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Ionothermal reaction between MnII(acetate)2·4H2O and 1,3,5-benzenetricarboxylic acid (H3BTC) in either of the two ionic liquids 1-ethyl-3-methylimidazolium bromide (EMIMBr) and 1-ethyl-3-methylimidazolium tosylate (EMIMOTs) resulted in the formation of the new metal–organic framework (MOF) EMIM[MnIIBTC] (BTC = 1,3,5-benzenetricarboxylate). The compound crystallizes in the orthorhombic space group Pbca with unit-cell parameters of a = 14.66658 (12), b = 12.39497 (9), c = 16.63509 (14) Å at 100 K. Multi-temperature single-crystal (15–340 K) and powder X-ray diffraction studies (100–400 K) reveal strongly anisotropic thermal expansion properties. The linear thermal expansion coefficients, αL(l), attain maximum values at 400 K along the a- and b-axis, with αL(a) = 115 × 10−6 K−1 and αL(b) = 75 × 10−6 K−1. At 400 K a negative thermal expansion coefficient of −40 × 10−6 K−1 is observed along the c-axis. The thermal expansion is coupled to a continuous deformation of the framework, which causes the structure to expand in two directions. Due to the rigidity of the linker, the expansion in the ab plane causes the network to contract along the c-axis. Hirshfeld surface analysis has been used to describe the interaction between the framework structure and the EMIM cation that resides within the channel. This reveals a number of rather weak interactions and one governing hydrogen-bonding interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520614003497/gw5029sup1.cif
Contains datablocks A100k, A200k, A293k, c100k, c160k, c220k, c280k, c300k, c320k, c340k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029a100ksup2.hkl
Contains datablock a100k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029c100ksup3.hkl
Contains datablock c100k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029c220ksup4.hkl
Contains datablock c220k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029c280ksup5.hkl
Contains datablock c280k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029c300ksup6.hkl
Contains datablock c300k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029c320ksup7.hkl
Contains datablock c320k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029c340ksup8.hkl
Contains datablock c340k

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614003497/gw5029c160ksup9.hkl
Contains datablock c160k

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520614003497/gw5029sup10.pdf
Additional information

Computing details top

Data collection: CrysAlis PRO, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) for A100k, A200k, A293k; CrysAlis PRO, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) for c100k, c160k, c220k, c280k, c300k, c320k, c340k. Cell refinement: CrysAlis PRO, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) for A100k, A200k, A293k; CrysAlis PRO, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) for c100k, c160k, c220k, c280k, c300k, c320k, c340k. Data reduction: CrysAlis PRO, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) for A100k, A200k, A293k; CrysAlis PRO, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) for c100k, c160k, c220k, c280k, c300k, c320k, c340k. Program(s) used to solve structure: XL, G.M. Sheldrick for A100k; SHELXS97 (Sheldrick, 1990) for A200k, A293k. Program(s) used to refine structure: XL, G.M. Sheldrick, Acta Cryst. (2008). A64, 112-122 for A100k; SHELXL, G.M. Sheldrick, Acta Cryst. (2008). A64, 112-122 for A200k, A293k, c100k, c160k, c220k, c280k, c300k, c320k, c340k. For all compounds, molecular graphics: O. V. Dolomanov, L. J. Bourhis, R. J. Gildea, J. A. K. Howard and H. Puschmann, OLEX2: a complete structure solution, refinement and analysis program. J. Appl. Cryst. (2009). 42, 339-341.; software used to prepare material for publication: O. V. Dolomanov, L. J. Bourhis, R. J. Gildea, J. A. K. Howard and H. Puschmann, OLEX2: a complete structure solution, refinement and analysis program. J. Appl. Cryst. (2009). 42, 339-341.

(A100k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.636 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.7107 Å
Orthorhombic, PbcaCell parameters from 19221 reflections
a = 14.66658 (13) Åθ = 1.6–26.3°
b = 12.39497 (9) ŵ = 0.91 mm1
c = 16.63509 (14) ÅT = 100 K
V = 3024.12 (4) Å3Prismatic, colorless
Z = 80.15 × 0.1 × 0.1 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3085 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2595 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.052
Detector resolution: 10.3590 pixels mm-1θmax = 26.4°, θmin = 2.5°
ω scansh = 1818
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1515
Tmin = 0.944, Tmax = 1.000l = 2020
62926 measured reflections
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)] = 0.029Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.074H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0298P)2 + 3.1301P]
where P = (Fo2 + 2Fc2)/3
3085 reflections(Δ/σ)max = 0.001
252 parametersΔρmax = 0.48 e Å3
308 restraintsΔρmin = 0.29 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Mn10.60521 (2)0.48211 (2)0.57858 (2)0.01431 (9)
O50.70905 (11)0.47937 (11)0.48412 (9)0.0285 (3)
O60.69872 (10)0.63114 (11)0.55141 (8)0.0244 (3)
O30.59455 (10)0.34596 (11)0.66585 (8)0.0230 (3)
O20.49860 (9)0.57987 (10)0.62631 (8)0.0183 (3)
C60.34762 (13)0.78092 (14)0.54026 (11)0.0165 (4)
H60.34370.75460.48800.020*
C120.3436 (4)0.2375 (4)0.7759 (3)0.0373 (11)0.833 (4)
H120.32360.16700.78340.045*0.833 (4)
C100.3921 (2)0.2204 (3)0.6314 (2)0.0479 (9)0.833 (4)
H10A0.42540.15530.64190.072*0.833 (4)
H10B0.42550.26420.59400.072*0.833 (4)
H10C0.33370.20280.60890.072*0.833 (4)
C130.3426 (2)0.3163 (3)0.8314 (2)0.0388 (8)0.833 (4)
H130.32250.31030.88420.047*0.833 (4)
C140.3886 (2)0.5147 (2)0.8322 (2)0.0449 (9)0.833 (4)
H14A0.32920.54680.84170.054*0.833 (4)
H14B0.42220.56160.79610.054*0.833 (4)
