inorganic compounds
The crystal structure of lithium manganese vanadate, LiMnVO4, is characterized by chains of edge-sharing MnO6 octahedra, bridged by pairs of edge-sharing LiO4 and VO4 tetrahedra. Cation–cation repulsions displace the V and Li ions from the tetrahedral centres and deform the tetrahedra further by shortening the mutually shared O—O edges. The smallest r.m.s. atomic displacements in thermal motion for Li and V are parallel to the shortest LiV vector with maximum vibrational motion normal to that direction. Cation–cation interactions between the Li and V tetrahedral sites play an important role.
Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803023742/br6121sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536803023742/br6121Isup2.hkl |
Computing details top
Data collection: MSC Software (Rigaku, 1996); cell refinement: MSC Software; data reduction: MSC Software; program(s) used to solve structure: RADY89 (Sasaki, 1989); program(s) used to refine structure: RADY89; molecular graphics: ORTEP-3 for Windows (Farrugia, 1997).
lithium manganese vanadate top
Crystal data top
LiMnVO4 | F(000) = 332.0 |
Mr = 176.82 | Dx = 3.663 Mg m−3 |
Orthorhombic, Cmcm | Mo Kα radiation, λ = 0.71069 Å |
Hall symbol: -C 2c 2 | Cell parameters from 25 reflections |
a = 5.7640 (3) Å | θ = 39.4–49.0° |
b = 8.7418 (9) Å | µ = 6.68 mm−1 |
c = 6.3629 (3) Å | T = 297 K |
V = 320.61 (4) Å3 | Sphere, brown |
Z = 4 | 0.08 mm (radius) |
Data collection top
Rigaku AFC-5S diffractometer | 902 reflections with F > 3σ(F) |
Radiation source: X-ray tube | Rint = 0.014 |
Graphite monochromator | θmax = 50.0°, θmin = 4.2° |
θ/2θ scans | h = 0→12 |
Absorption correction: for a sphere International Tables Vol C Table 6.3.3.3 | k = −18→0 |
Tmin = 0.330, Tmax = 0.343 | l = −13→13 |
1759 measured reflections | 3 standard reflections every 150 reflections |
944 independent reflections | intensity decay: none |
Refinement top
Refinement on F | 0 constraints |
Least-squares matrix: full | w = 1/[σ2(Fo) + (0.013936Fo)2] |
R[F2 > 2σ(F2)] = 0.022 | (Δ/σ)max < 0.001 |
wR(F2) = 0.033 | Δρmax = 0.18 e Å−3 |
S = 1.83 | Δρmin = −1.19 e Å−3 |
1663 reflections | Extinction correction: RADY89 (Sasaki, 1989) |
26 parameters | Extinction coefficient: 0.057 (4) |
0 restraints |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
x | y | z | Uiso*/Ueq | ||
Li | 0.0000 | 0.6637 (7) | 0.2500 | 0.0241 (11) | |
Mn | 0.0000 | 0.0000 | 0.0000 | 0.00856 (4) | |
V | 0.0000 | 0.35663 (3) | 0.2500 | 0.00709 (4) | |
O1 | 0.24050 (17) | 0.47975 (10) | 0.2500 | 0.01086 (13) | |
O2 | 0.0000 | 0.24600 (12) | 0.03228 (15) | 0.01164 (14) |
Atomic displacement parameters (Å2) top
U11 | U22 | U33 | U12 | U13 | U23 | |
Li | 0.033 (3) | 0.0183 (19) | 0.021 (2) | 0.000 | 0.000 | 0.000 |
Mn | 0.00905 (9) | 0.00916 (9) | 0.00747 (9) | 0.000 | 0.000 | 0.00023 (5) |
V | 0.00621 (8) | 0.00740 (9) | 0.00766 (9) | 0.000 | 0.000 | 0.000 |
O1 | 0.0097 (3) | 0.0122 (3) | 0.0107 (3) | −0.0030 (2) | 0.000 | 0.000 |
O2 | 0.0133 (3) | 0.0109 (3) | 0.0107 (3) | 0.000 | 0.000 | −0.0023 (2) |
Geometric parameters (Å, º) top
Li—O1 | 2.123 (4) | Mn—O2viii | 2.1602 (10) |
Li—O1i | 2.123 (4) | V—O1 | 1.7544 (9) |
Li—O2ii | 1.962 (2) | V—O1i | 1.7544 (9) |
Li—O2iii | 1.962 (2) | V—O2 | 1.6896 (10) |
Mn—O1iv | 2.1909 (6) | V—O2i | 1.6896 (10) |
Mn—O1v | 2.1909 (6) | O1—O1i | 2.772 (1) |
Mn—O1vi | 2.1909 (6) | O1—O1ix | 2.992 (1) |
Mn—O1vii | 2.1909 (6) | O1—O1iii | 3.2011 (2) |
Mn—O2 | 2.1602 (10) | ||
O1—Li—O1i | 81.5 (2) | O2—Mn—O2x | 180 |
O1—Li—O2iii | 107.7 (2) | O1—V—O1i | 104.35 (10) |
O2ii—Li—O2iii | 132.5 (3) | O1—V—O2 | 110.55 (2) |
O1vii—Mn—O1vi | 86.12 (6) | O2—V—O2xi | 110.2 (1) |
O1vii—Mn—O2 | 90.65 (6) |
Symmetry codes: (i) −x, y, −z+1/2; (ii) −x, −y+1, z+1/2; (iii) x, −y+1, −z; (iv) −x+1/2, −y+1/2, −z; (v) x−1/2, −y+1/2, −z; (vi) x−1/2, y−1/2, z; (vii) −x+1/2, y−1/2, −z+1/2; (viii) x, −y, −z; (ix) −x+1, y, −z+1/2; (x) −x, −y, −z; (xi) x, y, −z+1/2. |