Download citation
Download citation
link to html
The ability to perform neutron diffraction studies at simultaneous high pressures and high temperatures is a relatively recent development. The suitability of this technique for determining P–VT equations of state has been investigated by measuring the lattice parameters of Mg1−xFexO (x = 0.2, 0.3, 0.4), in the range P < 10.3 GPa and 300 < T < 986 K, by time-of-flight neutron powder diffraction. Pressures were determined using metallic Fe as a marker and temperatures were measured by neutron absorption resonance radiography. Within the resolution of the experiment, no evidence was found for any change in the temperature derivative of the isothermal incompressibility, ∂KT/∂T, with composition. By assuming that the equation-of-state parameters either varied linearly or were invariant with composition, the 60 measured state points were fitted simultaneously to a P–VTx equation of state, leading to values of ∂KT/∂T = −0.024 (9) GPa K−1 and of the isothermal Anderson–Grüneisen parameter δT = 4.0 (16) at 300 K. Two designs of simultaneous high-P/T cell were employed during this study. It appears that, by virtue of its extended pressure range, a design using toroidal gaskets is more suitable for equation-of-state studies than is the system described by Le Godec, Dove, Francis, Kohn, Marshall, Pawley, Price, Redfern, Rhodes, Ross, Schofield, Schooneveld, Syfosse, Tucker & Welch [Mineral. Mag. (2001), 65, 737–748].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0021889808025417/ks5172sup1.cif
Contains datablocks PRL42703_publ, PRL47388_ZRO2_publ, PRL42703_phase_1, PRL42703_phase_2, PRL47388_ZRO2_phase_1, PRL47388_ZRO2_phase_2, PRL47388_ZRO2_phase_3, PRL42703_p_01, PRL47388_ZRO2_p_01, PRL42703_overall, PRL47388_ZRO2_overall

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889808025417/ks5172PRL42703_p_01sup2.rtv
Contains datablock PRL42703_p_01

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0021889808025417/ks5172PRL42703_p_01sup3.hkl
Contains datablock PRL42703_p_01

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889808025417/ks5172PRL47388_ZRO2_p_01sup4.rtv
Contains datablock PRL47388_ZRO2_p_01

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0021889808025417/ks5172PRL47388_ZRO2_p_01sup5.hkl
Contains datablock PRL47388_ZRO2_p_01

zip

Zip compressed file https://doi.org/10.1107/S0021889808025417/ks5172sup6.zip
Supplementary data for Mg0.8Fe0.2O, Mg0.7Fe0.3O and Mg0.6Fe0.4O

