A detailed analysis of correlations between structural features and cation conductivity is performed for KAlO2 polymorphs in a wide temperature range of 300-1023 K. To explore the migration maps of K+ cations we have used neutron diffraction data for low- and high-temperature KAlO2 polymorphs and applied for the first time a novel algorithm based on the natural tiling concept and implemented it into the program package TOPOS. Five independent elementary channels for the K+ cation migration have been revealed whose cross-sections were found to be essentially different in the low-temperature form, indicating a high anisotropy of the cation conductivity. During the transition to the cubic high-temperature phase all five channels become equivalent with sharply increased cross-sections that account for the jump-like increase of the cation conductivity and gives rise to its three-dimensional character.
Supporting information
For all compounds, program(s) used to refine structure: FULLPROF.
Crystal data top
Al2O4·2(K) | c = 15.4564 (4) Å |
Mr = 196.16 | V = 918.26 (5) Å3 |
Orthorhombic, PBCA | Z = 8 |
Hall symbol: -P 2ac 2ab | Dx = 2.838 Mg m−3 |
a = 5.43867 (18) Å | Neutron radiation |
b = 10.9236 (3) Å | T = 300 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.529°, 2θmax = 164.629°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 1.263 | Profile function: pseudo-Voigt |
Rwp = 1.725 | 68 parameters |
Rexp = 1.251 | 0 restraints |
RBragg = 2.490 | Background function: linear interpolation |
1602 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Al1 | 0.2590 (10) | 0.0104 (5) | 0.1866 (7) | 0.0059 (5)* | |
Al2 | 0.2811 (8) | 0.2601 (5) | 0.0656 (5) | 0.0059 (5)* | |
K1 | 0.7534 (11) | 0.0067 (6) | 0.0611 (7) | 0.021 (5) | |
K2 | 0.7916 (10) | 0.2592 (5) | 0.1863 (5) | 0.014 (4) | |
O1 | 0.5673 (7) | 0.2848 (4) | 0.0162 (2) | 0.018 (2) | |
O2 | 0.1777 (7) | 0.4023 (3) | 0.10588 (19) | 0.0089 (19) | |
O3 | 0.2965 (6) | 0.1555 (3) | 0.1479 (2) | 0.0164 (18) | |
O4 | 0.0526 (7) | 0.4856 (3) | 0.2776 (3) | 0.012 (2) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
K1 | 0.020 (4) | 0.018 (4) | 0.026 (6) | 0.00000 | 0.015 (4) | 0.00000 |
K2 | 0.019 (3) | 0.014 (3) | 0.010 (5) | 0.00000 | −0.002 (3) | 0.00000 |
O1 | 0.0104 (18) | 0.029 (2) | 0.014 (2) | 0.00000 | 0.0093 (15) | 0.00000 |
O2 | 0.014 (2) | 0.0086 (18) | 0.0037 (19) | 0.00000 | −0.0033 (13) | 0.00000 |
O3 | 0.0044 (5) | 0.018 (2) | 0.027 (3) | 0.00000 | −0.0046 (16) | 0.00000 |
O4 | 0.0103 (19) | 0.012 (2) | 0.015 (2) | 0.00000 | −0.0071 (17) | 0.00000 |
Geometric parameters (Å, º) top
