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Single crystals of rubidium manganese arsenate, RbMn6(As2O7)2(As3O10), have been prepared by a solid-state reaction at 1173 K. The compound crystallizes in the monoclinic system, space group P21/m. The structure consists of a complex network of edge-sharing MnO6 octahedra, forming folded layers that are linked together by As2O7 and As3O10 groups, which is highly unusual. This arrangement delimits a tunnel parallel to the a-axis direction which accommodates Rb+.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536804004544/br6138sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536804004544/br6138Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](Mn-O) = 0.006 Å
  • R factor = 0.037
  • wR factor = 0.111
  • Data-to-parameter ratio = 12.5

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT213_ALERT_2_B Atom O6 has ADP max/min Ratio ............. 4.10 oblate
Alert level C PLAT213_ALERT_2_C Atom O13 has ADP max/min Ratio ............. 3.30 oblate PLAT220_ALERT_2_C Large Non-Solvent O Ueq(max)/Ueq(min) ... 2.85 Ratio PLAT241_ALERT_2_C Check High U(eq) as Compared to Neighbors .... O13
0 ALERT level A = In general: serious problem 1 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 4 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Computing details top

Data collection: CAD-4 EXPRESS (Duisenberg, 1992; Macíček & Yordanov, 1992); cell refinement: CAD-4 EXPRESS; data reduction: MolEN (Fair, 1990); program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: Diamond (Brandenburg, 1998); software used to prepare material for publication: SHELXL97.

Rubidium manganese arsenate(1;6;7) top
Crystal data top
As7Mn6O24RbF(000) = 1220
Mr = 1323.53Dx = 4.358 Mg m3
Monoclinic, P21/mMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybCell parameters from 25 reflections
a = 5.555 (1) Åθ = 1.5–27.0°
b = 27.830 (9) ŵ = 17.56 mm1
c = 6.842 (2) ÅT = 293 K
β = 107.56 (2)°Prismatic, colourless
V = 1008.5 (5) Å30.1 × 0.05 × 0.04 mm
Z = 2
Data collection top
Enarf–Nonius CAD-4
diffractometer
1726 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.079
Graphite monochromatorθmax = 27.0°, θmin = 1.5°
ω/2θ scansh = 07
Absorption correction: ψ scan
(North et al., 1968)
k = 035
Tmin = 0.363, Tmax = 0.495l = 88
2461 measured reflections2 standard reflections every 120 min
2240 independent reflections intensity decay: 0.4%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.037 w = 1/[σ2(Fo2) + (0.0524P)2 + 3.8056P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.111(Δ/σ)max < 0.001