C10A0.3434 (14)0.3807 (17)0.8949 (10)0.064 (6)*0.167 (4)
H10D0.39750.37270.92690.096*0.167 (4)
H10E0.29770.33120.91340.096*0.167 (4)
H10F0.32100.45320.89980.096*0.167 (4)
C15A0.462 (2)0.137 (3)0.623 (2)0.167 (17)*0.167 (4)
H15D0.48560.10090.67030.251*0.167 (4)
H15E0.50240.19500.60910.251*0.167 (4)
H15F0.45830.08670.57970.251*0.167 (4)
N10.3794 (6)0.2794 (4)0.7058 (3)0.0375 (14)0.833 (4)
N2A0.374 (4)0.267 (2)0.7045 (15)0.033 (7)*0.167 (4)
O10.52326 (9)0.38012 (10)0.50253 (7)0.0188 (3)
C90.73158 (13)0.57672 (15)0.49526 (11)0.0182 (4)
C40.69562 (12)0.41130 (15)0.85950 (11)0.0165 (4)
H40.72660.47390.84520.020*
C80.63727 (13)0.39929 (15)0.71807 (11)0.0173 (4)
C50.70287 (13)0.37141 (15)0.93758 (11)0.0165 (4)
C70.46284 (12)0.63615 (14)0.57134 (11)0.0153 (4)
O40.67486 (10)0.48798 (11)0.70128 (8)0.0219 (3)
C12A0.3942 (11)0.4246 (12)0.7521 (11)0.025 (4)*0.167 (4)
H12A0.40700.49760.75830.030*0.167 (4)
C150.4395 (2)0.5047 (3)0.9112 (2)0.0568 (10)0.833 (4)
H15A0.49980.47790.90120.085*0.833 (4)
H15B0.40760.45570.94590.085*0.833 (4)
H15C0.44320.57430.93640.085*0.833 (4)
N20.37718 (16)0.4083 (2)0.7948 (2)0.0351 (7)0.833 (4)
N1A0.3646 (10)0.3582 (13)0.8110 (8)0.027 (3)*0.167 (4)
C14A0.3696 (17)0.1812 (19)0.6413 (15)0.066 (8)*0.167 (4)
H14C0.33020.12330.65950.079*0.167 (4)
H14D0.34360.21110.59260.079*0.167 (4)
C110.39740 (19)0.3835 (3)0.7201 (3)0.0340 (7)0.833 (4)
H110.42090.43150.68250.041*0.833 (4)
C11A0.357 (2)0.2568 (18)0.7844 (14)0.035 (7)*0.167 (4)
H11A0.34400.19460.81340.042*0.167 (4)
C13A0.4023 (11)0.3689 (12)0.6829 (9)0.025 (4)*0.167 (4)
H13A0.42200.39330.63300.029*0.167 (4)
C20.59313 (12)0.26701 (15)0.82532 (11)0.0162 (4)
H20.55800.23080.78740.019*
C10.40392 (12)0.72966 (14)0.59571 (11)0.0155 (4)
C30.64237 (13)0.35806 (14)0.80271 (11)0.0155 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.01763 (16)0.01430 (15)0.01099 (15)0.00055 (11)0.00109 (11)0.00051 (11)
O50.0358 (9)0.0224 (7)0.0272 (8)0.0123 (6)0.0118 (7)0.0056 (6)
O60.0305 (8)0.0218 (7)0.0208 (7)0.0031 (6)0.0100 (6)0.0004 (6)
O30.0335 (8)0.0221 (7)0.0133 (7)0.0035 (6)0.0051 (6)0.0026 (5)
O20.0221 (7)0.0172 (6)0.0155 (6)0.0040 (5)0.0015 (5)0.0002 (5)
C60.0209 (9)0.0162 (9)0.0124 (9)0.0007 (7)0.0003 (8)0.0011 (7)
C120.021 (2)0.0309 (19)0.060 (3)0.0016 (16)0.0059 (17)0.0224 (16)
C100.0309 (18)0.051 (2)0.062 (2)0.0013 (17)0.0015 (16)0.0152 (17)
C130.0216 (14)0.0342 (16)0.060 (2)0.0019 (13)0.0030 (13)0.0267 (16)
C140.0272 (15)0.0356 (15)0.072 (2)0.0013 (12)0.0072 (15)0.0101 (15)
N10.021 (2)0.0309 (19)0.061 (2)0.0021 (16)0.0012 (12)0.0219 (13)
O10.0230 (7)0.0195 (7)0.0138 (6)0.0002 (6)0.0010 (5)0.0019 (5)
C90.0182 (10)0.0209 (9)0.0155 (9)0.0011 (8)0.0009 (7)0.0020 (8)
C40.0152 (9)0.0162 (9)0.0180 (9)0.0001 (7)0.0007 (7)0.0015 (7)
C80.0157 (9)0.0198 (9)0.0163 (9)0.0026 (7)0.0002 (7)0.0027 (7)
C50.0165 (9)0.0170 (9)0.0160 (9)0.0004 (7)0.0014 (7)0.0019 (7)
C70.0146 (9)0.0152 (9)0.0163 (9)0.0032 (7)0.0020 (7)0.0009 (7)
O40.0249 (8)0.0214 (7)0.0193 (7)0.0044 (6)0.0030 (6)0.0071 (6)
C150.0364 (18)0.067 (2)0.067 (2)0.0065 (17)0.0132 (17)0.0141 (19)
N20.0195 (12)0.0320 (14)0.0538 (19)0.0003 (10)0.0071 (11)0.0209 (12)
C110.0166 (14)0.0336 (17)0.052 (2)0.0026 (12)0.0020 (15)0.0186 (17)
C20.0165 (9)0.0169 (9)0.0152 (9)0.0009 (7)0.0019 (7)0.0010 (7)
C10.0171 (9)0.0137 (9)0.0156 (9)0.0011 (7)0.0008 (7)0.0008 (7)
C30.0156 (9)0.0165 (9)0.0144 (9)0.0024 (7)0.0002 (7)0.0018 (7)
Geometric parameters (Å, º) top
Mn1—O52.1885 (15)N1—C111.339 (6)
Mn1—O62.3447 (14)N2A—C14A1.497 (18)
Mn1—O32.2316 (14)N2A—C11A1.358 (19)
Mn1—O22.1316 (13)N2A—C13A1.376 (18)
Mn1—O12.1547 (13)O1—C7ii1.262 (2)
Mn1—C92.5946 (19)C9—C5iii1.503 (3)
Mn1—C82.5806 (18)C4—C51.394 (3)
Mn1—O42.2837 (14)C4—C31.392 (3)
O5—C91.265 (2)C8—O41.261 (2)
O6—C91.249 (2)C8—C31.500 (2)
O3—C81.259 (2)C5—C6iv1.394 (3)
O2—C71.264 (2)C5—C9v1.503 (3)
C6—C5i1.394 (3)C7—O1ii1.262 (2)
C6—C11.392 (3)C7—C11.501 (3)
C12—C131.344 (6)C12A—N1A1.352 (15)
C12—N11.380 (5)C12A—C13A1.347 (12)
C10—N11.450 (6)N2—C111.315 (5)
C13—N21.389 (4)N1A—C11A1.338 (18)
C14—C151.515 (5)C2—C1iv1.394 (2)
C14—N21.468 (4)C2—C31.392 (3)
C10A—N1A1.457 (16)C1—C2i1.394 (2)
C15A—C14A1.494 (19)
O5—Mn1—O657.78 (5)C13A—N2A—C14A118.9 (19)
O5—Mn1—O3120.28 (6)C7ii—O1—Mn1125.12 (12)
O5—Mn1—C929.11 (6)O5—C9—Mn157.34 (10)
O5—Mn1—C8120.84 (6)O5—C9—C5iii118.80 (17)
O5—Mn1—O4109.33 (6)O6—C9—Mn164.46 (10)
O6—Mn1—C928.73 (5)O6—C9—O5121.60 (18)
O6—Mn1—C8112.34 (6)O6—C9—C5iii119.56 (17)
O3—Mn1—O6139.65 (5)C5iii—C9—Mn1172.51 (13)
O3—Mn1—C9137.68 (6)C3—C4—C5120.47 (17)
O3—Mn1—C829.19 (5)O3—C8—Mn159.84 (9)
O3—Mn1—O458.26 (5)O3—C8—O4121.50 (17)
O2—Mn1—O5141.88 (5)O3—C8—C3119.59 (17)
O2—Mn1—O693.04 (5)O4—C8—Mn162.21 (10)
O2—Mn1—O397.82 (5)O4—C8—C3118.90 (17)
O2—Mn1—O198.22 (5)C3—C8—Mn1171.43 (13)
O2—Mn1—C9117.78 (6)C6iv—C5—C9v121.02 (16)
O2—Mn1—C891.42 (5)C6iv—C5—C4119.44 (17)
O2—Mn1—O488.68 (5)C4—C5—C9v119.48 (17)
O1—Mn1—O587.57 (5)O2—C7—C1118.00 (16)
O1—Mn1—O6132.48 (5)O1ii—C7—O2123.32 (17)
O1—Mn1—O384.22 (5)O1ii—C7—C1118.64 (16)
O1—Mn1—C9110.49 (5)C8—O4—Mn188.55 (11)
O1—Mn1—C8113.34 (6)C13A—C12A—N1A109.7 (13)
O1—Mn1—O4142.46 (5)C13—N2—C14126.5 (3)
C8—Mn1—C9122.00 (6)C11—N2—C13107.7 (3)
O4—Mn1—O683.42 (5)C11—N2—C14125.8 (3)
O4—Mn1—C998.25 (5)C12A—N1A—C10A130.3 (16)
O4—Mn1—C829.24 (5)C11A—N1A—C10A118.7 (19)
C9—O5—Mn193.55 (12)C11A—N1A—C12A110.9 (15)
C9—O6—Mn186.81 (11)C15A—C14A—N2A111 (3)
C8—O3—Mn190.97 (11)N2—C11—N1110.4 (3)
C7—O2—Mn1110.40 (11)N1A—C11A—N2A102.8 (18)
C1—C6—C5i120.49 (17)C12A—C13A—N2A102.8 (15)
C13—C12—N1108.1 (5)C3—C2—C1iv120.54 (17)
C12—C13—N2107.0 (3)C6—C1—C7121.00 (16)
N2—C14—C15110.5 (3)C6—C1—C2i119.44 (17)
C12—N1—C10125.5 (5)C2i—C1—C7119.55 (16)
C11—N1—C12106.7 (5)C4—C3—C8120.24 (17)
C11—N1—C10127.7 (4)C2—C3—C4119.47 (17)
C11A—N2A—C14A128 (2)C2—C3—C8120.29 (17)
C11A—N2A—C13A113.3 (18)
Symmetry codes: (i) x+1, y+1/2, z+3/2; (ii) x+1, y+1, z+1; (iii) x+3/2, y+1, z1/2; (iv) x+1, y1/2, z+3/2; (v) x+3/2, y+1, z+1/2.