Al1—O2i | 1.752 (9) | K1—O2v | 2.796 (11) |
Al1—O3 | 1.706 (7) | K1—O2i | 2.698 (7) |
Al1—O4ii | 1.803 (7) | K1—O4vi | 2.717 (11) |
Al1—O4i | 1.761 (10) | K2—O1 | 2.912 (8) |
Al2—O1 | 1.755 (6) | K2—O2vii | 2.898 (7) |
Al2—O1iii | 1.786 (7) | K2—O3 | 2.981 (6) |
Al2—O2 | 1.765 (7) | K2—O3viii | 2.802 (8) |
Al2—O3 | 1.712 (8) | K2—O4viii | 2.849 (7) |
K1—O1iv | 2.703 (8) | | |
| | | |
O2—Al1—O3 | 110.668 | O1viii—Al2—O1 | 108.160 |
O2—Al1—O4 | 107.574 | O1viii—Al2—O2 | 107.502 |
O2—Al1—O4 | 110.532 | O1viii—Al2—O3 | 103.672 |
O3—Al1—O4 | 111.067 | O1—Al2—O2 | 106.489 |
O3—Al1—O4 | 110.690 | O1—Al2—O3 | 111.993 |
O4—Al1—O4 | 106.177 | O2—Al2—O3 | 109.926 |
Symmetry codes: (i) −x+1/2, y−1/2, z; (ii) −x, y−1/2, −z+1/2; (iii) x−1/2, −y+1/2, −z; (iv) −x+3/2, y−1/2, z; (v) x+1/2, −y+1/2, −z; (vi) −x+1, y−1/2, −z+1/2; (vii) x+1, y, z; (viii) x+1/2, y, −z+1/2. |
Crystal data top
Al2O4·2(K) | c = 15.4698 (9) Å |
Mr = 196.16 | V = 921.64 (10) Å3 |
Orthorhombic, PBCA | Z = 8 |
Hall symbol: -P 2ac 2ab | Dx = 2.827 Mg m−3 |
a = 5.4457 (3) Å | Neutron radiation |
b = 10.9401 (7) Å | T = 400 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.531°, 2θmax = 164.831°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 4.444 | Profile function: pseudo-Voigt |
Rwp = 5.756 | 70 parameters |
Rexp = 4.851 | 0 restraints |
RBragg = 3.196 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Al1 | 0.2579 (18) | 0.0116 (9) | 0.1864 (11) | 0.0069 (10)* | |
Al2 | 0.2791 (14) | 0.2596 (9) | 0.0661 (9) | 0.0069 (10)* | |
K1 | 0.752 (2) | 0.0065 (10) | 0.0625 (12) | 0.024 (9) | |
K2 | 0.7901 (18) | 0.2596 (9) | 0.1875 (10) | 0.021 (7) | |
O1 | 0.5651 (13) | 0.2827 (7) | 0.0165 (4) | 0.021 (4) | |
O2 | 0.1799 (14) | 0.4013 (6) | 0.1066 (3) | 0.011 (3) | |
O3 | 0.2965 (12) | 0.1549 (7) | 0.1477 (4) | 0.020 (3) | |
O4 | 0.0527 (14) | 0.4851 (6) | 0.2775 (5) | 0.014 (4) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
K1 | 0.027 (9) | 0.010 (8) | 0.034 (12) | 0.00000 | 0.018 (8) | 0.00000 |
K2 | 0.023 (6) | 0.025 (7) | 0.016 (9) | 0.00000 | 0.006 (5) | 0.00000 |
O1 | 0.013 (3) | 0.028 (4) | 0.020 (4) | 0.00000 | 0.008 (3) | 0.00000 |
O2 | 0.020 (4) | 0.008 (3) | 0.006 (3) | 0.00000 | −0.005 (2) | 0.00000 |
O3 | 0.0081 (11) | 0.033 (4) | 0.021 (5) | 0.00000 | −0.003 (3) | 0.00000 |
O4 | 0.007 (3) | 0.022 (5) | 0.015 (4) | 0.00000 | −0.002 (3) | 0.00000 |
Geometric parameters (Å, º) top
Al1—O2i | 1.759 (15) | K1—O2v | 2.831 (18) |
Al1—O3 | 1.691 (13) | K1—O2i | 2.706 (14) |
Al1—O4ii | 1.805 (13) | K1—O4vi | 2.704 (19) |
Al1—O4i | 1.770 (17) | K2—O1 | 2.926 (16) |
Al2—O1 | 1.755 (12) | K2—O2vii | 2.911 (13) |