S = 1.09Δρmax = 1.58 e Å3
2240 reflectionsΔρmin = 1.47 e Å3
179 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0007 (2)
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
As10.27497 (14)0.47698 (3)0.69774 (12)0.0063 (2)
As20.68483 (15)0.38723 (3)0.87410 (12)0.0069 (2)
As30.5271 (2)0.25000.56840 (17)0.0069 (3)
As40.22919 (14)0.33587 (3)0.27565 (12)0.0067 (2)
Rb0.6964 (2)0.25000.10323 (18)0.0157 (3)
Mn10.1836 (2)0.54331 (5)0.82064 (19)0.0092 (3)
Mn20.2149 (2)0.40166 (5)0.40127 (18)0.0085 (3)
Mn30.1078 (2)0.31554 (4)0.74999 (18)0.0085 (3)
O10.8760 (10)0.4017 (2)0.1078 (8)0.0087 (11)
O20.1082 (11)0.4523 (2)0.4749 (9)0.0106 (12)
O30.4178 (11)0.52893 (19)0.6737 (9)0.0100 (11)
O40.8293 (15)0.25000.7056 (13)0.0133 (18)
O50.3887 (11)0.38634 (19)0.2693 (9)0.0106 (12)
O60.8518 (11)0.3769 (2)0.7101 (8)0.0122 (12)
O70.4942 (11)0.2986 (2)0.4071 (9)0.0138 (12)
O80.0451 (10)0.3365 (2)0.4307 (8)0.0104 (12)
O90.1132 (11)0.4800 (2)0.8687 (9)0.0117 (12)
O100.1027 (11)0.3067 (2)0.0578 (8)0.0116 (12)
O110.3127 (15)0.25000.6908 (12)0.0098 (16)
O120.4812 (11)0.3433 (2)0.8713 (10)0.0160 (13)
O130.5441 (13)0.4425 (2)0.7970 (11)0.0250 (16)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
As10.0062 (4)0.0067 (4)0.0068 (4)0.0002 (3)0.0032 (3)0.0005 (3)
As20.0051 (4)0.0089 (4)0.0070 (4)0.0005 (3)0.0023 (3)0.0008 (3)
As30.0055 (5)0.0079 (5)0.0081 (5)0.0000.0033 (4)0.000
As40.0068 (4)0.0070 (4)0.0075 (4)0.0007 (3)0.0041 (3)0.0010 (3)
Rb0.0164 (6)0.0182 (6)0.0150 (6)0.0000.0084 (5)0.000
Mn10.0083 (6)0.0112 (6)0.0091 (6)0.0005 (5)0.0043 (5)0.0019 (5)
Mn20.0075 (6)0.0106 (6)0.0086 (6)0.0005 (5)0.0044 (5)0.0006 (5)
Mn30.0095 (6)0.0088 (6)0.0083 (6)0.0010 (5)0.0042 (5)0.0003 (5)
O10.010 (3)0.010 (3)0.007 (3)0.001 (2)0.003 (2)0.002 (2)
O20.009 (3)0.013 (3)0.012 (3)0.003 (2)0.005 (2)0.002 (2)
O30.012 (3)0.004 (3)0.018 (3)0.001 (2)0.009 (2)0.000 (2)
O40.004 (4)0.022 (5)0.013 (4)0.0000.001 (3)0.000
O50.010 (3)0.003 (3)0.019 (3)0.002 (2)0.004 (2)0.000 (2)
O60.014 (3)0.018 (3)0.008 (3)0.003 (2)0.009 (2)0.002 (2)
O70.014 (3)0.010 (3)0.019 (3)0.008 (2)0.007 (2)0.008 (2)
O80.010 (3)0.015 (3)0.010 (3)0.008 (2)0.007 (2)0.006 (2)
O90.013 (3)0.013 (3)0.013 (3)0.001 (2)0.009 (2)0.002 (2)
O100.017 (3)0.012 (3)0.006 (3)0.005 (2)0.004 (2)0.000 (2)
O110.011 (4)0.014 (4)0.008 (4)0.0000.008 (3)0.000
O120.012 (3)0.017 (3)0.021 (3)0.007 (2)0.007 (3)0.000 (3)
O130.017 (3)0.016 (3)0.037 (4)0.012 (3)0.001 (3)0.003 (3)
Geometric parameters (Å, º) top
As1—O21.674 (6)Rb—O12vi3.090 (6)
As1—O91.679 (6)Rb—O12v3.090 (6)
As1—O31.681 (5)Rb—O8iii3.456 (6)
As1—O131.733 (6)Rb—O8iv3.456 (6)
As2—O121.661 (6)Mn1—O9vii2.143 (6)
As2—O1i1.680 (5)Mn1—O3viii2.175 (6)
As2—O61.683 (5)Mn1—O2ix2.189 (6)
As2—O131.734 (6)Mn1—O1x2.235 (6)
As3—O111.650 (8)Mn1—O5ix2.255 (6)
As3—O41.658 (8)Mn1—O92.366 (6)
As3—O7ii1.721 (6)Mn2—O6viii2.145 (6)
As3—O71.721 (6)Mn2—O5viii2.156 (6)
As4—O101.656 (6)Mn2—O1viii2.213 (5)
As4—O51.668 (5)Mn2—O22.217 (6)
As4—O81.681 (5)Mn2—O3ix2.217 (6)
As4—O71.803 (6)Mn2—O82.289 (6)
Rb—O10iii2.846 (6)Mn3—O10i2.129 (6)
Rb—O10iv2.846 (6)Mn3—O122.134 (6)
Rb—O72.971 (6)Mn3—O82.185 (5)
Rb—O7ii2.971 (6)Mn3—O6viii2.186 (6)
Rb—O11v2.980 (8)Mn3—O112.251 (5)
Rb—O4v3.026 (8)Mn3—O4viii2.351 (5)
O2—As1—O9113.0 (3)O10iv—Rb—O8iii98.57 (15)
O2—As1—O3114.3 (3)O7ii—Rb—O8iii96.89 (15)
O9—As1—O3113.1 (3)O11v—Rb—O8iii135.62 (9)
O2—As1—O13107.7 (3)O4v—Rb—O8iii109.98 (14)
O9—As1—O13109.6 (3)O12vi—Rb—O8iii166.54 (15)
O3—As1—O1397.9 (3)O10iii—Rb—O8iv98.57 (15)
O12—As2—O1i114.9 (3)O7—Rb—O8iv96.89 (15)
O12—As2—O6112.2 (3)O11v—Rb—O8iv135.62 (9)
O1i—As2—O6111.0 (3)O4v—Rb—O8iv109.98 (14)
O12—As2—O13113.9 (3)O12v—Rb—O8iv166.54 (15)
O1i—As2—O13100.0 (3)O9vii—Mn1—O3viii105.0 (2)
O6—As2—O13103.7 (3)O9vii—Mn1—O2ix154.8 (2)
O11—As3—O4118.4 (4)O3viii—Mn1—O2ix92.0 (2)
O11—As3—O7ii111.9 (2)O9vii—Mn1—O1x95.3 (2)
O4—As3—O7ii104.9 (3)O3viii—Mn1—O1x146.3 (2)
O11—As3—O7111.9 (2)O9vii—Mn1—O5ix117.4 (2)
O4—As3—O7104.9 (3)O3viii—Mn1—O9119.8 (2)
O7ii—As3—O7103.7 (4)O1x—Mn1—O991.4 (2)
O10—As4—O5118.3 (3)O5ix—Mn1—O9163.2 (2)
O10—As4—O8113.5 (3)O6viii—Mn2—O5viii101.6 (2)
O5—As4—O8115.9 (3)O6viii—Mn2—O1viii151.0 (2)
O10—As4—O7103.2 (3)O5viii—Mn2—O1viii96.0 (2)
O5—As4—O797.9 (3)O6viii—Mn2—O295.3 (2)
O8—As4—O7104.6 (3)O5viii—Mn2—O2151.1 (2)
O10iii—Rb—O7107.67 (17)O6viii—Mn2—O3ix115.6 (2)
O10iv—Rb—O7143.95 (16)O1viii—Mn2—O3ix91.6 (2)
O10iii—Rb—O7ii143.95 (16)O5viii—Mn2—O8114.7 (2)
O10iv—Rb—O7ii107.67 (17)O2—Mn2—O892.1 (2)
O10iii—Rb—O11v105.12 (17)O3ix—Mn2—O8166.8 (2)
O10iv—Rb—O11v105.12 (17)O10i—Mn3—O8166.9 (2)
O7—Rb—O11v110.44 (17)O12—Mn3—O897.8 (2)
O7ii—Rb—O11v110.44 (17)O10i—Mn3—O6viii90.7 (2)
O7—Rb—O4v151.10 (12)O12—Mn3—O6viii106.5 (2)
O7ii—Rb—O4v151.10 (12)O10i—Mn3—O11104.0 (2)
O10iii—Rb—O12vi127.33 (16)O6viii—Mn3—O11162.9 (3)
O7—Rb—O12vi124.96 (17)O12—Mn3—O4viii148.9 (2)
O10iv—Rb—O12v127.33 (16)O8—Mn3—O4viii100.2 (3)
O7ii—Rb—O12v124.96 (17)O6viii—Mn3—O4viii102.3 (2)
O12vi—Rb—O12v114.4 (2)
Symmetry codes: (i) x, y, z+1; (ii) x, y+1/2, z; (iii) x+1, y, z; (iv) x+1, y+1/2, z; (v) x, y, z1; (vi) x, y+1/2, z1; (vii) x, y+1, z+2; (viii) x1, y, z; (ix) x, y+1, z+1; (x) x+1, y+1, z+1.
 

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