Computing details top

Figures top
[Figure 1]
[Figure 2]
(PRL42703_phase_1) top
Crystal data top
Fe0.20Mg0.80OV = 74.07 Å3
Mr = 46.62Z = 4
Cubic, Fm3m? radiation, λ = ? Å
a = 4.19971 (13) Å?, ? × ? × ? mm
Data collection top
Refinement top
Least-squares matrix: full2524 data points
Rp = 0.283Profile function: TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 47.4 #6 (sig-2) = 9.9 #7 (gam-0) = 0.00 #8 (gam-1) = 9.53 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 14 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 73.3 #6 (sig-2) = 8.9 #7 (gam-0) = 0.00 #8 (gam-1) = 5.71 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0
Rwp = 0.13612 parameters
Rexp = 0.0920 restraints
R(F2) = 0.15908(Δ/σ)max = 0.29
χ2 = 2.190Background function: GSAS Background function number 1 with 4 terms. Shifted Chebyshev function of 1st kind 1: 0.238471 2: -2.329730E-02 3: 8.919900E-02 4: -5.781030E-02
Crystal data top
Fe0.20Mg0.80OV = 74.07 Å3
Mr = 46.62Z = 4
Cubic, Fm3m? radiation, λ = ? Å
a = 4.19971 (13) Å?, ? × ? × ? mm
Data collection top
Refinement top
Rp = 0.2832524 data points
Rwp = 0.13612 parameters
Rexp = 0.0920 restraints
R(F2) = 0.15908(Δ/σ)max = 0.29
χ2 = 2.190
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Mg0.00.00.00.0101 (11)*0.8
Fe0.00.00.00.0060 (3)*0.2
O0.50.50.50.0072 (5)*
(PRL42703_phase_2) top
Crystal data top
FeV = 22.92 Å3
Mr = 55.85Z = 2
Cubic, Im3m? radiation, λ = ? Å
a = 2.8403 (3) Å?, ? × ? × ? mm
Data collection top
Refinement top
Least-squares matrix: full2524 data points
Rp = 0.283Profile function: TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 47.4 #6 (sig-2) = 9.9 #7 (gam-0) = 0.00 #8 (gam-1) = 9.53 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 14 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 73.3 #6 (sig-2) = 8.9 #7 (gam-0) = 0.00 #8 (gam-1) = 5.71 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0
Rwp = 0.13612 parameters
Rexp = 0.0920 restraints
R(F2) = 0.15908(Δ/σ)max = 0.29
χ2 = 2.190Background function: GSAS Background function number 1 with 4 terms. Shifted Chebyshev function of 1st kind 1: 0.238471 2: -2.329730E-02 3: 8.919900E-02 4: -5.781030E-02
Crystal data top
FeV = 22.92 Å3
Mr = 55.85Z = 2
Cubic, Im3m? radiation, λ = ? Å
a = 2.8403 (3) Å?, ? × ? × ? mm
Data collection top
Refinement top
Rp = 0.2832524 data points
Rwp = 0.13612 parameters
Rexp = 0.0920 restraints
R(F2) = 0.15908(Δ/σ)max = 0.29
χ2 = 2.190
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
FE10.00.00.00.0081 (13)*
(PRL47388_ZRO2_phase_1) top
Crystal data top
Fe0.30Mg0.70OV = 73.54 Å3
Mr = 49.77Z = 4
Cubic, Fm3m? radiation, λ = ? Å
a = 4.1896 (2) Å?, ? × ? × ? mm
Data collection top
Refinement top
Least-squares matrix: full2524 data points
Rp = 0.083Profile function: TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 203.9 #6 (sig-2) = -16.0 #7 (gam-0) = 0.00 #8 (gam-1) = 31.42 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 104.6 #6 (sig-2) = -34.9 #7 (gam-0) = 0.00 #8 (gam-1) = 25.65 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 14 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2248 #2 (bet-0) = 0.026918 #3 (bet-1) = 0.029309 #4 (sig-0) = 0.0 #5 (sig-1) = 71.8 #6 (sig-2) = 8.3 #7 (gam-0) = 0.00 #8 (gam-1) = 6.00 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0
Rwp = 0.08319 parameters
Rexp = 0.0480 restraints
R(F2) = 0.38423(Δ/σ)max = 0.46
χ2 = 2.993Background function: GSAS Background function number 2 with 8 terms. Cosine Fourier series 1: -13.9330 2: 27.0721 3: -21.7005 4: 15.3369 5: -8.91545 6: 4.30403 7: -1.50325 8: 0.342467
Crystal data top
Fe0.30Mg0.70OV = 73.54 Å3
Mr = 49.77Z = 4
Cubic, Fm3m? radiation, λ = ? Å
a = 4.1896 (2) Å?, ? × ? × ? mm
Data collection top
Refinement top