(A200k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.621 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.7107 Å
Orthorhombic, PbcaCell parameters from 16059 reflections
a = 14.77158 (16) Åθ = 1.6–27.8°
b = 12.42598 (11) ŵ = 0.90 mm1
c = 16.62769 (16) ÅT = 200 K
V = 3052.03 (5) Å3Prismatic, colorless
Z = 80.15 × 0.1 × 0.1 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3642 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2904 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.056
Detector resolution: 10.3590 pixels mm-1θmax = 27.9°, θmin = 2.5°
ω scansh = 1919
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1616
Tmin = 0.961, Tmax = 1.000l = 2121
65078 measured reflections
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)] = 0.032Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.072H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0208P)2 + 2.6647P]
where P = (Fo2 + 2Fc2)/3
3642 reflections(Δ/σ)max = 0.001
252 parametersΔρmax = 0.31 e Å3
310 restraintsΔρmin = 0.35 e Å3
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*/UeqOcc. (<1)
Mn10.60476 (2)0.48355 (2)0.57927 (2)0.01867 (8)
O50.70911 (11)0.48089 (11)0.48541 (9)0.0403 (4)
O60.69819 (11)0.63237 (11)0.55128 (8)0.0359 (4)
O30.59329 (10)0.34818 (11)0.66732 (8)0.0310 (3)
O20.49845 (9)0.58148 (10)0.62566 (7)0.0246 (3)
C60.34726 (12)0.78084 (14)0.53932 (11)0.0217 (4)
H60.34300.75420.48720.026*
C120.3434 (4)0.2387 (4)0.7748 (3)0.0555 (12)0.867 (4)
H120.32430.16820.78270.067*0.867 (4)
C100.3918 (3)0.2209 (4)0.6302 (3)0.0713 (11)0.867 (4)
H10A0.42760.15790.64090.107*0.867 (4)
H10B0.42270.26560.59190.107*0.867 (4)
H10C0.33420.19970.60870.107*0.867 (4)
C130.3420 (2)0.3179 (3)0.8300 (2)0.0554 (10)0.867 (4)
H130.32190.31230.88290.066*0.867 (4)
C140.3879 (2)0.5157 (3)0.8298 (3)0.0680 (11)0.867 (4)
H14A0.32910.54800.83940.082*0.867 (4)
H14B0.42120.56210.79340.082*0.867 (4)
C10A0.347 (3)0.383 (3)0.8991 (15)0.134 (14)*0.133 (4)
H10D0.40230.37470.92910.202*0.133 (4)
H10E0.30260.33360.91850.202*0.133 (4)
H10F0.32520.45560.90560.202*0.133 (4)
C15A0.461 (3)0.147 (5)0.628 (3)0.23 (3)*0.133 (4)
H15D0.48290.11180.67530.351*0.133 (4)
H15E0.50020.20610.61450.351*0.133 (4)
H15F0.45960.09690.58400.351*0.133 (4)
N10.3782 (5)0.2804 (4)0.7044 (3)0.0525 (14)0.867 (4)
N2A0.374 (4)0.270 (2)0.7090 (16)0.043 (8)*0.133 (4)
O10.52509 (9)0.38039 (10)0.50320 (7)0.0246 (3)
C90.73148 (13)0.57772 (15)0.49609 (11)0.0244 (4)
C40.69506 (12)0.41174 (14)0.86066 (10)0.0213 (4)
H40.72560.47440.84660.026*
C80.63627 (12)0.40077 (14)0.71923 (11)0.0219 (4)
C50.70289 (12)0.37115 (14)0.93850 (10)0.0211 (4)
C70.46217 (12)0.63685 (13)0.57053 (10)0.0193 (4)
O40.67367 (10)0.48897 (11)0.70250 (8)0.0303 (3)
C12A0.3917 (19)0.4265 (17)0.7518 (13)0.050 (6)*0.133 (4)
H12A0.40330.49980.75640.060*0.133 (4)
C150.4390 (3)0.5060 (4)0.9090 (3)0.0893 (14)0.867 (4)
H15A0.49870.47860.89890.134*0.867 (4)
H15B0.40720.45780.94410.134*0.867 (4)
H15C0.44330.57560.93380.134*0.867 (4)
N20.37619 (16)0.4095 (2)0.7932 (2)0.0501 (7)0.867 (4)
N1A0.3648 (14)0.3625 (17)0.8132 (11)0.044 (5)*0.133 (4)
C14A0.367 (3)0.189 (3)0.643 (2)0.101 (15)*0.133 (4)
H14C0.34260.22240.59490.121*0.133 (4)
H14D0.32680.13070.65870.121*0.133 (4)
C110.3967 (2)0.3838 (3)0.7191 (3)0.0477 (8)0.867 (4)
H110.42100.43120.68160.057*0.867 (4)
C11A0.354 (3)0.261 (2)0.7874 (15)0.035 (7)*0.133 (4)
H11A0.33640.20090.81650.042*0.133 (4)
C13A0.3993 (16)0.3695 (16)0.6831 (11)0.034 (5)*0.133 (4)
H13A0.41710.39190.63220.040*0.133 (4)
C20.59283 (12)0.26833 (14)0.82635 (10)0.0207 (4)
H20.55750.23260.78850.025*
C10.40377 (12)0.73029 (14)0.59484 (10)0.0196 (4)
C30.64164 (12)0.35903 (14)0.80374 (10)0.0195 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.02312 (14)0.01875 (13)0.01415 (13)0.00047 (11)0.00189 (11)0.00097 (10)
O50.0509 (10)0.0312 (7)0.0389 (9)0.0196 (7)0.0186 (7)0.0071 (7)
O60.0470 (9)0.0314 (7)0.0293 (7)0.0055 (7)0.0187 (7)0.0006 (6)
O30.0432 (9)0.0326 (7)0.0171 (6)0.0063 (6)0.0073 (6)0.0045 (6)
O20.0289 (7)0.0234 (6)0.0214 (7)0.0076 (5)0.0023 (5)0.0006 (5)
C60.0269 (10)0.0218 (8)0.0165 (9)0.0008 (7)0.0021 (7)0.0014 (7)
C120.035 (2)0.044 (2)0.088 (3)0.0001 (19)0.006 (2)0.0335 (19)
C100.050 (2)0.065 (2)0.099 (3)0.009 (2)0.006 (2)0.019 (2)
C130.0340 (16)0.0499 (18)0.082 (2)0.0039 (14)0.0050 (15)0.0376 (19)
C140.0406 (18)0.0503 (17)0.113 (3)0.0021 (14)0.0153 (18)0.0087 (18)
N10.0288 (18)0.0419 (18)0.087 (3)0.0046 (13)0.0019 (13)0.0307 (14)
O10.0305 (7)0.0255 (7)0.0178 (6)0.0003 (6)0.0024 (5)0.0044 (5)
C90.0260 (10)0.0273 (9)0.0199 (9)0.0036 (8)0.0008 (7)0.0037 (7)
C40.0214 (9)0.0202 (8)0.0224 (9)0.0021 (7)0.0006 (7)0.0025 (7)
C80.0214 (9)0.0243 (9)0.0200 (9)0.0025 (7)0.0002 (7)0.0047 (7)
C50.0210 (9)0.0231 (9)0.0193 (9)0.0014 (7)0.0023 (7)0.0017 (7)
C70.0199 (8)0.0179 (8)0.0203 (9)0.0016 (7)0.0017 (7)0.0024 (7)
O40.0362 (8)0.0287 (7)0.0260 (7)0.0068 (6)0.0047 (6)0.0109 (6)
C150.059 (2)0.105 (3)0.104 (3)0.009 (2)0.020 (2)0.027 (3)
N20.0279 (13)0.0461 (14)0.076 (2)0.0003 (11)0.0089 (12)0.0284 (14)
C110.0248 (14)0.0420 (17)0.076 (3)0.0050 (13)0.0037 (19)0.0288 (18)
C20.0225 (9)0.0219 (9)0.0176 (8)0.0011 (7)0.0028 (7)0.0009 (7)
C10.0215 (9)0.0184 (8)0.0190 (8)0.0011 (7)0.0006 (7)0.0012 (6)