Al2—O1iii | 1.790 (13) | K2—O3 | 2.986 (12) |
Al2—O2 | 1.757 (12) | K2—O3viii | 2.795 (16) |
Al2—O3 | 1.707 (14) | K2—O4viii | 2.837 (12) |
K1—O1iv | 2.737 (14) | | |
| | | |
O2—Al1—O3 | 111.315 | O1viii—Al2—O1 | 107.634 |
O2—Al1—O4 | 106.704 | O1viii—Al2—O2 | 107.564 |
O2—Al1—O4 | 109.519 | O1viii—Al2—O3 | 103.881 |
O3—Al1—O4 | 112.021 | O1—Al2—O2 | 106.405 |
O3—Al1—O4 | 111.173 | O1—Al2—O3 | 112.983 |
O4—Al1—O4 | 105.867 | O2—Al2—O3 | 110.203 |
Symmetry codes: (i) −x+1/2, y−1/2, z; (ii) −x, y−1/2, −z+1/2; (iii) x−1/2, −y+1/2, −z; (iv) −x+3/2, y−1/2, z; (v) x+1/2, −y+1/2, −z; (vi) −x+1, y−1/2, −z+1/2; (vii) x+1, y, z; (viii) x+1/2, y, −z+1/2. |
Crystal data top
Al2O4·2(K) | c = 15.4893 (12) Å |
Mr = 196.16 | V = 926.38 (12) Å3 |
Orthorhombic, PBCA | Z = 8 |
Hall symbol: -P 2ac 2ab | Dx = 2.813 Mg m−3 |
a = 5.4560 (4) Å | Neutron radiation |
b = 10.9617 (8) Å | T = 500 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.534°, 2θmax = 164.834°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 4.701 | Profile function: pseudo-Voigt |
Rwp = 6.056 | 70 parameters |
Rexp = 4.863 | 0 restraints |
RBragg = 3.861 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Al1 | 0.260 (2) | 0.0095 (11) | 0.1845 (11) | 0.0097 (12)* | |
Al2 | 0.2793 (16) | 0.2607 (10) | 0.0671 (10) | 0.0097 (12)* | |
K1 | 0.744 (2) | 0.0060 (11) | 0.0606 (14) | 0.029 (11) | |
K2 | 0.787 (2) | 0.2603 (10) | 0.1868 (12) | 0.025 (9) | |
O1 | 0.5661 (15) | 0.2814 (8) | 0.0161 (4) | 0.026 (4) | |
O2 | 0.1817 (15) | 0.4001 (7) | 0.1067 (4) | 0.015 (4) | |
O3 | 0.2935 (14) | 0.1529 (8) | 0.1464 (5) | 0.026 (4) | |
O4 | 0.0539 (16) | 0.4877 (7) | 0.2771 (6) | 0.023 (5) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
K1 | 0.026 (10) | 0.011 (9) | 0.051 (15) | 0.00000 | 0.020 (9) | 0.00000 |
K2 | 0.024 (7) | 0.024 (9) | 0.028 (11) | 0.00000 | −0.002 (6) | 0.00000 |
O1 | 0.021 (4) | 0.044 (5) | 0.012 (4) | 0.00000 | 0.012 (3) | 0.00000 |
O2 | 0.018 (4) | 0.009 (4) | 0.019 (4) | 0.00000 | −0.002 (3) | 0.00000 |
O3 | 0.0081 (13) | 0.033 (5) | 0.038 (6) | 0.00000 | −0.002 (3) | 0.00000 |
O4 | 0.006 (4) | 0.042 (7) | 0.022 (5) | 0.00000 | −0.004 (4) | 0.00000 |
Geometric parameters (Å, º) top
Al1—O2i | 1.730 (16) | K1—O1iv | 2.759 (15) |
Al1—O3 | 1.689 (15) | K1—O2v | 2.81 (2) |
Al1—O4ii | 1.829 (15) | K1—O2i | 2.693 (15) |
Al1—O4i | 1.774 (18) | K1—O4vi | 2.75 (2) |
Al2—O1 | 1.768 (13) | K2—O1 | 2.915 (19) |
Al2—O1iii | 1.796 (15) | K2—O2vii | 2.920 (15) |
Al2—O2 | 1.731 (14) | K2—O3viii | 2.839 (19) |
Al2—O3 | 1.706 (16) | K2—O4viii | 2.854 (14) |
| | | |
O2—Al1—O3 | 112.454 | O1viii—Al2—O1 | 106.596 |
