiv) x+1/2, −y+1/2, −z+1/2. |
CoLa1.5O6Sr0.5Ti | Z = 2 |
Mr = 455.00 | ? _exptl_crystal_density_diffrn 6.391(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 402.8 |
Orthorhombic, Pnma | Synchrotron radiation, λ = 0.621000 Å |
Hall symbol: -P 2ac 2n | µ = 8.31 mm−1 |
a = 5.49186 (7) Å | T = 295 K |
b = 7.77013 (10) Å | Particle morphology: plate-like SEM |
c = 5.53014 (7) Å | black |
V = 235.99 (1) Å3 | cylinder, 15 × 20 mm |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Scan method: step |
Radiation source: Synchrotron | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Si 111 monochromator | Tmin = ?, Tmax = ? |
Specimen mounting: Borosilicate 0.3 mm capillary | 2θmin = 8.069°, 2θmax = 47.009°, 2θstep = 0.010° |
Data collection mode: transmission |
Refinement on Inet | 3895 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.070 | 34 parameters |
Rwp = 0.089 | 0 restraints |
Rexp = 0.059 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.058 | (Δ/σ)max = 0.01 |
χ2 = 5.045 | Background function: Set of experimental background points |
CoLa1.5O6Sr0.5Ti | V = 235.99 (1) Å3 |
Mr = 455.00 | Z = 2 |
Orthorhombic, Pnma | Synchrotron radiation, λ = 0.621000 Å |
a = 5.49186 (7) Å | µ = 8.31 mm−1 |
b = 7.77013 (10) Å | T = 295 K |
c = 5.53014 (7) Å | cylinder, 15 × 20 mm |
Home-made heavy-duty Theta-2theta goniometer diffractometer | Absorption correction: for a cylinder mounted on the φ axis Cromer and Liberman algorithm |
Specimen mounting: Borosilicate 0.3 mm capillary | Tmin = ?, Tmax = ? |
Data collection mode: transmission | 2θmin = 8.069°, 2θmax = 47.009°, 2θstep = 0.010° |
Scan method: step |
Rp = 0.070 | χ2 = 5.045 |
Rwp = 0.089 | 3895 data points |
Rexp = 0.059 | 34 parameters |
RBragg = 0.058 | 0 restraints |
Experimental. Synchrotron source |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Co1 | 0.50000 | 0.00000 | 0.00000 | 0.0076 (10)* | 0.50000 |
Ti1 | 0.50000 | 0.00000 | 0.00000 | 0.0076 (10)* | 0.50000 |
La1 | 0.0092 (3) | 0.25000 | 0.0021 (2) | 0.00989 (17)* | 0.74672 |
Sr1 | 0.0092 (3) | 0.25000 | 0.0021 (2) | 0.00989 (17)* | 0.25328 |
O1 | 0.7631 (3) | 0.03058 (11) | 0.2374 (3) | 0.0125 (2)* | |
O1_2 | 0.0029 (5) | 0.75000 | 0.4426 (2) | 0.0091 (3)* |
La1—O1i | 2.5351 (17) | La1—O1_2x | 3.0716 (16) |
La1—O1ii | 2.6318 (17) | La1—O1_2xi | 2.832 (3) |
La1—O1iii | 2.8409 (15) | La1—O1_2xii | 2.700 (3) |
La1—O1iv | 3.0219 (16) | Co1—O1 | 1.9667 (16) |
La1—O1v | 2.8409 (15) | Co1—O1xiii | 1.9642 (16) |
La1—O1vi | 3.0219 (16) | Co1—O1v | 1.9667 (16) |
La1—O1vii | 2.5351 (17) | Co1—O1viii | 1.9642 (16) |