C30.0207 (9)0.0207 (8)0.0172 (8)0.0011 (7)0.0009 (7)0.0022 (7)
Geometric parameters (Å, º) top
Mn1—O52.1939 (15)N1—C111.336 (6)
Mn1—O62.3540 (14)N2A—C14A1.489 (19)
Mn1—O32.2364 (13)N2A—C11A1.340 (19)
Mn1—O22.1311 (13)N2A—C13A1.367 (19)
Mn1—O12.1512 (13)O1—C7ii1.259 (2)
Mn1—C92.6051 (19)C9—C5iii1.503 (2)
Mn1—C82.5866 (18)C4—C51.394 (2)
Mn1—O42.2889 (13)C4—C31.396 (2)
O5—C91.260 (2)C8—O41.258 (2)
O6—C91.243 (2)C8—C31.500 (2)
O3—C81.255 (2)C5—C6iv1.394 (2)
O2—C71.265 (2)C5—C9v1.503 (2)
C6—C5i1.394 (2)C7—O1ii1.259 (2)
C6—C11.394 (2)C7—C11.502 (2)
C12—C131.347 (6)C12A—N1A1.354 (17)
C12—N11.380 (5)C12A—C13A1.349 (13)
C10—N11.453 (6)N2—C111.309 (5)
C13—N21.387 (4)N1A—C11A1.337 (18)
C14—C151.522 (5)C2—C1iv1.394 (2)
C14—N21.464 (4)C2—C31.390 (2)
C10A—N1A1.474 (18)C1—C2i1.394 (2)
C15A—C14A1.51 (2)
O5—Mn1—O657.26 (5)C13A—N2A—C14A113 (2)
O5—Mn1—O3120.50 (6)C7ii—O1—Mn1126.33 (12)
O5—Mn1—C928.86 (5)O5—C9—Mn157.16 (10)
O5—Mn1—C8120.50 (6)O5—C9—C5iii118.86 (17)
O5—Mn1—O4108.95 (6)O6—C9—Mn164.48 (10)
O6—Mn1—C928.46 (5)O6—C9—O5121.46 (17)
O6—Mn1—C8112.63 (6)O6—C9—C5iii119.63 (17)
O3—Mn1—O6139.88 (5)C5iii—C9—Mn1172.44 (13)
O3—Mn1—C9137.72 (6)C5—C4—C3120.45 (16)
O3—Mn1—C829.02 (5)O3—C8—Mn159.82 (9)
O3—Mn1—O457.98 (5)O3—C8—O4121.56 (17)
O2—Mn1—O5141.61 (6)O3—C8—C3119.40 (16)
O2—Mn1—O693.15 (5)O4—C8—Mn162.21 (9)
O2—Mn1—O397.86 (5)O4—C8—C3119.02 (16)
O2—Mn1—O198.63 (5)C3—C8—Mn1171.84 (13)
O2—Mn1—C9117.72 (6)C6iv—C5—C9v120.95 (16)
O2—Mn1—C891.95 (5)C4—C5—C6iv119.52 (16)
O2—Mn1—O489.25 (5)C4—C5—C9v119.47 (16)
O1—Mn1—O587.54 (5)O2—C7—C1117.95 (15)
O1—Mn1—O6132.27 (5)O1ii—C7—O2123.35 (16)
O1—Mn1—O383.99 (5)O1ii—C7—C1118.66 (15)
O1—Mn1—C9110.40 (5)C8—O4—Mn188.69 (11)
O1—Mn1—C8112.99 (5)C13A—C12A—N1A110.8 (18)
O1—Mn1—O4141.92 (5)C13—N2—C14126.8 (4)
C8—Mn1—C9121.80 (6)C11—N2—C13107.4 (3)
O4—Mn1—O683.86 (5)C11—N2—C14125.8 (3)
O4—Mn1—C998.19 (5)C12A—N1A—C10A133 (2)
O4—Mn1—C829.10 (5)C11A—N1A—C10A117 (3)
C9—O5—Mn193.99 (12)C11A—N1A—C12A110.2 (18)
C9—O6—Mn187.06 (11)N2A—C14A—C15A107 (4)
C8—O3—Mn191.16 (11)N2—C11—N1111.1 (3)
C7—O2—Mn1111.13 (11)N1A—C11A—N2A102 (2)
C1—C6—C5i120.37 (16)C12A—C13A—N2A100.7 (19)
C13—C12—N1108.1 (4)C3—C2—C1iv120.71 (16)
C12—C13—N2107.0 (3)C6—C1—C7120.93 (15)
N2—C14—C15110.3 (3)C2i—C1—C6119.43 (16)
C12—N1—C10125.5 (4)C2i—C1—C7119.63 (16)
C11—N1—C12106.4 (5)C4—C3—C8120.19 (16)
C11—N1—C10128.1 (5)C2—C3—C4119.37 (16)
C11A—N2A—C14A131 (3)C2—C3—C8120.44 (16)
C11A—N2A—C13A116 (2)
Symmetry codes: (i) x+1, y+1/2, z+3/2; (ii) x+1, y+1, z+1; (iii) x+3/2, y+1, z1/2; (iv) x+1, y1/2, z+3/2; (v) x+3/2, y+1, z+1/2.
(A293k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.6 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.7107 Å
Orthorhombic, PbcaCell parameters from 18118 reflections
a = 14.92869 (16) Åθ = 1.6–27.0°
b = 12.49901 (11) ŵ = 0.89 mm1
c = 16.58142 (15) ÅT = 293 K
V = 3093.99 (5) Å3Prismatic, colorless
Z = 80.15 × 0.1 × 0.1 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3410 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2721 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.059
Detector resolution: 10.3590 pixels mm-1θmax = 27.1°, θmin = 2.5°
ω scansh = 1919
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.36.20 (release 27-06-2012 CrysAlis171 .NET) (compiled Jul 11 2012,15:38:31) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
k = 1616
Tmin = 0.961, Tmax = 1.000l = 2121
83298 measured reflections
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)] = 0.033Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.085H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0296P)2 + 2.6174P]
where P = (Fo2 + 2Fc2)/3
3410 reflections(Δ/σ)max = 0.001
252 parametersΔρmax = 0.44 e Å3
308 restraintsΔρmin = 0.33 e Å3
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*/UeqOcc. (<1)
Mn10.60410 (2)0.48591 (2)0.58143 (2)0.02605 (10)
O50.70823 (14)0.48420 (14)0.48821 (12)0.0592 (5)
O60.69846 (13)0.63408 (14)0.55358 (11)0.0544 (5)
O30.59201 (12)0.35245 (13)0.67052 (9)0.0456 (4)
O20.49855 (10)0.58519 (12)0.62365 (9)0.0354 (4)
C60.34702 (14)0.78080 (16)0.53671 (12)0.0305 (5)
H60.34240.75350.48470.037*
C120.3428 (4)0.2416 (5)0.7722 (4)0.0802 (17)0.873 (5)
H120.32490.17140.78130.096*0.873 (5)
C100.3904 (4)0.2203 (5)0.6267 (4)0.1069 (18)0.873 (5)
H10A0.43280.16410.63690.160*0.873 (5)
H10B0.41330.26670.58540.160*0.873 (5)
H10C0.33470.18970.60920.160*0.873 (5)
C130.3408 (3)0.3208 (4)0.8264 (3)0.0828 (15)0.873 (5)
H130.32100.31610.87940.099*0.873 (5)
C140.3846 (3)0.5189 (4)0.8221 (4)0.120 (2)0.873 (5)
H14A0.32620.55020.83190.144*0.873 (5)
H14B0.41650.56430.78430.144*0.873 (5)
C10A0.347 (3)0.390 (4)0.8942 (17)0.155 (19)*0.127 (5)
H10D0.40210.38070.92370.233*0.127 (5)
H10E0.30250.34250.91560.233*0.127 (5)
H10F0.32720.46240.89910.233*0.127 (5)
C15A0.467 (4)0.148 (7)0.640 (5)0.30 (4)*0.127 (5)
H15D0.47650.12230.58640.456*0.127 (5)
H15E0.47580.09130.67800.456*0.127 (5)
H15F0.50760.20550.65140.456*0.127 (5)
N10.3760 (5)0.2814 (4)0.7003 (4)0.0801 (17)0.873 (5)
N2A0.379 (3)0.273 (2)0.7110 (14)0.035 (6)*0.127 (5)
O10.52765 (11)0.38079 (12)0.50551 (8)0.0351 (4)
C90.73146 (15)0.57952 (18)0.49881 (13)0.0353 (5)
C40.69402 (14)0.41214 (16)0.86382 (12)0.0296 (4)
H40.72450.47440.84980.036*
