Literature DB >> 21582037

Li(3)Al(MoO(2))(2)O(2)(AsO(4))(2).

Mounir Hajji1, Mohamed Faouzi Zid, Ahmed Driss.   

Abstract

Single crystals of trilithium(I) aluminium(III) bis-[dioxidomolybdenum(VI)] dioxide bis-[arsenate(V)], Li(3)AlMo(2)As(2)O(14), have been prepared by solid-state reaction at 788 K. The structure consists of AsO(4) tetra-hedra, AlO(6) octa-hedra and Mo(2)O(10) groups sharing corners to form a three-dimensional framework containing channels running respectively along the [100] and [010] directions, where the Li(+) ions are located. This structure is compared with compounds having (MX(2)O(12))(n) chains (M = Mo, Al and X = P, As) and others containing M(2)O(10) (M = Mo, Fe) dimers.

Entities:  

Year:  2009        PMID: 21582037      PMCID: PMC2968439          DOI: 10.1107/S160053680900631X

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Littérature assocíee

Pour le détail de la préparation, voir: Hajji et al. (2004 ▶, 2005 ▶); Zid et al. (1997 ▶, 1998 ▶). Pour le détail des composés avec structures reliées, voir: Lii et al. (1989 ▶); Leclaire et al. (1990 ▶); Driss & Jouini (1989 ▶); Guesdon et al. (1994 ▶); Borel et al. (1994 ▶); LeBail et al. (1995 ▶). Pour le détail des propriétés des composés reliés, voir: Manthiram & Goodenough, 1989 ▶; Tarascon et al., 1991 ▶; Sigala et al., 1997 ▶; Padhi et al., 1997 ▶; Masquelier et al., 1998 ▶. Pour le calcul des valences des liaisons, voir: Brown & Altermatt (1985 ▶)

Partie expérimentale

Données crystallines

Li3Al(MoO2)2O2(AsO4)2 M = 613.52 Triclinique, a = 5.213 (1) Å b = 5.426 (1) Å c = 9.474 (2) Å α = 95.98 (2)° β = 102.25 (1)° γ = 105.30 (1)° V = 248.92 (9) Å3 Z = 1 Mo Kα radiation μ = 9.29 mm−1 T = 298 K 0.20 × 0.15 × 0.12 mm

Collection des données

Diffractomètre Enraf–Nonius TurboCAD-4 Correction d’absorption: ψ scan (North et al., 1968 ▶) T min = 0.209, T max = 0.328 1663 réflexions mesurées 1084 réflexions independantes 1077 réflexions avec I > 2σ(I) R int = 0.007 2 réflexions de référence fréquence: 120 min décroissance d’intensité: 1.1%