La1—O1viii | 2.6318 (17) | Co1—O1_2xiv | 1.9684 (2) |
La1—O1_2ix | 2.4602 (16) | Co1—O1_2xii | 1.9684 (2) |
O1—Co1—O1 | 91.23 (12) | O1—Co1—O1_2 | 90.32 (9) |
O1—Co1—O1 | 180.00 (15) | O1—Co1—O1 | 91.23 (12) |
O1—Co1—O1 | 88.77 (12) | O1—Co1—O1_2 | 89.68 (10) |
O1—Co1—O1_2 | 90.32 (9) | O1—Co1—O1_2 | 90.32 (9) |
O1—Co1—O1_2 | 89.68 (10) | O1—Co1—O1_2 | 90.32 (9) |
O1—Co1—O1 | 88.77 (12) | O1—Co1—O1_2 | 89.68 (10) |
O1—Co1—O1 | 180.00 (15) | O1_2—Co1—O1_2 | 180.000 (17) |
O1—Co1—O1_2 | 89.68 (10) |
Symmetry codes: (i) x−1, y, z; (ii) x−1/2, −y+1/2, −z+1/2; (iii) −x+1, y+1/2, −z; (iv) −x+1/2, −y, z−1/2; (v) −x+1, −y, −z; (vi) −x+1/2, y+1/2, z−1/2; (vii) x−1, −y+1/2, z; (viii) x−1/2, y, −z+1/2; (ix) −x, y−1/2, −z; (x) −x, y−1/2, −z+1; (xi) −x−1/2, −y+1, z−1/2; (xii) −x+1/2, −y+1, z−1/2; (xiii) −x+3/2, −y, z−1/2; (xiv) x+1/2, −y+1/2, −z+1/2. |
CoLa1.5O6Sr0.5Ti | Z = 2 |
Mr = 455.00 | ? _exptl_crystal_density_diffrn 6.391(1) _exptl_crystal_density_meas ? _exptl_crystal_density_method 'not measured' _exptl_crystal_F_000 99.6 |
Orthorhombic, Pnma | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
Hall symbol: -P 2ac 2n | µ = 0.00 mm−1 |
a = 5.49186 (7) Å | T = 295 K |
b = 7.77013 (10) Å | Particle morphology: plate-like SEM |
c = 5.53014 (7) Å | black |
V = 235.99 (1) Å3 | cylinder, 15 × 20 mm |
High-resolution two-axis diffractometer | Data collection mode: transmission |
Radiation source: nuclear reactor, D2B beamline ILL | Scan method: step |
Ge monochromator | 2θmin = 0.270°, 2θmax = 160.229°, 2θstep = 0.050° |
Specimen mounting: 'vanadium can' |
Refinement on Inet | 3895 data points |
Least-squares matrix: full with fixed elements per cycle | Profile function: pseudo-Voigt |
Rp = 0.030 | 34 parameters |
Rwp = 0.040 | 0 restraints |
Rexp = 0.016 | Weighting scheme based on measured s.u.'s 1/[Yi + σ(Yi)] |
RBragg = 0.027 | (Δ/σ)max = 0.01 |
χ2 = 41.290 | Background function: Set of experimental background points |
CoLa1.5O6Sr0.5Ti | V = 235.99 (1) Å3 |
Mr = 455.00 | Z = 2 |
Orthorhombic, Pnma | Constant Wavelength Neutron Diffraction radiation, λ = 1.594000 Å |
a = 5.49186 (7) Å | µ = 0.00 mm−1 |
b = 7.77013 (10) Å | T = 295 K |
c = 5.53014 (7) Å | cylinder, 15 × 20 mm |
High-resolution two-axis diffractometer | Scan method: step |
Specimen mounting: 'vanadium can' | 2θmin = 0.270°, 2θmax = 160.229°, 2θstep = 0.050° |
Data collection mode: transmission |
Rp = 0.030 | χ2 = 41.290 |
Rwp = 0.040 | 3895 data points |
Rexp = 0.016 | 34 parameters |
RBragg = 0.027 | 0 restraints |
Experimental. Neutron reactor |