C80.63408 (14)0.40394 (17)0.72266 (13)0.0309 (4)
C50.70263 (14)0.37062 (17)0.94150 (12)0.0299 (4)
C70.46131 (13)0.63850 (15)0.56818 (12)0.0266 (4)
O40.67059 (12)0.49162 (13)0.70615 (10)0.0453 (4)
C12A0.391 (2)0.429 (2)0.7490 (16)0.064 (8)*0.127 (5)
H12A0.40210.50240.75370.077*0.127 (5)
C150.4373 (4)0.5117 (6)0.9019 (5)0.172 (3)0.873 (5)
H15A0.49710.48720.89120.258*0.873 (5)
H15B0.40800.46230.93750.258*0.873 (5)
H15C0.43960.58100.92670.258*0.873 (5)
N20.3742 (2)0.4115 (3)0.7880 (3)0.0781 (11)0.873 (5)
N1A0.3623 (18)0.365 (2)0.8105 (13)0.055 (6)*0.127 (5)
C14A0.372 (4)0.189 (3)0.647 (3)0.116 (19)*0.127 (5)
H14C0.35080.21940.59690.139*0.127 (5)
H14D0.33100.13250.66380.139*0.127 (5)
C110.3941 (3)0.3837 (4)0.7147 (4)0.0733 (12)0.873 (5)
H110.41840.43000.67660.088*0.873 (5)
C11A0.354 (3)0.264 (2)0.7873 (15)0.038 (7)*0.127 (5)
H11A0.33630.20370.81630.045*0.127 (5)
C13A0.401 (2)0.3718 (19)0.6803 (13)0.046 (7)*0.127 (5)
H13A0.41750.39270.62860.056*0.127 (5)
C20.59214 (14)0.27078 (16)0.82931 (12)0.0285 (4)
H20.55660.23610.79140.034*
C10.40353 (13)0.73162 (16)0.59233 (12)0.0270 (4)
C30.64023 (14)0.36115 (16)0.80707 (12)0.0276 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Mn10.03163 (18)0.02672 (16)0.01979 (16)0.00084 (13)0.00259 (13)0.00153 (12)
O50.0742 (13)0.0476 (10)0.0559 (11)0.0292 (9)0.0273 (10)0.0097 (9)
O60.0705 (13)0.0472 (10)0.0454 (10)0.0081 (9)0.0316 (9)0.0006 (8)
O30.0647 (12)0.0468 (9)0.0252 (8)0.0114 (8)0.0123 (8)0.0090 (7)
O20.0419 (9)0.0343 (8)0.0299 (8)0.0122 (7)0.0029 (7)0.0006 (6)
C60.0382 (12)0.0301 (10)0.0232 (10)0.0038 (9)0.0052 (9)0.0039 (8)
C120.051 (3)0.063 (3)0.126 (4)0.002 (2)0.008 (3)0.049 (2)
C100.086 (4)0.088 (3)0.147 (5)0.012 (3)0.014 (3)0.032 (3)
C130.055 (2)0.073 (3)0.120 (4)0.006 (2)0.005 (2)0.048 (3)
C140.074 (3)0.076 (3)0.209 (6)0.013 (2)0.035 (3)0.000 (3)
N10.049 (2)0.063 (2)0.128 (4)0.0103 (16)0.003 (2)0.049 (2)
O10.0440 (9)0.0361 (8)0.0252 (8)0.0001 (7)0.0025 (7)0.0065 (6)
C90.0363 (12)0.0395 (12)0.0300 (11)0.0044 (10)0.0049 (9)0.0045 (9)
C40.0304 (11)0.0287 (10)0.0299 (11)0.0038 (9)0.0010 (9)0.0026 (8)
C80.0296 (11)0.0352 (11)0.0279 (10)0.0021 (9)0.0012 (8)0.0073 (9)
C50.0306 (11)0.0326 (11)0.0264 (10)0.0027 (9)0.0054 (8)0.0001 (8)
C70.0264 (10)0.0257 (9)0.0278 (11)0.0013 (8)0.0021 (8)0.0030 (8)
O40.0570 (11)0.0417 (9)0.0371 (9)0.0117 (8)0.0082 (8)0.0164 (7)
C150.090 (4)0.193 (7)0.233 (7)0.019 (4)0.024 (4)0.087 (6)
N20.0422 (18)0.068 (2)0.124 (3)0.0029 (15)0.0175 (19)0.040 (2)
C110.0338 (18)0.061 (2)0.125 (4)0.0085 (18)0.013 (3)0.045 (2)
C20.0319 (11)0.0293 (10)0.0243 (10)0.0026 (8)0.0052 (8)0.0006 (8)
C10.0306 (10)0.0261 (10)0.0242 (10)0.0014 (8)0.0018 (8)0.0006 (8)
C30.0293 (10)0.0300 (10)0.0236 (10)0.0014 (8)0.0019 (8)0.0034 (8)
Geometric parameters (Å, º) top
Mn1—O52.1923 (18)N1—C111.328 (7)
Mn1—O62.3723 (17)N2A—C14A1.49 (2)
Mn1—O32.2355 (16)N2A—C11A1.324 (19)
Mn1—O22.1243 (15)N2A—C13A1.378 (19)
Mn1—O12.1479 (15)O1—C7ii1.256 (2)
Mn1—C92.619 (2)C9—C5iii1.503 (3)
Mn1—C82.595 (2)C4—C51.395 (3)
Mn1—O42.2951 (17)C4—C31.392 (3)
O5—C91.253 (3)C8—O41.254 (3)
O6—C91.238 (3)C8—C31.501 (3)
O3—C81.247 (3)C5—C6iv1.393 (3)
O2—C71.265 (2)C5—C9v1.503 (3)
C6—C5i1.393 (3)C7—O1ii1.256 (2)
C6—C11.393 (3)C7—C11.503 (3)
C12—C131.337 (8)C12A—N1A1.366 (18)
C12—N11.382 (6)C12A—C13A1.356 (18)
C10—N11.457 (7)N2—C111.299 (7)
C13—N21.392 (5)N1A—C11A1.331 (19)
C14—C151.542 (9)C2—C1iv1.390 (3)
C14—N21.465 (6)C2—C31.388 (3)
C10A—N1A1.439 (19)C1—C2i1.390 (3)
C15A—C14A1.51 (5)
O5—Mn1—O656.58 (6)C13A—N2A—C14A113 (3)
O5—Mn1—O3121.06 (7)C7ii—O1—Mn1128.16 (14)
O5—Mn1—C928.46 (7)O5—C9—Mn156.48 (12)
O5—Mn1—C8120.67 (8)O5—C9—C5iii119.1 (2)
O5—Mn1—O4109.21 (8)O6—C9—Mn164.75 (12)
O6—Mn1—C928.16 (6)O6—C9—O5121.1 (2)
O6—Mn1—C8112.42 (7)O6—C9—C5iii119.7 (2)
O3—Mn1—O6139.39 (7)C5iii—C9—Mn1172.29 (16)
O3—Mn1—C9137.52 (7)C3—C4—C5120.48 (19)
O3—Mn1—C828.72 (6)O3—C8—Mn159.43 (11)
O3—Mn1—O457.50 (6)O3—C8—O4121.2 (2)
O2—Mn1—O5139.81 (7)O3—C8—C3119.54 (19)
O2—Mn1—O692.78 (6)O4—C8—Mn162.16 (11)
O2—Mn1—O399.10 (6)O4—C8—C3119.23 (19)
O2—Mn1—O198.99 (6)C3—C8—Mn1173.03 (15)
O2—Mn1—C9116.73 (7)C6iv—C5—C9v121.23 (19)
O2—Mn1—C893.51 (6)C6iv—C5—C4119.37 (19)
O2—Mn1—O490.33 (6)C4—C5—C9v119.34 (19)
O1—Mn1—O587.57 (6)O2—C7—C1117.81 (17)
O1—Mn1—O6132.76 (6)O1ii—C7—O2123.27 (19)
O1—Mn1—O383.57 (6)O1ii—C7—C1118.89 (18)
O1—Mn1—C9110.63 (6)C8—O4—Mn188.94 (13)
O1—Mn1—C8112.28 (6)C13A—C12A—N1A110 (2)
O1—Mn1—O4140.99 (6)C13—N2—C14127.4 (5)
C8—Mn1—C9121.54 (7)C11—N2—C13107.0 (4)
O4—Mn1—O683.93 (6)C11—N2—C14125.6 (5)
O4—Mn1—C998.25 (7)C12A—N1A—C10A130 (3)
O4—Mn1—C828.90 (6)C11A—N1A—C10A118 (3)
C9—O5—Mn195.05 (14)C11A—N1A—C12A112 (2)
C9—O6—Mn187.08 (14)N2A—C14A—C15A103 (5)
C8—O3—Mn191.85 (13)N2—C11—N1112.2 (5)
C7—O2—Mn1113.22 (13)N2A—C11A—N1A100 (2)
C1—C6—C5i120.41 (19)C12A—C13A—N2A98.2 (19)
C13—C12—N1108.7 (5)C3—C2—C1iv120.72 (19)
C12—C13—N2106.7 (5)C6—C1—C7120.85 (18)
N2—C14—C15109.4 (5)C2i—C1—C6119.46 (18)
C12—N1—C10125.9 (6)C2i—C1—C7119.67 (18)
C11—N1—C12105.4 (6)C4—C3—C8120.16 (18)
C11—N1—C10128.7 (6)C2—C3—C4119.43 (18)
C11A—N2A—C14A126 (3)C2—C3—C8120.40 (18)
C11A—N2A—C13A120 (2)
Symmetry codes: (i) x+1, y+1/2, z+3/2; (ii) x+1, y+1, z+1; (iii) x+3/2, y+1, z1/2; (iv) x+1, y1/2, z+3/2; (v) x+3/2, y+1, z+1/2.