Affinement

R[F 2 > 2σ(F 2)] = 0.013 wR(F 2) = 0.039 S = 1.06 1084 réflexions 104 paramètres Δρmax = 0.64 e Å−3 Δρmin = −0.41 e Å−3 Collection des données: CAD-4 EXPRESS (Duisenberg, 1992 ▶; Macíček & Yordanov, 1992 ▶); affinement des paramètres de la maille: CAD-4 EXPRESS; reduction des données: XCAD4 (Harms & Wocadlo, 1995 ▶); programme(s) pour la solution de la structure: SHELXS97 (Sheldrick, 2008 ▶); programme(s) pour l’affinement de la structure: SHELXL97 (Sheldrick, 2008 ▶); graphisme moléculaire: DIAMOND (Brandenburg, 1998 ▶); logiciel utilisé pour préparer le matériel pour publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053680900631X/br2097sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S160053680900631X/br2097Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Li3Al(MoO2)2O2(AsO4)2Z = 1
Mr = 613.52F(000) = 284
Triclinic, P1Dx = 4.093 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 5.213 (1) ÅCell parameters from 25 reflections
b = 5.426 (1) Åθ = 10–16°
c = 9.474 (2) ŵ = 9.29 mm1
α = 95.98 (2)°T = 298 K
β = 102.25 (1)°Prism, yellow
γ = 105.30 (1)°0.20 × 0.15 × 0.12 mm
V = 248.92 (9) Å3
Enraf–Nonius TurboCAD-4 diffractometer1077 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.007
graphiteθmax = 27.0°, θmin = 2.2°
ω/2θ scansh = −2→6
Absorption correction: ψ scan (North et al., 1968)k = −6→6
Tmin = 0.209, Tmax = 0.328l = −12→12
1663 measured reflections2 standard reflections every 120 min
1084 independent reflections intensity decay: 1.1%
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.013w = 1/[σ2(Fo2) + (0.021P)2 + 0.6735P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.039(Δ/σ)max = 0.001
S = 1.06Δρmax = 0.64 e Å3
1084 reflectionsΔρmin = −0.41 e Å3
104 parametersExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0263 (14)
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
Mo0.49876 (4)0.84099 (4)0.35495 (2)0.00633 (9)
As0.15020 (5)0.23501 (5)0.17692 (3)0.00601 (10)
Al0.50000.00000.00000.0026 (2)
Li10.00000.50000.50000.0225 (16)
Li20.8077 (14)0.6121 (14)0.1486 (9)0.0392 (16)
O10.6756 (4)0.1635 (4)0.4618 (2)0.0099 (4)
O20.7195 (4)0.6684 (4)0.4132 (2)0.0132 (4)
O30.4158 (4)0.2923 (4)0.0959 (2)0.0109 (4)
O40.8654 (4)0.2067 (4)0.0441 (2)0.0110 (4)
O50.5596 (4)0.8659 (4)0.1781 (2)0.0098 (4)
O60.1363 (4)−0.0156 (4)0.2672 (2)0.0101 (4)
O70.1633 (4)0.5095 (4)0.2895 (2)0.0106 (4)
U11U22U33U12U13U23
Mo0.00695 (13)0.00664 (13)0.00518 (13)0.00175 (8)0.00146 (8)0.00074 (8)
As0.00626 (14)0.00629 (14)0.00524 (14)0.00179 (10)0.00123 (10)0.00057 (9)
Al0.0027 (5)0.0038 (4)0.0011 (4)0.0005 (4)0.0004 (3)0.0002 (3)
Li10.018 (4)0.018 (4)0.031 (4)0.007 (3)−0.001 (3)0.011 (3)
Li20.031 (3)0.031 (3)0.063 (5)0.017 (3)0.014 (3)0.017 (3)
O10.0108 (9)0.0086 (9)0.0086 (8)0.0001 (7)0.0024 (7)0.0012 (7)
O20.0137 (10)0.0127 (9)0.0146 (10)0.0055 (8)0.0035 (8)0.0044 (8)