O2—Al1—O4 | 107.954 | O1viii—Al2—O2 | 108.510 |
O2—Al1—O4 | 111.393 | O1viii—Al2—O3 | 109.870 |
O3—Al1—O4 | 109.671 | O1—Al2—O2 | 106.372 |
O3—Al1—O4 | 107.613 | O1—Al2—O3 | 111.744 |
O4—Al1—O4 | 110.245 | O2—Al2—O3 | 111.589 |
Symmetry codes: (i) −x+1/2, y−1/2, z; (ii) −x, y−1/2, −z+1/2; (iii) x−1/2, −y+1/2, −z; (iv) −x+3/2, y−1/2, z; (v) x+1/2, −y+1/2, −z; (vi) −x+1, y−1/2, −z+1/2; (vii) x+1, y, z; (viii) x+1/2, y, −z+1/2. |
Crystal data top
Al2O4·2(K) | c = 15.5103 (14) Å |
Mr = 196.16 | V = 931.53 (14) Å3 |
Orthorhombic, PBCA | Z = 8 |
Hall symbol: -P 2ac 2ab | Dx = 2.797 Mg m−3 |
a = 5.4668 (4) Å | Neutron radiation |
b = 10.9862 (9) Å | T = 600 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.542°, 2θmax = 164.842°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 4.565 | Profile function: pseudo-Voigt |
Rwp = 5.776 | 70 parameters |
Rexp = 4.869 | 0 restraints |
RBragg = 4.455 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Al1 | 0.256 (2) | 0.0108 (11) | 0.1870 (11) | 0.0127 (12)* | |
Al2 | 0.2795 (17) | 0.2589 (11) | 0.0656 (11) | 0.0127 (12)* | |
K1 | 0.749 (3) | 0.0050 (12) | 0.0635 (15) | 0.037 (13) | |
K2 | 0.782 (2) | 0.2574 (11) | 0.1888 (13) | 0.033 (10) | |
O1 | 0.5636 (16) | 0.2803 (9) | 0.0158 (5) | 0.032 (5) | |
O2 | 0.1885 (16) | 0.3986 (7) | 0.1076 (5) | 0.020 (4) | |
O3 | 0.2938 (15) | 0.1508 (9) | 0.1450 (6) | 0.037 (5) | |
O4 | 0.0510 (17) | 0.4873 (8) | 0.2767 (7) | 0.031 (6) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
K1 | 0.037 (12) | 0.017 (10) | 0.057 (17) | 0.00000 | 0.023 (12) | 0.00000 |
K2 | 0.021 (8) | 0.034 (10) | 0.043 (14) | 0.00000 | −0.001 (6) | 0.00000 |
O1 | 0.022 (4) | 0.051 (6) | 0.022 (5) | 0.00000 | 0.003 (4) | 0.00000 |
O2 | 0.027 (5) | 0.003 (4) | 0.029 (5) | 0.00000 | −0.004 (3) | 0.00000 |
O3 | 0.0132 (15) | 0.053 (6) | 0.044 (7) | 0.00000 | −0.006 (4) | 0.00000 |
O4 | 0.006 (4) | 0.062 (9) | 0.024 (5) | 0.00000 | −0.004 (4) | 0.00000 |
Geometric parameters (Å, º) top
Al1—O2i | 1.769 (17) | K1—O2v | 2.88 (2) |
Al1—O3 | 1.683 (16) | K1—O2i | 2.749 (18) |
Al1—O4ii | 1.789 (15) | K1—O4vi | 2.72 (2) |
Al1—O4i | 1.765 (18) | K2—O1 | 2.95 (2) |
Al2—O1 | 1.750 (14) | K2—O2vii | 2.988 (16) |
Al2—O1iii | 1.781 (16) | K2—O3 | 2.993 (15) |
Al2—O2 | 1.740 (15) | K2—O3viii | 2.83 (2) |
Al2—O3 | 1.713 (18) | K2—O4viii | 2.874 (15) |
K1—O1iv | 2.773 (17) | | |
| | | |
O2—Al1—O3 | 110.263 | O1viii—Al2—O1 | 107.917 |
O2—Al1—O4 | 106.230 | O1viii—Al2—O2 | 107.483 |
O2—Al1—O4 | 110.142 | O1viii—Al2—O3 | 109.870 |
O3—Al1—O4 | 111.647 | O1—Al2—O2 | 106.810 |
O3—Al1—O4 | 111.429 | O1—Al2—O3 | 111.712 |
O4—Al1—O4 | 106.954 | O2—Al2—O3 | 111.857 |