(c100k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.643 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 2242 reflections
a = 14.6452 (4) Åθ = 2.4–29.3°
b = 12.3672 (4) ŵ = 0.91 mm1
c = 16.6648 (5) ÅT = 100 K
V = 3018.33 (16) Å3Prism, colorless
Z = 80.15 × 0.11 × 0.07 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3611 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2412 reflections with I > 2σ(I)
Detector resolution: 10.3590 pixels mm-1Rint = 0.061
ω scansθmax = 29.3°, θmin = 2.4°
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1418
Tmin = 0.977, Tmax = 1.000k = 1612
10796 measured reflectionsl = 1922
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)] = 0.055Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.117H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0362P)2 + 0.987P]
where P = (Fo2 + 2Fc2)/3
3611 reflections(Δ/σ)max = 0.001
254 parametersΔρmax = 0.57 e Å3
308 restraintsΔρmin = 0.57 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O40.67534 (15)0.48793 (17)0.70085 (13)0.0211 (5)
O50.70950 (15)0.47909 (18)0.48389 (14)0.0249 (6)
O30.59521 (15)0.34538 (17)0.66611 (13)0.0237 (5)
O60.69875 (15)0.63023 (17)0.55109 (13)0.0239 (5)
C90.7314 (2)0.5737 (3)0.49452 (18)0.0158 (6)
C80.63842 (19)0.3976 (2)0.71656 (18)0.0145 (6)
C30.6427 (2)0.3582 (2)0.80239 (18)0.0160 (7)
O20.49864 (14)0.57963 (16)0.62623 (12)0.0169 (5)
N1A0.370 (4)0.268 (3)0.701 (2)0.041 (11)*0.179 (6)
C110.3976 (3)0.3836 (5)0.7212 (4)0.0303 (11)0.821 (6)
H110.42140.43220.68230.036*0.821 (6)
C100.3927 (5)0.2209 (6)0.6330 (4)0.0450 (15)0.821 (6)
H10D0.33330.19690.61260.067*0.821 (6)
H10E0.43160.15790.64270.067*0.821 (6)
H10F0.42180.26820.59340.067*0.821 (6)
C120.3436 (7)0.2363 (7)0.7774 (5)0.0379 (18)0.821 (6)
H120.32310.16420.78510.046*0.821 (6)
C130.3433 (3)0.3161 (4)0.8317 (3)0.0378 (13)0.821 (6)
H130.32300.31020.88570.045*0.821 (6)
C140.3891 (3)0.5158 (4)0.8330 (3)0.0416 (13)0.821 (6)
H14C0.32830.54800.84310.050*0.821 (6)
H14D0.42280.56440.79630.050*0.821 (6)
C150.4400 (4)0.5063 (5)0.9105 (3)0.0529 (16)0.821 (6)
H15D0.49950.47260.90070.079*0.821 (6)
H15E0.40490.46160.94800.079*0.821 (6)
H15F0.44890.57840.93350.079*0.821 (6)
Mn10.60517 (3)0.48140 (4)0.57834 (3)0.01355 (15)
C70.4630 (2)0.6366 (2)0.57131 (18)0.0141 (6)
C60.3478 (2)0.7816 (2)0.54075 (18)0.0169 (7)
H60.34420.75540.48730.020*
C10.4037 (2)0.7297 (2)0.59605 (18)0.0149 (7)
C50.7030 (2)0.3719 (2)0.93676 (18)0.0161 (7)
C20.5933 (2)0.2670 (2)0.82546 (18)0.0155 (7)
H20.55710.22990.78700.019*
C40.6959 (2)0.4119 (2)0.85911 (18)0.0169 (7)
H40.72740.47610.84460.020*
O10.52298 (14)0.37976 (16)0.50259 (12)0.0171 (5)
N2A0.3647 (15)0.3603 (19)0.8094 (11)0.031 (6)*0.179 (6)
C12A0.4020 (18)0.3697 (18)0.6809 (14)0.033 (6)*0.179 (6)
H12A0.42230.39430.62990.039*0.179 (6)
C13A0.3978 (19)0.4266 (19)0.7499 (15)0.034 (7)*0.179 (6)
H13A0.41480.50020.75640.041*0.179 (6)
C14A0.3395 (19)0.378 (3)0.8925 (13)0.071 (9)*0.179 (6)
H14A0.30600.31420.91240.085*0.179 (6)
H14B0.29730.44090.89510.085*0.179 (6)
C15A0.418 (3)0.399 (4)0.946 (2)0.15 (2)*0.179 (6)
H15A0.47420.37140.92150.231*0.179 (6)
H15B0.40820.36320.99780.231*0.179 (6)
H15C0.42450.47740.95500.231*0.179 (6)
N10.3798 (7)0.2800 (6)0.7077 (5)0.0335 (17)0.821 (6)
N20.3780 (3)0.4101 (4)0.7954 (3)0.0330 (11)0.821 (6)
C10A0.374 (3)0.185 (3)0.637 (3)0.089 (19)*0.179 (6)
H10A0.35870.21850.58520.133*0.179 (6)
H10B0.33030.12780.64900.133*0.179 (6)
H10C0.43580.15490.63420.133*0.179 (6)
C11A0.354 (3)0.260 (2)0.7805 (19)0.033 (10)*0.179 (6)
H11A0.33920.19630.80980.040*0.179 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O40.0243 (12)0.0215 (12)0.0176 (11)0.0047 (10)0.0031 (10)0.0057 (9)
O50.0307 (13)0.0214 (12)0.0226 (12)0.0060 (10)0.0113 (11)0.0027 (10)
O30.0365 (14)0.0188 (12)0.0158 (11)0.0045 (10)0.0016 (11)0.0026 (9)