O30.0115 (9)0.0094 (9)0.0126 (9)0.0020 (7)0.0067 (7)0.0010 (7)
O40.0086 (9)0.0135 (9)0.0092 (9)0.0025 (7)−0.0009 (7)0.0025 (7)
O50.0093 (9)0.0115 (9)0.0083 (9)0.0020 (7)0.0025 (7)0.0020 (7)
O60.0099 (9)0.0110 (9)0.0114 (9)0.0044 (7)0.0032 (7)0.0061 (7)
O70.0109 (9)0.0086 (9)0.0108 (9)0.0004 (7)0.0048 (7)−0.0023 (7)
Mo—O21.707 (2)Al—O3v1.942 (2)
Mo—O51.782 (2)Al—O31.942 (2)
Mo—O1i1.822 (2)Li1—O2ii2.000 (2)
Mo—O72.080 (2)Li1—O2iv2.000 (2)
Mo—O1ii2.123 (2)Li1—O1ii2.073 (2)
Mo—O6i2.261 (2)Li1—O1iv2.073 (2)
Mo—Moiii3.0849 (8)Li1—O7viii2.328 (2)
As—O61.6737 (19)Li1—O72.328 (2)
As—O4iv1.6903 (19)Li2—O52.159 (7)
As—O31.6960 (19)Li2—O32.225 (7)
As—O71.7164 (19)Li2—O6ix2.272 (8)
Al—O4v1.870 (2)Li2—O7x2.275 (7)
Al—O41.870 (2)Li2—O42.435 (7)
Al—O5vi1.905 (2)Li2—O3vii2.533 (8)
Al—O5vii1.905 (2)Li2—O22.645 (8)
O2—Mo—O598.47 (9)O2ii—Li1—O2iv180.000 (1)
O2—Mo—O1i102.62 (9)O2ii—Li1—O1ii86.18 (8)
O5—Mo—O1i104.19 (9)O2iv—Li1—O1ii93.82 (8)
O2—Mo—O792.53 (9)O2ii—Li1—O1iv93.82 (8)
O5—Mo—O796.70 (8)O2iv—Li1—O1iv86.18 (8)
O1i—Mo—O7151.88 (8)O1ii—Li1—O1iv180.0
O2—Mo—O1ii96.79 (9)O2ii—Li1—O7viii90.24 (8)
O5—Mo—O1ii163.86 (8)O2iv—Li1—O7viii89.76 (8)
O1i—Mo—O1ii77.39 (9)O1ii—Li1—O7viii106.95 (7)
O7—Mo—O1ii77.39 (7)O1iv—Li1—O7viii73.05 (7)
O2—Mo—O6i167.49 (8)O2ii—Li1—O789.76 (8)
O5—Mo—O6i83.83 (8)O2iv—Li1—O790.24 (7)
O1i—Mo—O6i88.62 (8)O1ii—Li1—O773.05 (7)
O7—Mo—O6i74.97 (8)O1iv—Li1—O7106.95 (7)
O1ii—Mo—O6i80.14 (7)O7viii—Li1—O7180.0
O6—As—O4iv115.31 (9)O5—Li2—O385.6 (3)
O6—As—O3112.28 (9)O5—Li2—O6ix79.0 (2)
O4iv—As—O3106.27 (9)O3—Li2—O6ix158.9 (4)
O6—As—O7111.28 (10)O5—Li2—O7x136.7 (4)
O4iv—As—O7100.31 (10)O3—Li2—O7x112.7 (3)
O3—As—O7110.70 (9)O6ix—Li2—O7x71.1 (2)
O4v—Al—O4180.00 (15)O5—Li2—O4151.9 (4)
O4v—Al—O5vi88.07 (8)O3—Li2—O468.8 (2)
O4—Al—O5vi91.93 (8)O6ix—Li2—O4128.6 (3)
O4v—Al—O5vii91.93 (8)O7x—Li2—O467.36 (19)
O4—Al—O5vii88.07 (8)O5—Li2—O3vii69.4 (2)
O5vi—Al—O5vii180.00 (10)O3—Li2—O3vii81.2 (3)
O4v—Al—O3v87.61 (9)O6ix—Li2—O3vii106.3 (3)
O4—Al—O3v92.39 (9)O7x—Li2—O3vii148.8 (4)
O5vi—Al—O3v88.69 (8)O4—Li2—O3vii94.6 (3)
O5vii—Al—O3v91.31 (8)O5—Li2—O265.9 (2)
O4v—Al—O392.39 (9)O3—Li2—O284.0 (2)
O4—Al—O387.61 (9)O6ix—Li2—O276.6 (3)
O5vi—Al—O391.31 (8)O7x—Li2—O277.0 (2)
O5vii—Al—O388.69 (8)O4—Li2—O2120.1 (3)
O3v—Al—O3180.00 (12)O3vii—Li2—O2133.7 (3)
  3 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  [Li(MoO2)2O(AsO4)].

Authors:  Mounir Hajji; Mohamed Faouzi Zid; Tahar Jouini
Journal:  Acta Crystallogr C       Date:  2005-04-30       Impact factor: 1.172

3.  [Beta-LiMoO2(AsO4)].

Authors:  Mounir Hajji; Mohamed Faouzi Zid; Ahmed Driss; Tahar Jouini
Journal:  Acta Crystallogr C       Date:  2004-07-21       Impact factor: 1.172

  3 in total
  1 in total

1.  K(MoO2)4O3(AsO4).

Authors:  Raja Jouini; Mohamed Faouzi Zid; Ahmed Driss
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2013-05-25
  1 in total

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