Rp = 0.0832524 data points
Rwp = 0.08319 parameters
Rexp = 0.0480 restraints
R(F2) = 0.38423(Δ/σ)max = 0.46
χ2 = 2.993
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Mg0.00.00.00.0072 (13)*0.7
Fe0.00.00.00.0072 (13)*0.3
O0.50.50.50.0086 (16)*
(PRL47388_ZRO2_phase_2) top
Crystal data top
FeV = 22.60 Å3
Mr = 55.85Z = 2
Cubic, Im3m? radiation, λ = ? Å
a = 2.8274 (4) Å?, ? × ? × ? mm
Data collection top
Refinement top
Least-squares matrix: full2524 data points
Rp = 0.083Profile function: TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 203.9 #6 (sig-2) = -16.0 #7 (gam-0) = 0.00 #8 (gam-1) = 31.42 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 104.6 #6 (sig-2) = -34.9 #7 (gam-0) = 0.00 #8 (gam-1) = 25.65 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 14 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2248 #2 (bet-0) = 0.026918 #3 (bet-1) = 0.029309 #4 (sig-0) = 0.0 #5 (sig-1) = 71.8 #6 (sig-2) = 8.3 #7 (gam-0) = 0.00 #8 (gam-1) = 6.00 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0
Rwp = 0.08319 parameters
Rexp = 0.0480 restraints
R(F2) = 0.38423(Δ/σ)max = 0.46
χ2 = 2.993Background function: GSAS Background function number 2 with 8 terms. Cosine Fourier series 1: -13.9330 2: 27.0721 3: -21.7005 4: 15.3369 5: -8.91545 6: 4.30403 7: -1.50325 8: 0.342467
Crystal data top
FeV = 22.60 Å3
Mr = 55.85Z = 2
Cubic, Im3m? radiation, λ = ? Å
a = 2.8274 (4) Å?, ? × ? × ? mm
Data collection top
Refinement top
Rp = 0.0832524 data points
Rwp = 0.08319 parameters
Rexp = 0.0480 restraints
R(F2) = 0.38423(Δ/σ)max = 0.46
χ2 = 2.993
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
FE10.00.00.00.005*
(PRL47388_ZRO2_phase_3) top
Crystal data top
O2Zrβ = 100.16 (9)°
Mr = 123.22V = 135.53 Å3
Monoclinic, P21/cZ = 4
a = 5.213 (5) Å? radiation, λ = ? Å
b = 4.967 (6) Å?, ? × ? × ? mm
c = 5.318 (5) Å
Data collection top
Refinement top
Least-squares matrix: full2524 data points
Rp = 0.083Profile function: TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 203.9 #6 (sig-2) = -16.0 #7 (gam-0) = 0.00 #8 (gam-1) = 31.42 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 21 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2342 #2 (bet-0) = 0.025207 #3 (bet-1) = 0.028487 #4 (sig-0) = 0.0 #5 (sig-1) = 104.6 #6 (sig-2) = -34.9 #7 (gam-0) = 0.00 #8 (gam-1) = 25.65 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0, TOF Profile function number 3 with 14 terms Profile coefficients for exponential pseudovoigt convolution Von Dreele, 1990 (unpublished) #1 (alp ) = 0.2248 #2 (bet-0) = 0.026918 #3 (bet-1) = 0.029309 #4 (sig-0) = 0.0 #5 (sig-1) = 71.8 #6 (sig-2) = 8.3 #7 (gam-0) = 0.00 #8 (gam-1) = 6.00 #9 (gam-2) = 0.00 #10(gsf ) = 0.00 #11(g1ec ) = 0.00 #12(g2ec ) = 0.00 #13(rstr ) = 0.000 #14(rsta ) = 0.000 #15(rsca ) = 0.000 #16(L11) = 0.000 #17(L22) = 0.000 #18(L33) = 0.000 #19(L12) = 0.000 #20(L13) = 0.000 #21(L23) = 0.000 Peak tails are ignored where the intensity is below 0.0010 times the peak Aniso. broadening axis 0.0 0.0 1.0
Rwp = 0.08319 parameters
Rexp = 0.0480 restraints
R(F2) = 0.38423(Δ/σ)max = 0.46
χ2 = 2.993Background function: GSAS Background function number 2 with 8 terms. Cosine Fourier series 1: -13.9330 2: 27.0721 3: -21.7005 4: 15.3369 5: -8.91545 6: 4.30403 7: -1.50325 8: 0.342467
Crystal data top
O2Zrβ = 100.16 (9)°
Mr = 123.22V = 135.53 Å3
Monoclinic, P21/cZ = 4
a = 5.213 (5) Å? radiation, λ = ? Å
b = 4.967 (6) Å?, ? × ? × ? mm
c = 5.318 (5) Å
Data collection top
Refinement top
Rp = 0.0832524 data points
Rwp = 0.08319 parameters
Rexp = 0.0480 restraints
R(F2) = 0.38423(Δ/σ)max = 0.46
χ2 = 2.993
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
ZR10.27580.04110.20820.01*
O20.07030.33590.34060.01*
O30.44230.75490.47890.01*