Refinement. Symmetry-adapted Rietveld refinement by simulteneuos fitting of SXRD and NPD data. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Co1 | 0.50000 | 0.00000 | 0.00000 | 0.0076 (10)* | 0.50000 |
Ti1 | 0.50000 | 0.00000 | 0.00000 | 0.0076 (10)* | 0.50000 |
La1 | 0.0092 (3) | 0.25000 | 0.0021 (2) | 0.00989 (17)* | 0.74672 |
Sr1 | 0.0092 (3) | 0.25000 | 0.0021 (2) | 0.00989 (17)* | 0.25328 |
O1 | 0.7631 (3) | 0.03058 (11) | 0.2374 (3) | 0.0125 (2)* | |
O1_2 | 0.0029 (5) | 0.75000 | 0.4426 (2) | 0.0091 (3)* |
La1—O1i | 2.5351 (17) | La1—O1_2x | 3.0716 (16) |
La1—O1ii | 2.6318 (17) | La1—O1_2xi | 2.832 (3) |
La1—O1iii | 2.8409 (15) | La1—O1_2xii | 2.700 (3) |
La1—O1iv | 3.0219 (16) | Co1—O1 | 1.9667 (16) |
La1—O1v | 2.8409 (15) | Co1—O1xiii | 1.9642 (16) |
La1—O1vi | 3.0219 (16) | Co1—O1v | 1.9667 (16) |
La1—O1vii | 2.5351 (17) | Co1—O1viii | 1.9642 (16) |
La1—O1viii | 2.6318 (17) | Co1—O1_2xiv | 1.9684 (2) |
La1—O1_2ix | 2.4602 (16) | Co1—O1_2xii | 1.9684 (2) |
O1—Co1—O1 | 91.23 (12) | O1—Co1—O1_2 | 90.32 (9) |
O1—Co1—O1 | 180.00 (15) | O1—Co1—O1 | 91.23 (12) |
O1—Co1—O1 | 88.77 (12) | O1—Co1—O1_2 | 89.68 (10) |
O1—Co1—O1_2 | 90.32 (9) | O1—Co1—O1_2 | 90.32 (9) |
O1—Co1—O1_2 | 89.68 (10) | O1—Co1—O1_2 | 90.32 (9) |
O1—Co1—O1 | 88.77 (12) | O1—Co1—O1_2 | 89.68 (10) |
O1—Co1—O1 | 180.00 (15) | O1_2—Co1—O1_2 | 180.000 (17) |
O1—Co1—O1_2 | 89.68 (10) |
Symmetry codes: (i) x−1, y, z; (ii) x−1/2, −y+1/2, −z+1/2; (iii) −x+1, y+1/2, −z; (iv) −x+1/2, −y, z−1/2; (v) −x+1, −y, −z; (vi) −x+1/2, y+1/2, z−1/2; (vii) x−1, −y+1/2, z; (viii) x−1/2, y, −z+1/2; (ix) −x, y−1/2, −z; (x) −x, y−1/2, −z+1; (xi) −x−1/2, −y+1, z−1/2; (xii) −x+1/2, −y+1, z−1/2; (xiii) −x+3/2, −y, z−1/2; (xiv) x+1/2, −y+1/2, −z+1/2. |
Experimental details
(LCTO_SXRD) | (LCTO_NPD) | (LSCT10_XRD) | (LSCT10_NPD) | |
Crystal data | ||||
Chemical formula | Co2La4O12Ti2 | Co2La4O12Ti2 | CoLa1.9O6Sr0.1Ti | CoLa1.9O6Sr0.1Ti |
Mr | 480.62 | 480.62 | 475.52 | 475.52 |
Crystal system, space group | Monoclinic, P21/n | Monoclinic, P21/n | Monoclinic, P21/n | Monoclinic, P21/n |
Temperature (K) | 295 | 295 | 295 | 295 |
a, b, c (Å) | 5.55510 (9), 5.57813 (8), 7.85718 (12) | 5.55510 (9), 5.57813 (8), 7.85718 (12) | 5.55318 (8), 5.56557 (7), 7.84995 (10) | 5.55318 (8), 5.56557 (7), 7.84995 (10) |
α, β, γ (°) | 90, 90.005 (5), 90 | 90, 90.005 (5), 90 | 90, 90.007 (5), 90 | 90, 90.007 (5), 90 |
V (Å3) | 243.47 (1) | 243.47 (1) | 242.62 (1) | 242.62 (1) |
Z | 2 | 2 | 2 | 2 |
Radiation type | Synchrotron, λ = 0.621000 Å | Constant Wavelength Neutron Diffraction, λ = 1.594000 Å | Cu Kα1, λ = 1.540560 Å | Constant Wavelength Neutron Diffraction, λ = 1.594000 Å |
µ (mm−1) | 7.37 | 0.00 | – | 0.00 |
Specimen shape, size (mm) | Cylinder, 15 × 20 | Cylinder, 15 × 20 | Flat sheet, 20 × 20 | Cylinder, 15 × 20 |
Data collection | ||||
Diffractometer | Home-made heavy-duty Theta-2theta goniometer diffractometer | High-resolution two-axis diffractometer | Bruker D8 Advance diffractometer | High-resolution two-axis diffractometer |
Specimen mounting | Borosilicate 0.3 mm capillary | 'vanadium can' | Aluminium Sample holder | 'vanadium can' |
Data collection mode | Transmission | Transmission | Reflexion | Transmission |
Scan method | Step | Step | Step | Step |
Absorption correction | For a cylinder mounted on the φ axis Cromer and Liberman algorithm | – | – | – |
2θ values (°) | 2θmin = 7.989 2θmax = 46.991 2θstep = 0.010 | 2θmin = 0.239 2θmax = 160.189 2θstep = 0.050 | 2θmin = 19.880 2θmax = 99.882 2θstep = 0.020 | 2θmin = 0.245 2θmax = 160.195 2θstep = 0.050 |
Refinement | ||||
R factors and goodness of fit | Rp = 0.073, Rwp = 0.100, Rexp = 0.058, RBragg = 0.036, χ2 = 8.418 | Rp = 0.046, Rwp = 0.059, Rexp = 0.039, RBragg = 0.032, χ2 = 5.505 | Rp = 0.036, Rwp = 0.047, Rexp = 0.035, RBragg = 0.083, χ2 = 3.147 | Rp = 0.364, Rwp = 0.047, Rexp = 0.027, RBragg = 0.023, χ2 = 9.624 |
No. of data points | 3901 | 3901 | 4061 | 4061 |
No. of parameters | 40 | 40 | 34 | 34 |
(LSCT20_SXRD) | (LSCT20_NPD) | (LSCT30_SXRD) | (LSCT30_NPD) | |
Crystal data | ||||
Chemical formula | CoLa1.8O6Sr0.2Ti | CoLa1.8O6Sr0.2Ti | CoLa1.7O6Sr0.3Ti | CoLa1.7O6Sr0.3Ti |
Mr | 470.39 | 470.39 | 465.26 | 465.26 |
Crystal system, space group | Monoclinic, P21/n | Monoclinic, P21/n | Orthorhombic, Pnma | Orthorhombic, Pnma |
Temperature (K) | 295 | 295 | 295 | 295 |
a, b, c (Å) | 5.55020 (11), 5.54838 (9), 7.83763 (10) | 5.55020 (11), 5.54838 (9), 7.83763 (10) | 5.52939 (10), 7.81873 (13), 5.54331 (9) | 5.52939 (10), 7.81873 (13), 5.54331 (9) |
α, β, γ (°) | 90, 90.014 (7), 90 | 90, 90.014 (7), 90 | 90, 90, 90 | 90, 90, 90 |
V (Å3) | 241.36 (1) | 241.36 (1) | 239.65 (1) | 239.65 (1) |
Z | 2 | 2 | 2 | 2 |
Radiation type | Synchrotron, λ = 0.621000 Å | Constant Wavelength Neutron Diffraction, λ = 1.594000 Å | Synchrotron, λ = 0.621000 Å | Constant Wavelength Neutron Diffraction, λ = 1.594000 Å |
µ (mm−1) | 7.73 | 0.00 | 7.92 | 0.00 |
Specimen shape, size (mm) | Cylinder, 15 × 20 | Cylinder, 15 × 20 | Cylinder, 15 × 20 | Cylinder, 15 × 20 |
Data collection | ||||
Diffractometer | Home-made heavy-duty Theta-2theta goniometer diffractometer | High-resolution two-axis diffractometer | Home-made heavy-duty Theta-2theta goniometer diffractometer | High-resolution two-axis diffractometer |
Specimen mounting | Borosilicate 0.3 mm capillary | 'vanadium can' | Borosilicate 0.3 mm capillary | 'vanadium can' |
Data collection mode | Transmission | Transmission | Transmission | Transmission |
Scan method | Step | Step | Step | Step |
Absorption correction | – | – | – | – |
2θ values (°) | 2θmin = 7.011 2θmax = 37.302 2θstep = 0.010 | 2θmin = 0.241 2θmax = 160.191 2θstep = 0.050 | 2θmin = 8.056 2θmax = 46.996 2θstep = 0.010 | 2θmin = 0.309 2θmax = 160.220 2θstep = 0.050 |
Refinement | ||||
R factors and goodness of fit | Rp = 0.156, Rwp = 0.239, Rexp = 0.213, RBragg = 0.079, χ2 = 1.573 | Rp = 0.035, Rwp = 0.045, Rexp = 0.026, RBragg = 0.025, χ2 = 8.804 | Rp = 0.059, Rwp = 0.077, Rexp = 0.058, RBragg = 0.042, χ2 = 3.082 | Rp = 0.036, Rwp = 0.045, Rexp = 0.027, RBragg = 0.021, χ2 = 6.965 |
No. of data points | 3030 | 3901 | 3895 | 4061 |
No. of parameters | 40 | 40 | 30 | 30 |
(LSCT50_SXRD) | (LSCT50_NPD) | |
Crystal data | ||
Chemical formula | CoLa1.5O6Sr0.5Ti | CoLa1.5O6Sr0.5Ti |
Mr | 455.00 | 455.00 |
Crystal system, space group | Orthorhombic, Pnma | Orthorhombic, Pnma |
Temperature (K) | 295 | 295 |
a, b, c (Å) | 5.49186 (7), 7.77013 (10), 5.53014 (7) | 5.49186 (7), 7.77013 (10), 5.53014 (7) |
α, β, γ (°) | 90, 90, 90 | 90, 90, 90 |
V (Å3) | 235.99 (1) | 235.99 (1) |
Z | 2 | 2 |
Radiation type | Synchrotron, λ = 0.621000 Å | Constant Wavelength Neutron Diffraction, λ = 1.594000 Å |
µ (mm−1) | 8.31 | 0.00 |
Specimen shape, size (mm) | Cylinder, 15 × 20 | Cylinder, 15 × 20 |
Data collection | ||
Diffractometer | Home-made heavy-duty Theta-2theta goniometer diffractometer | High-resolution two-axis diffractometer |
Specimen mounting | Borosilicate 0.3 mm capillary | 'vanadium can' |
Data collection mode | Transmission | Transmission |
Scan method | Step | Step |
Absorption correction | – | – |
2θ values (°) | 2θmin = 8.069 2θmax = 47.009 2θstep = 0.010 | 2θmin = 0.270 2θmax = 160.229 2θstep = 0.050 |
Refinement | ||
R factors and goodness of fit | Rp = 0.070, Rwp = 0.089, Rexp = 0.059, RBragg = 0.058, χ2 = 5.045 | Rp = 0.030, Rwp = 0.040, Rexp = 0.016, RBragg = 0.027, χ2 = 41.290 |
No. of data points | 3895 | 3895 |
No. of parameters | 34 | 34 |
Computer programs: FULLPROF.
Symmetry-adapted Rietveld refinement is a powerfull tool to understand the physical mechanism which stabilize a certain structured derived from a high simmetry parent structure within displazative-type phase transitions.