Symmetry codes: (i) −x+1/2, y−1/2, z; (ii) −x, y−1/2, −z+1/2; (iii) x−1/2, −y+1/2, −z; (iv) −x+3/2, y−1/2, z; (v) x+1/2, −y+1/2, −z; (vi) −x+1, y−1/2, −z+1/2; (vii) x+1, y, z; (viii) x+1/2, y, −z+1/2. |
Crystal data top
Al2O4·2(K) | c = 15.5359 (18) Å |
Mr = 196.16 | V = 937.35 (17) Å3 |
Orthorhombic, PBCA | Z = 8 |
Hall symbol: -P 2ac 2ab | Dx = 2.780 Mg m−3 |
a = 5.4788 (5) Å | Neutron radiation |
b = 11.0123 (11) Å | T = 700 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.547°, 2θmax = 164.847°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 4.701 | Profile function: pseudo-Voigt |
Rwp = 5.915 | 70 parameters |
Rexp = 4.863 | 0 restraints |
RBragg = 5.940 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Al1 | 0.255 (2) | 0.0106 (14) | 0.1849 (12) | 0.0164 (13)* | |
Al2 | 0.2783 (19) | 0.2600 (12) | 0.0632 (12) | 0.0164 (13)* | |
K1 | 0.749 (3) | 0.0045 (15) | 0.067 (2) | 0.054 (12) | |
K2 | 0.774 (2) | 0.2593 (12) | 0.1897 (14) | 0.030 (8) | |
O1 | 0.5622 (19) | 0.2773 (11) | 0.0163 (6) | 0.042 (5) | |
O2 | 0.1872 (18) | 0.3957 (9) | 0.1095 (6) | 0.029 (4) | |
O3 | 0.2938 (16) | 0.1493 (10) | 0.1444 (7) | 0.042 (6) | |
O4 | 0.048 (2) | 0.4878 (10) | 0.2750 (9) | 0.043 (8) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
K1 | 0.022 (5) | 0.031 (6) | 0.11 (2) | 0.00000 | 0.024 (14) | 0.00000 |
K2 | 0.022 (5) | 0.031 (6) | 0.038 (13) | 0.00000 | −0.010 (6) | 0.00000 |
O1 | 0.028 (4) | 0.074 (8) | 0.025 (6) | 0.00000 | 0.0003 (4) | 0.00000 |
O2 | 0.0053 (11) | 0.021 (5) | 0.061 (7) | 0.00000 | −0.006 (5) | 0.00000 |
O3 | 0.0138 (17) | 0.056 (7) | 0.057 (8) | 0.00000 | −0.008 (5) | 0.00000 |
O4 | 0.021 (5) | 0.068 (10) | 0.040 (8) | 0.00000 | 0.013 (5) | 0.00000 |
Geometric parameters (Å, º) top
Al1—O2i | 1.753 (19) | K1—O2v | 2.98 (3) |
Al1—O3 | 1.666 (19) | K1—O2i | 2.75 (2) |
Al1—O4ii | 1.791 (17) | K1—O4vi | 2.70 (3) |
Al1—O4i | 1.79 (2) | K2—O1 | 2.94 (2) |
Al2—O1 | 1.728 (16) | K2—O2vii | 2.991 (17) |
Al2—O1iii | 1.760 (18) | K2—O3 | 2.978 (15) |
Al2—O2 | 1.732 (17) | K2—O3viii | 2.85 (2) |
Al2—O3 | 1.76 (2) | K2—O4viii | 2.856 (17) |
K1—O1iv | 2.82 (2) | | |
| | | |
O2—Al1—O3 | 112.731 | O1viii—Al2—O1 | 109.597 |
O2—Al1—O4 | 107.380 | O1viii—Al2—O2 | 108.421 |
O2—Al1—O4 | 108.251 | O1viii—Al2—O3 | 109.623 |
O3—Al1—O4 | 112.229 | O1—Al2—O2 | 107.400 |
O3—Al1—O4 | 110.365 | O1—Al2—O3 | 112.005 |
O4—Al1—O4 | 105.542 | O2—Al2—O3 | 108.331 |
Symmetry codes: (i) −x+1/2, y−1/2, z; (ii) −x, y−1/2, −z+1/2; (iii) x−1/2, −y+1/2, −z; (iv) −x+3/2, y−1/2, z; (v) x+1/2, −y+1/2, −z; (vi) −x+1, y−1/2, −z+1/2; (vii) x+1, y, z; (viii) x+1/2, y, −z+1/2. |
Crystal data top
Al2O4·2(K) | c = 15.5598 (5) Å |
Mr = 196.16 | V = 942.40 (6) Å3 |
Orthorhombic, PBCA | Z = 8 |
Hall symbol: -P 2ac 2ab | Dx = 2.765 Mg m−3 |
a = 5.4888 (2) Å | Neutron radiation |
b = 11.0346 (4) Å | T = 773 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.538°, 2θmax = 164.838°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 2.984 | Profile function: pseudo-Voigt |
Rwp = 3.859 | 66 parameters |
Rexp = 1.577 | 0 restraints |
RBragg = 5.993 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Al1 | 0.249 (3) | 0.0060 (18) | 0.1853 (15) | 0.020 (4)* | |
Al2 | 0.272 (2) | 0.2554 (11) | 0.0647 (15) | 0.020 (4)* | |
K1 | 0.761 (6) | 0.0022 (19) | 0.0604 (19) | 0.07 (2) | |
K2 | 0.782 (3) | 0.2559 (14) | 0.1888 (16) | 0.050 (16) | |
O1 | 0.553 (2) | 0.2729 (14) | 0.0141 (7) | 0.070 (10) | |
O2 | 0.192 (3) | 0.3933 (13) | 0.1115 (8) | 0.063 (10) | |
O3 | 0.2922 (16) | 0.1482 (10) | 0.1417 (7) | 0.029 (6) | |
O4 | 0.045 (2) | 0.4910 (9) | 0.2758 (8) | 0.039 (7) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
K1 | 0.088 (19) | 0.09 (2) | 0.025 (17) | 0.00000 | −0.01103 | 0.00000 |
K2 | 0.042 (11) | 0.08 (2) | 0.025 (16) | 0.00000 | −0.001 (7) | 0.00000 |
O1 | 0.026 (6) | 0.128 (15) | 0.054 (9) | 0.00000 | 0.026 (5) | 0.00000 |
O2 | 0.105 (12) | 0.031 (8) | 0.052 (9) | 0.00000 | −0.004 (7) | 0.00000 |
O3 | 0.011 (4) | 0.027 (7) | 0.049 (7) | 0.00000 | 0.003 (5) | 0.00000 |
O4 | 0.018 (6) | 0.078 (10) | 0.022 (5) | 0.00000 | 0.005 (6) | 0.00000 |
Geometric parameters (Å, º) top
Al1—O2i | 1.72 (2) | K1—O2v | 3.33 (3) |
Al1—O3 | 1.72 (2) | K1—O3 | 3.29 (3) |
Al1—O4ii | 1.73 (2) | K1—O4vi | 2.77 (3) |
Al1—O4i | 1.82 (2) | K2—O1 | 3.00 (2) |
Al2—O1 | 1.743 (16) | K2—O2vii | 2.961 (17) |
Al2—O1iii | 1.745 (18) | K2—O2viii | 3.49 (2) |
Al2—O2 | 1.744 (16) | K2—O3 | 3.036 (16) |
Al2—O3 | 1.69 (2) | K2—O3vii | 3.124 (16) |
K1—O1 | 3.28 (2) | K2—O3viii | 2.89 (2) |
K1—O1iv | 3.17 (2) | K2—O4vii | 3.259 (17) |
K1—O1v | 2.82 (2) | K2—O4vi | 3.122 (16) |
K1—O2iv | 2.94 (3) | K2—O4viii | 2.958 (16) |
K1—O2i | 2.87 (3) | | |
| | | |
O2—Al1—O3 | 111.579 | O1viii—Al2—O1 | 108.178 |
O2—Al1—O4 | 109.951 | O1viii—Al2—O2 | 108.421 |
O2—Al1—O4 | 109.404 | O1viii—Al2—O3 | 109.870 |
O3—Al1—O4 | 110.626 | O1—Al2—O2 | 105.984 |
O3—Al1—O4 | 107.613 | O1—Al2—O3 | 114.750 |
O4—Al1—O4 | 107.548 | O2—Al2—O3 | 109.413 |
Symmetry codes: (i) −x+1/2, y−1/2, z; (ii) −x, y−1/2, −z+1/2; (iii) x−1/2, −y+1/2, −z; (iv) x+1/2, −y+1/2, −z; (v) −x+3/2, y−1/2, z; (vi) −x+1, y−1/2, −z+1/2; (vii) x+1, y, z; (viii) x+1/2, y, −z+1/2. |
Crystal data top
Al8O16·8(K) | V = 475.16 (7) Å3 |
Mr = 783.62 | Z = 1 |
Cubic, FD3M | Dx = 2.739 Mg m−3 |
Hall symbol: -F 4vw 2vw 3 | Neutron radiation |
a = 7.8033 (6) Å | T = 833 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.520°, 2θmax = 164.820°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 5.985 | Profile function: pseudo-Voigt |
Rwp = 7.808 | 26 parameters |
Rexp = 4.914 | 0 restraints |
RBragg = 11.546 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | Occ. (<1) |
Al1 | 0.12500 | 0.12500 | 0.12500 | 0.0272 (13)* | |
K1 | 0.37500 | 0.37500 | 0.37500 | 0.065 (2)* | |
O2 | 0.05 (2) | −0.04 (2) | −0.01 (7) | 0.037 (6)* | 0.08333 |
Geometric parameters (Å, º) top
Al1—O2 | 1.8 (3) | K1—O2ii | 2.8 (2) |
Al1—O2i | 1.8 (3) | K1—O2iii | 2.8 (2) |
| | | |
O2—Al1—O2i | 29 | | |
Symmetry codes: (i) z, x, y; (ii) x, −y+1/4, −z+1/4; (iii) −y+1/4, −z+1/4, x. |
Crystal data top
Al8O16·8(K) | V = 477.83 (5) Å3 |
Mr = 783.62 | Z = 1 |
Cubic, FD3M | Dx = 2.723 Mg m−3 |
Hall symbol: -F 4vw 2vw 3 | Neutron radiation |
a = 7.8179 (5) Å | T = 923 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.540°, 2θmax = 164.840°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 4.625 | Profile function: pseudo-Voigt |
Rwp = 6.153 | 32 parameters |
Rexp = 4.898 | 0 restraints |
RBragg = 3.186 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | Occ. (<1) |
Al1 | 0.12500 | 0.12500 | 0.12500 | 0.0293 (11)* | |
K1 | 0.37500 | 0.37500 | 0.37500 | 0.0677 (18)* | |
O2 | 0.036 (10) | −0.048 (4) | 0.01 (3) | 0.035 (5)* | 0.08333 |
Geometric parameters (Å, º) top
Al1—O2 | 1.77 (13) | K1—O2ii | 2.92 (11) |
Al1—O2i | 1.75 (15) | K1—O2iii | 2.9 (2) |
| | | |
O2—Al1—O2i | 31 | | |
Symmetry codes: (i) −x, −y, −z; (ii) x, −y+1/4, −z+1/4; (iii) −y+1/4, −z+1/4, x. |
Crystal data top
Al8O16·8(K) | V = 480.58 (4) Å3 |
Mr = 783.62 | Z = 1 |
Cubic, FD3M | Dx = 2.715 Mg m−3 |
Hall symbol: -F 4vw 2vw 3 | Neutron radiation |
a = 7.8329 (3) Å | T = 1023 K |
Data collection top
HPRT neutron diffractometer | 2θmin = 4.546°, 2θmax = 164.846°, 2θstep = 0.100° |
Radiation source: nuclear reactor | |
Refinement top
Rp = 2.564 | Profile function: pseudo-Voigt |
Rwp = 3.541 | 32 parameters |
Rexp = 1.611 | 0 restraints |
RBragg = 4.334 | Background function: linear interpolation |
1604 data points | |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Al1 | 0.12500 | 0.12500 | 0.12500 | 0.0486 (9)* | |
K1 | 0.37500 | 0.37500 | 0.37500 | 0.0921 (13)* | |
O2 | 0.00000 | 0.00000 | 0.00000 | 0.197 (6)* | |
Geometric parameters (Å, º) top
Al1—O2 | 1.6959 (1) | K1—O2i | 3.2474 (1) |
| | | |
O2—Al1—O2i | 109.471 | | |
Symmetry code: (i) x, −y+1/4, −z+1/4. |