Experimental details

(PRL42703_phase_1)(PRL42703_phase_2)(PRL47388_ZRO2_phase_1)(PRL47388_ZRO2_phase_2)
Crystal data
Chemical formulaFe0.20Mg0.80OFeFe0.30Mg0.70OFe
Mr46.6255.8549.7755.85
Crystal system, space groupCubic, Fm3mCubic, Im3mCubic, Fm3mCubic, Im3m
Temperature (K)????
a, b, c (Å)4.19971 (13), 4.19971, 4.199712.8403 (3), 2.84034, 2.840344.1896 (2), 4.18955, 4.189552.8274 (4), 2.8274, 2.8274
α, β, γ (°)90, 90, 9090, 90, 9090, 90, 9090, 90, 90
V3)74.0722.9273.5422.60
Z4242
Radiation type?, λ = ? Å?, λ = ? Å?, λ = ? Å?, λ = ? Å
Specimen shape, size (mm)?, ? × ? × ??, ? × ? × ??, ? × ? × ??, ? × ? × ?
Data collection
Diffractometer????
Specimen mounting????
Data collection mode????
Scan method????
2θ values (°)2θmin = ? 2θmax = ? 2θstep = ?2θmin = ? 2θmax = ? 2θstep = ?2θmin = ? 2θmax = ? 2θstep = ?2θmin = ? 2θmax = ? 2θstep = ?
Refinement
R factors and goodness of fitRp = 0.283, Rwp = 0.136, Rexp = 0.092, R(F2) = 0.15908, χ2 = 2.190Rp = 0.283, Rwp = 0.136, Rexp = 0.092, R(F2) = 0.15908, χ2 = 2.190Rp = 0.083, Rwp = 0.083, Rexp = 0.048, R(F2) = 0.38423, χ2 = 2.993Rp = 0.083, Rwp = 0.083, Rexp = 0.048, R(F2) = 0.38423, χ2 = 2.993
No. of data points2524252425242524
No. of parameters12121919
(Δ/σ)max0.290.290.460.46


(PRL47388_ZRO2_phase_3)
Crystal data
Chemical formulaO2Zr
Mr123.22
Crystal system, space groupMonoclinic, P21/c
Temperature (K)?
a, b, c (Å)5.213 (5), 4.967 (6), 5.318 (5)
α, β, γ (°)90, 100.16 (9), 90
V3)135.53
Z4
Radiation type?, λ = ? Å
Specimen shape, size (mm)?, ? × ? × ?
Data collection
Diffractometer?
Specimen mounting?
Data collection mode?
Scan method?
2θ values (°)2θmin = ? 2θmax = ? 2θstep = ?
Refinement
R factors and goodness of fitRp = 0.083, Rwp = 0.083, Rexp = 0.048, R(F2) = 0.38423, χ2 = 2.993
No. of data points2524
No. of parameters19
(Δ/σ)max0.46

Computer programs: GSAS.

 

Follow J. Appl. Cryst.
Sign up for e-alerts
Follow J. Appl. Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds