The electron density distribution in α-spodumene, LiAl(SiO
3)
2, was derived from high-resolution X-ray diffraction experiments. The results obtained from both Mo
Kα- and Ag
Kα-wavelength data sets are reported. The features of the Si—O and Al—O bonds are related to the geometrical parameters of the Si—O—Al and Si—O—Si bridges on the one hand and to the O
Li
+ interaction on the other. Kappa refinements against the two data sets yielded almost the same net charges for the Si (+1.8 e) and O (−1.0 e) atoms in spodumene. However, the Al net charge obtained from the Ag
Kα data (+1.9 e) is larger than the net charge derived from the Mo
Kα data (+1.5 e). This difference correlates with a more contracted Al valence shell revealed by the shorter X-ray wavelength (κ = 1.4 for the Ag
Kα data set). The derived net charges were used to calculate the Madelung potential at the spodumene atomic sites. The electrostatic energy for the chemical formula LiAl(SiO
3)
2 was −8.60 e
2 Å
−1 (−123.84 eV) from the net charges derived from the Ag
Kα data and −6.97 e
2 Å
−1 (−100.37 eV) from the net charges derived from the Mo
Kα data.
Supporting information
| Structure factor file (CIF format) Contains datablock I |
| Structure factor file (CIF format) Contains datablock AgKa |
| Crystallographic Information File (CIF) Contains datablocks spod, I, II |
| Portable Document Format (PDF) file Supplementary material |
For both compounds, data collection: CAD-4 (Enraf-Nonius, 1989); cell refinement: CAD-4 (Enraf-Nonius, 1989); data reduction: DREADD (Blessing, 1987, 1989); program(s) used to refine structure: MOLLY (Hansen & Coppens, 1978).
Crystal data top
LiAl(SiO3)2 | F(000) = 368.0 |
Mr = 186.09 | Dx = 3.18 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.7107 Å |
a = 9.462 (1) Å | Cell parameters from 25 reflections |
b = 8.392 (1) Å | θ = 16.4–30.5° |
c = 5.221 (1) Å | µ = 1.05 mm−1 |
β = 110.18 (1)° | T = 293 K |
V = 389.12 (8) Å3 | Parallelepiped, colourless |
Z = 4 | 0.36 × 0.18 × 0.06 mm |
Data collection top
Enraf-Nonius CAD4 diffractometer | Rint = 0.021 |
ω/2θ scans | θmax = 60.1°, θmin = 3.3° |
Absorption correction: integration empirical (using intensity measurements) integration (ABSORB, G. de Titta, 1985)
and empirical (using intensity measurements) (DREADD, R. Blessing, 1995) | h = −22→22 |
Tmin = 0.68, Tmax = 0.95 | k = −18→20 |
12984 measured reflections | l = −12→11 |
2945 independent reflections | 3 standard reflections every 120 min |
2366 reflections with I > 3σ(I) | intensity decay: none |
Refinement top
Refinement on F | w = 1/[σ2(F2) + (0.0130F2)2] |
R[F2 > 2σ(F2)] = 0.014 | (Δ/σ)max < 0.001 |
wR(F2) = 0.015 | Δρmax = 0.3 e Å−3 |
S = 0.97 | Δρmin = −0.1 e Å−3 |
2366 reflections | Extinction correction: Becker-Coppens type 1 Lorentzian isotropic |
138 parameters | Extinction coefficient: 5.0x102 |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Si | 0.29410 (1) | 0.09347 (1) | 0.25592 (1) | 0.00377 (2) | |
Al | 0.00000 | 0.90667 (1) | 0.25000 | 0.00409 (2) | |
O1 | 0.10971 (2) | 0.08232 (2) | 0.14056 (4) | 0.00479 (4) | |
O2 | 0.36470 (2) | 0.26713 (2) | 0.30048 (4) | 0.00758 (5) | |
O3 | 0.35663 (2) | 0.98674 (3) | 0.05827 (4) | 0.00749 (5) | |
Li | 0.00000 | 0.27467 (13) | 0.25000 | 0.01464 (4) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Si | 0.00360 (2) | 0.00432 (2) | 0.00332 (2) | −0.00061 (2) | 0.00109 (2) | −0.00019 (2) |
Al | 0.00407 (3) | 0.00419 (3) | 0.00393 (3) | 0.00000 | 0.00126 (3) | 0.00000 |
O1 | 0.00368 (4) | 0.00563 (5) | 0.00463 (5) | −0.00036 (4) | 0.00090 (4) | 0.00013 (4) |
O2 | 0.00799 (6) | 0.00560 (5) | 0.00983 (6) | −0.00293 (4) | 0.00393 (5) | −0.00098 (5) |
O3 | 0.00572 (5) | 0.01129 (6) | 0.00508 (5) | 0.00067 (5) | 0.00139 (4) | −0.00337 (5) |
Li | 0.0146 (4) | 0.0139 (4) | 0.0159 (4) | 0.00000 | 0.0058 (3) | 0.00000 |
Geometric parameters (Å, º) top
Si—O2 | 1.5866 (2) | Al—O1iv | 1.9451 (2) |
Si—O3i | 1.6242 (2) | Al—O1v | 1.9965 (2) |
Si—O3ii | 1.6280 (2) | Li—O1 | 2.1021 (8) |
Si—O1 | 1.6404 (2) | Li—O3vi | 2.2524 (9) |
Al—O2iii | 1.8200 (2) | Li—O2vii | 2.2797 (3) |
| | | |
O2—Si—O3i | 111.87 (1) | O1—Li—O3xii | 116.70 (1) |
O2—Si—O3ii | 104.11 (1) | O1—Li—O3vi | 139.84 (1) |
O2—Si—O1 | 116.55 (1) | O2xi—Li—O1 | 75.92 (2) |
O3i—Si—O3ii | 107.32 (1) | O2vii—Li—O1 | 90.40 (3) |
O3i—Si—O1 | 108.04 (1) | O3xii—Li—O2vii | 68.03 (1) |
O3ii—Si—O1 | 108.50 (1) | O3xii—Li—O2xi | 128.13 (4) |
O2iii—Al—O2viii | 99.90 (1) | Si—O1—Aliv | 119.85 (1) |
O2iii—Al—O1ix | 88.43 (1) | Si—O1—Ali | 121.95 (1) |
O2iii—Al—O1v | 167.85 (1) | Si—O2—Alxiii | 148.37 (1) |
O1v—Al—O1ix | 84.82 (1) | Siv—O3—Sixiv | 138.91 (1) |
O2iii—Al—O1ii | 91.52 (1) | Aliv—O1—Ali | 101.12 (1) |
O2iii—Al—O1iv | 91.98 (1) | Si—O1—Li | 114.76 (2) |
O1ii—Al—O1ix | 78.88 (1) | Si—O2—Livii | 93.91 (3) |
O1ii—Al—O1v | 97.05 (1) | Siv—O3—Lixv | 116.68 (1) |
O1iv—Al—O1ii | 174.55 (1) | Sixiv—O3—Lixv | 93.78 (2) |
O1—Li—O1x | 79.67 (4) | Aliv—O1—Li | 96.51 (1) |
O2vii—Li—O2xi | 162.29 (5) | Ali—O1—Li | 97.76 (2) |
O3vi—Li—O3xii | 75.59 (3) | Alxiii—O2—Livii | 94.29 (2) |
Symmetry codes: (i) x, y−1, z; (ii) x, −y+1, z+1/2; (iii) x−1/2, y+1/2, z; (iv) −x, −y+1, −z; (v) x, y+1, z; (vi) x−1/2, y−1/2, z; (vii) −x+1/2, −y+1/2, −z+1; (viii) −x+1/2, y+1/2, −z+1/2; (ix) −x, y+1, −z+1/2; (x) −x, y, −z+1/2; (xi) x−1/2, −y+1/2, z−1/2; (xii) −x+1/2, y−1/2, −z+1/2; (xiii) x+1/2, y−1/2, z; (xiv) x, −y+1, z−1/2; (xv) x+1/2, y+1/2, z. |
Crystal data top
LiAl(SiO3)2 | F(000) = 368.0 |
Mr = 186.09 | Dx = 3.18 Mg m−3 |
Monoclinic, C2/c | Ag Kα radiation, λ = 0.5608 Å |
a = 9.456 (1) Å | Cell parameters from 25 reflections |
b = 8.386 (1) Å | θ = 9.4–23.6° |
c = 5.216 (1) Å | µ = 0.54 mm−1 |
β = 110.13 (1)° | T = 293 K |
V = 388.36 (9) Å3 | Parallelepiped, colourless |
Z = 4 | 0.36 × 0.18 × 0.06 mm |
Data collection top
Enraf-Nonius CAD4 diffractometer | Rint = 0.021 |
ω/2θ scans | θmax = 45.0°, θmin = 2.6° |
Absorption correction: integration empirical (using intensity measurements) integration (ABSORB, G. de Titta, 1985)
and empirical (using intensity measurements) (DREADD, R. Blessing, 1995) | h = −23→23 |
Tmin = 0.82, Tmax = 0.97 | k = −21→21 |
15850 measured reflections | l = −13→13 |
3241 independent reflections | 4 standard reflections every 120 min |
2261 reflections with I > 3σ(I) | intensity decay: none |
Refinement top
Refinement on F | w = 1/[σ2(F2) + (0.0160F2)2] |
R[F2 > 2σ(F2)] = 0.016 | (Δ/σ)max < 0.001 |
wR(F2) = 0.015 | Δρmax = 0.2 e Å−3 |
S = 0.84 | Δρmin = −0.1 e Å−3 |
2261 reflections | Extinction correction: Becker-Coppens type 1 Lorentzian isotropic |
138 parameters | Extinction coefficient: 4.9.102 |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top | x | y | z | Uiso*/Ueq | |
Si | 0.29410 (1) | 0.09345 (1) | 0.25593 (2) | 0.00397 (3) | |
Al | 0.00000 | 0.90669 (2) | 0.25000 | 0.00424 (4) | |
O1 | 0.10975 (2) | 0.08237 (2) | 0.14061 (4) | 0.00495 (5) | |
O2 | 0.36470 (3) | 0.26708 (3) | 0.30050 (5) | 0.00771 (6) | |
O3 | 0.35663 (2) | 0.98668 (3) | 0.05824 (4) | 0.00766 (6) | |
Li | 0.00000 | 0.27494 (14) | 0.25000 | 0.01474 (4) | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Si | 0.00386 (3) | 0.00447 (3) | 0.00355 (3) | −0.00062 (2) | 0.00125 (2) | −0.00020 (2) |
Al | 0.00420 (4) | 0.00427 (4) | 0.00418 (4) | 0.00000 | 0.00134 (3) | 0.00000 |
O1 | 0.00389 (5) | 0.00587 (6) | 0.00469 (6) | −0.00033 (5) | 0.00096 (4) | 0.00020 (5) |
O2 | 0.00817 (7) | 0.00569 (6) | 0.00991 (7) | −0.00291 (5) | 0.00392 (6) | −0.00084 (6) |
O3 | 0.00590 (6) | 0.01141 (8) | 0.00529 (6) | 0.00068 (6) | 0.00145 (5) | −0.00339 (6) |
Li | 0.0154 (5) | 0.0137 (5) | 0.0151 (5) | 0.00000 | 0.0051 (4) | 0.00000 |
Geometric parameters (Å, º) top
Si—O2 | 1.5852 (2) | Al—O1iv | 1.9447 (2) |
Si—O3i | 1.6230 (2) | Al—O1v | 1.9951 (2) |
Si—O3ii | 1.6268 (2) | Li—O1 | 2.1019 (9) |
Si—O1 | 1.6393 (2) | Li—O3vi | 2.2491 (9) |
Al—O2iii | 1.8190 (2) | Li—O2vii | 2.2791 (3) |
| | | |
O2—Si—O3i | 111.89 (1) | O1—Li—O3xii | 116.68 (1) |
O2—Si—O3ii | 104.07 (1) | O1—Li—O3vi | 139.84 (1) |
O2—Si—O1 | 116.54 (1) | O2xi—Li—O1 | 75.92 (2) |
O3i—Si—O3ii | 107.32 (1) | O2vii—Li—O1 | 90.32 (3) |
O3i—Si—O1 | 108.02 (1) | O3xii—Li—O2vii | 68.00 (1) |
O3ii—Si—O1 | 108.55 (1) | O3xii—Li—O2xi | 128.22 (4) |
O2iii—Al—O2viii | 99.87 (2) | Si—O1—Aliv | 119.90 (1) |
O2iii—Al—O1ix | 88.45 (1) | Si—O1—Ali | 121.93 (1) |
O2iii—Al—O1v | 167.87 (2) | Si—O2—Alxiii | 148.39 (2) |
O1v—Al—O1ix | 84.80 (1) | Siv—O3—Sixiv | 138.89 (2) |
O2iii—Al—O1ii | 91.55 (1) | Aliv—O1—Ali | 101.07 (1) |
O2iii—Al—O1iv | 91.94 (1) | Si—O1—Li | 114.76 (2) |
O1ii—Al—O1ix | 78.93 (1) | Si—O2—Livii | 93.89 (3) |
O1ii—Al—O1v | 97.02 (1) | Siv—O3—Lixv | 116.65 (1) |
O1iv—Al—O1ii | 174.59 (1) | Sixiv—O3—Lixv | 93.86 (2) |
O1—Li—O1x | 79.60 (4) | Aliv—O1—Li | 96.48 (1) |
O2vii—Li—O2xi | 162.21 (6) | Ali—O1—Li | 97.81 (2) |
O3vi—Li—O3xii | 75.72 (3) | Alxiii—O2—Livii | 94.28 (2) |
Symmetry codes: (i) x, y−1, z; (ii) x, −y+1, z+1/2; (iii) x−1/2, y+1/2, z; (iv) −x, −y+1, −z; (v) x, y+1, z; (vi) x−1/2, y−1/2, z; (vii) −x+1/2, −y+1/2, −z+1; (viii) −x+1/2, y+1/2, −z+1/2; (ix) −x, y+1, −z+1/2; (x) −x, y, −z+1/2; (xi) x−1/2, −y+1/2, z−1/2; (xii) −x+1/2, y−1/2, −z+1/2; (xiii) x+1/2, y−1/2, z; (xiv) x, −y+1, z−1/2; (xv) x+1/2, y+1/2, z. |