O60.0294 (13)0.0228 (13)0.0194 (12)0.0049 (10)0.0096 (11)0.0010 (10)
C90.0119 (15)0.0257 (17)0.0099 (14)0.0027 (12)0.0031 (12)0.0023 (13)
C80.0095 (15)0.0161 (16)0.0180 (15)0.0006 (12)0.0000 (13)0.0075 (12)
C30.0153 (16)0.0164 (16)0.0163 (14)0.0012 (12)0.0004 (13)0.0010 (12)
O20.0198 (11)0.0153 (11)0.0157 (11)0.0034 (9)0.0020 (9)0.0006 (9)
C110.014 (2)0.032 (3)0.045 (3)0.0007 (19)0.001 (2)0.020 (2)
C100.030 (3)0.047 (4)0.058 (3)0.004 (3)0.004 (3)0.013 (3)
C120.023 (3)0.029 (3)0.062 (4)0.004 (3)0.000 (2)0.025 (2)
C130.027 (3)0.033 (3)0.054 (3)0.001 (2)0.001 (2)0.029 (2)
C140.024 (3)0.034 (3)0.066 (3)0.0013 (19)0.007 (2)0.007 (2)
C150.038 (3)0.061 (4)0.060 (3)0.004 (3)0.012 (3)0.007 (3)
Mn10.0164 (3)0.0129 (3)0.0113 (2)0.00004 (19)0.0006 (2)0.00046 (19)
C70.0116 (15)0.0151 (16)0.0157 (15)0.0036 (11)0.0022 (13)0.0012 (13)
C60.0189 (16)0.0177 (17)0.0140 (15)0.0011 (13)0.0000 (14)0.0004 (13)
C10.0153 (16)0.0141 (16)0.0154 (15)0.0014 (12)0.0028 (13)0.0013 (12)
C50.0149 (16)0.0182 (17)0.0152 (15)0.0009 (13)0.0002 (13)0.0025 (13)
C20.0168 (16)0.0165 (16)0.0133 (15)0.0002 (12)0.0020 (14)0.0028 (13)
C40.0166 (16)0.0145 (16)0.0196 (15)0.0001 (12)0.0002 (13)0.0015 (13)
O10.0193 (12)0.0171 (12)0.0149 (11)0.0010 (9)0.0003 (10)0.0015 (9)
N10.016 (3)0.031 (3)0.054 (3)0.002 (2)0.006 (2)0.0183 (19)
N20.018 (2)0.028 (2)0.052 (3)0.0014 (16)0.0054 (18)0.0208 (18)
Geometric parameters (Å, º) top
O4—C81.269 (3)C12—C131.339 (9)
O4—Mn12.287 (2)C12—N11.386 (7)
O5—C91.226 (4)C13—N21.406 (6)
O5—Mn12.194 (2)C14—C151.495 (7)
O3—C81.234 (4)C14—N21.459 (6)
O3—Mn12.234 (2)Mn1—O12.150 (2)
O6—C91.267 (4)C7—C11.500 (4)
O6—Mn12.339 (2)C7—O1ii1.265 (3)
C9—Mn12.583 (3)C6—C11.390 (4)
C9—C5i1.517 (4)C6—C5iii1.393 (4)
C8—C31.512 (4)C1—C2iii1.388 (4)
C8—Mn12.572 (3)C5—C9iv1.517 (4)
C3—C21.394 (4)C5—C6v1.393 (4)
C3—C41.393 (4)C5—C41.389 (4)
O2—Mn12.132 (2)C2—C1v1.388 (4)
O2—C71.267 (3)O1—C7ii1.264 (3)
N1A—C12A1.378 (19)N2A—C13A1.374 (18)
N1A—C10A1.47 (2)N2A—C14A1.451 (18)
N1A—C11A1.36 (2)N2A—C11A1.342 (19)
C11—N11.327 (9)C12A—C13A1.350 (13)
C11—N21.310 (7)C14A—C15A1.485 (19)
C10—N11.456 (8)
C8—O4—Mn187.80 (18)C8—Mn1—C9121.79 (9)
C9—O5—Mn193.80 (19)O2—Mn1—O488.54 (8)
C8—O3—Mn191.08 (18)O2—Mn1—O5141.77 (8)
C9—O6—Mn186.08 (18)O2—Mn1—O397.82 (8)
O5—C9—O6122.3 (3)O2—Mn1—O693.04 (8)
O5—C9—Mn157.93 (16)O2—Mn1—C9118.32 (9)
O5—C9—C5i119.8 (3)O2—Mn1—C891.89 (9)
O6—C9—Mn164.61 (16)O2—Mn1—O198.23 (8)
O6—C9—C5i117.8 (3)O1—Mn1—O4142.78 (8)
C5i—C9—Mn1172.8 (2)O1—Mn1—O587.77 (8)
O4—C8—C3117.4 (3)O1—Mn1—O384.70 (8)
O4—C8—Mn162.67 (15)O1—Mn1—O6132.38 (8)
O3—C8—O4122.6 (3)O1—Mn1—C9109.98 (9)
O3—C8—C3119.8 (3)O1—Mn1—C8113.33 (9)
O3—C8—Mn160.26 (16)O2—C7—C1117.8 (3)
C3—C8—Mn1169.9 (2)O1ii—C7—O2123.2 (3)
C2—C3—C8120.0 (3)O1ii—C7—C1118.9 (3)
C4—C3—C8120.8 (3)C1—C6—C5iii120.4 (3)
C4—C3—C2119.2 (3)C6—C1—C7120.9 (3)
C7—O2—Mn1110.32 (18)C2iii—C1—C7119.7 (3)
C12A—N1A—C10A117 (3)C2iii—C1—C6119.3 (3)
C11A—N1A—C12A111 (3)C6v—C5—C9iv121.5 (3)
C11A—N1A—C10A131 (3)C4—C5—C9iv118.7 (3)
N2—C11—N1111.0 (5)C4—C5—C6v119.7 (3)
C13—C12—N1106.3 (7)C1v—C2—C3120.8 (3)
C12—C13—N2108.5 (6)C5—C4—C3120.3 (3)
N2—C14—C15110.9 (4)C7ii—O1—Mn1125.05 (19)
O4—Mn1—O683.24 (8)C13A—N2A—C14A133 (2)
O4—Mn1—C998.36 (9)C11A—N2A—C13A110 (2)
O4—Mn1—C829.53 (8)C11A—N2A—C14A117 (3)
O5—Mn1—O4109.15 (9)C13A—C12A—N1A105 (2)
O5—Mn1—O3120.36 (9)C12A—C13A—N2A109 (2)
O5—Mn1—O657.52 (8)N2A—C14A—C15A114 (3)
O5—Mn1—C928.27 (9)C11—N1—C10127.2 (6)
O5—Mn1—C8120.36 (9)C11—N1—C12108.0 (7)
O3—Mn1—O458.09 (8)C12—N1—C10124.8 (7)
O3—Mn1—O6139.27 (8)C11—N2—C13106.2 (5)
O3—Mn1—C9137.19 (9)C11—N2—C14127.2 (5)
O3—Mn1—C828.67 (8)C13—N2—C14126.6 (5)
O6—Mn1—C929.31 (8)N2A—C11A—N1A105 (2)
O6—Mn1—C8112.34 (9)
Symmetry codes: (i) x+3/2, y+1, z1/2; (ii) x+1, y+1, z+1; (iii) x+1, y+1/2, z+3/2; (iv) x+3/2, y+1, z+1/2; (v) x+1, y1/2, z+3/2.
(c160k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.634 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 2092 reflections
a = 14.7079 (5) Åθ = 2.4–29.3°
b = 12.3931 (4) ŵ = 0.91 mm1
c = 16.6458 (5) ÅT = 160 K
V = 3034.14 (17) Å3Prism, colorless
Z = 80.15 × 0.11 × 0.07 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3632 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2276 reflections with I > 2σ(I)
Detector resolution: 10.3590 pixels mm-1Rint = 0.064
ω scansθmax = 29.3°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1418
Tmin = 0.974, Tmax = 1.000k = 1216
10847 measured reflectionsl = 2219
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)] = 0.066Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.163H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0525P)2 + 6.2464P]
where P = (Fo2 + 2Fc2)/3
3632 reflections(Δ/σ)max = 0.002
212 parametersΔρmax = 0.88 e Å3
282 restraintsΔρmin = 0.61 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O20.49859 (19)0.5806 (2)0.62602 (17)0.0218 (6)
O30.5952 (2)0.3468 (2)0.66660 (18)0.0299 (7)
O10.52422 (19)0.3799 (2)0.50315 (16)0.0214 (6)
O40.6741 (2)0.4887 (2)0.70191 (17)0.0265 (7)
C70.4624 (3)0.6371 (3)0.5709 (2)0.0176 (8)
C20.5932 (3)0.2675 (3)0.8258 (2)0.0199 (9)
H20.55760.23050.78700.024*
C90.7313 (3)0.5746 (4)0.4951 (2)0.0209 (9)
C100.3911 (7)0.2212 (8)0.6321 (5)0.057 (2)*0.797 (7)
H10A0.43570.16360.64080.086*0.797 (7)
H10B0.41280.26940.58960.086*0.797 (7)
H10C0.33280.18940.61620.086*0.797 (7)
C11A0.3485 (15)0.2618 (18)0.7903 (12)0.014 (4)*0.203 (7)
H11A0.32420.20340.82050.016*0.203 (7)
C12A0.4002 (13)0.3676 (14)0.6852 (12)0.015 (4)*0.203 (7)
H12A0.41870.39400.63410.018*0.203 (7)
C13A0.3936 (17)0.4206 (17)0.7537 (13)0.030 (5)*0.203 (7)
H13A0.40660.49540.75870.036*0.203 (7)
C140.3884 (5)0.5157 (6)0.8324 (5)0.053 (2)*0.797 (7)
H14A0.32800.54800.84270.063*0.797 (7)
H14B0.42180.56390.79530.063*0.797 (7)
C150.4387 (6)0.5073 (7)0.9084 (5)0.068 (3)*0.797 (7)
H15A0.49850.47510.89830.102*0.797 (7)
H15B0.40460.46170.94590.102*0.797 (7)
H15C0.44650.57940.93160.102*0.797 (7)
O50.7093 (2)0.4809 (2)0.48469 (19)0.0337 (8)
C60.3472 (3)0.7812 (3)0.5403 (2)0.0196 (9)
H60.34280.75410.48700.023*
C50.7030 (3)0.3715 (3)0.9376 (2)0.0208 (9)
C40.6954 (3)0.4113 (3)0.8599 (2)0.0206 (9)
H40.72710.47520.84540.025*
C10.4036 (3)0.7302 (3)0.5953 (2)0.0185 (8)
C30.6424 (3)0.3592 (3)0.8034 (2)0.0202 (9)
C80.6377 (3)0.3984 (3)0.7175 (2)0.0195 (8)
N1A0.374 (3)0.2631 (18)0.7062 (15)0.048 (6)*0.203 (7)
C120.3451 (6)0.2363 (7)0.7739 (5)0.044 (2)*0.797 (7)
H120.32610.16360.78090.053*0.797 (7)
C130.3434 (5)0.3171 (6)0.8310 (4)0.0432 (18)*0.797 (7)
H130.32320.31030.88490.052*0.797 (7)
C14A0.345 (2)0.381 (3)0.8978 (15)0.095 (12)*0.203 (7)
H14C0.31680.31490.92080.114*0.203 (7)
H14D0.29880.43870.89960.114*0.203 (7)
C15A0.424 (3)0.413 (5)0.951 (2)0.146 (19)*0.203 (7)
H15D0.48070.38500.92790.219*0.203 (7)
H15E0.41530.38331.00470.219*0.203 (7)
H15F0.42720.49190.95390.219*0.203 (7)
N10.3794 (7)0.2817 (6)0.7054 (4)0.0418 (18)*0.797 (7)
C10A0.381 (5)0.184 (4)0.641 (3)0.14 (2)*0.203 (7)
H10D0.44550.16490.63380.208*0.203 (7)
H10E0.35710.21440.59170.208*0.203 (7)
H10F0.34690.11880.65570.208*0.203 (7)
C110.3966 (5)0.3849 (6)0.7216 (5)0.0388 (16)*0.797 (7)
H110.42070.43430.68360.047*0.797 (7)
N20.3768 (4)0.4102 (5)0.7950 (4)0.0402 (15)*0.797 (7)
N2A0.367 (2)0.360 (2)0.8152 (12)0.065 (6)*0.203 (7)
O60.6983 (2)0.6313 (2)0.55136 (18)0.0321 (8)
Mn10.60497 (4)0.48245 (5)0.57893 (4)0.0171 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O20.0258 (15)0.0208 (15)0.0187 (14)0.0047 (12)0.0009 (12)0.0014 (12)
O30.043 (2)0.0257 (16)0.0213 (15)0.0052 (14)0.0035 (14)0.0065 (13)
O10.0267 (16)0.0199 (15)0.0175 (14)0.0012 (12)0.0007 (13)0.0035 (12)
O40.0296 (16)0.0288 (17)0.0210 (14)0.0058 (13)0.0033 (13)0.0085 (12)
C70.0178 (19)0.017 (2)0.0183 (19)0.0022 (15)0.0007 (17)0.0026 (16)
C20.022 (2)0.020 (2)0.0182 (19)0.0000 (16)0.0027 (18)0.0020 (16)
C90.018 (2)0.029 (2)0.0157 (18)0.0011 (16)0.0013 (16)0.0045 (16)
O50.0411 (19)0.0280 (17)0.0319 (17)0.0119 (15)0.0170 (15)0.0033 (14)
C60.020 (2)0.020 (2)0.019 (2)0.0002 (16)0.0003 (17)0.0017 (17)
C50.020 (2)0.023 (2)0.0195 (19)0.0001 (17)0.0016 (17)0.0028 (16)
C40.021 (2)0.018 (2)0.0226 (19)0.0019 (16)0.0004 (17)0.0000 (16)
C10.018 (2)0.017 (2)0.021 (2)0.0015 (15)0.0008 (17)0.0009 (16)
C30.023 (2)0.019 (2)0.0189 (18)0.0002 (16)0.0019 (16)0.0030 (15)
C80.0139 (19)0.023 (2)0.0219 (18)0.0002 (15)0.0027 (16)0.0081 (15)
O60.0404 (19)0.0306 (17)0.0253 (16)0.0058 (14)0.0150 (15)0.0007 (13)
Mn10.0210 (3)0.0166 (3)0.0138 (3)0.0003 (2)0.0013 (3)0.0004 (2)
Geometric parameters (Å, º) top
O2—C71.271 (5)C14—C151.468 (11)
O2—Mn12.131 (3)C14—N21.458 (9)
O3—C81.231 (5)O5—Mn12.194 (3)
O3—Mn12.231 (3)C6—C5iv1.390 (6)
O1—C7i1.265 (5)C6—C11.388 (6)
O1—Mn12.149 (3)C5—C9v1.516 (6)
O4—C81.267 (5)C5—C6ii1.390 (6)
O4—Mn12.287 (3)C5—C41.389 (6)
C7—O1i1.265 (5)C4—C31.383 (6)
C7—C11.498 (5)C1—C2iv1.394 (5)
C2—C1ii1.394 (5)C3—C81.511 (6)
C2—C31.397 (6)C8—Mn12.576 (4)
C9—O51.218 (5)N1A—C10A1.464 (18)
C9—C5iii1.516 (6)C12—C131.380 (10)
C9—O61.268 (5)C12—N11.368 (10)
C9—Mn12.589 (4)C13—N21.390 (9)
C10—N11.443 (10)C14A—C15A1.513 (19)
C11A—N1A1.448 (18)C14A—N2A1.437 (18)
C11A—N2A1.310 (18)N1—C111.331 (10)
C12A—C13A1.320 (17)C11—N21.294 (9)
C12A—N1A1.398 (18)O6—Mn12.344 (3)
C13A—N2A1.331 (18)
C7—O2—Mn1110.8 (2)N2A—C14A—C15A116 (3)
C8—O3—Mn191.5 (2)C12—N1—C10122.4 (8)
C7i—O1—Mn1125.8 (3)C11—N1—C10130.4 (8)
C8—O4—Mn188.0 (2)C11—N1—C12107.3 (7)
O2—C7—C1118.0 (3)N2—C11—N1112.4 (7)
O1i—C7—O2123.2 (4)C13—N2—C14127.0 (7)
O1i—C7—C1118.8 (4)C11—N2—C14126.5 (7)
C1ii—C2—C3120.3 (4)C11—N2—C13106.5 (6)
O5—C9—C5iii120.0 (4)C11A—N2A—C13A110.2 (17)
O5—C9—O6122.1 (4)C11A—N2A—C14A115 (2)
O5—C9—Mn157.7 (2)C13A—N2A—C14A134 (3)
C5iii—C9—Mn1173.0 (3)C9—O6—Mn186.1 (2)
O6—C9—C5iii117.8 (4)O2—Mn1—O398.18 (12)
O6—C9—Mn164.6 (2)O2—Mn1—O198.49 (11)
N2A—C11A—N1A104.0 (17)O2—Mn1—O488.72 (11)
C13A—C12A—N1A102.9 (16)O2—Mn1—C9118.25 (13)
C12A—C13A—N2A113.8 (17)O2—Mn1—O5141.37 (12)
N2—C14—C15111.3 (7)O2—Mn1—C892.22 (12)
C9—O5—Mn194.4 (3)O2—Mn1—O693.01 (11)
C1—C6—C5iv120.6 (4)O3—Mn1—O457.89 (11)
C6ii—C5—C9v121.8 (4)O3—Mn1—C9136.98 (13)
C4—C5—C9v118.8 (4)O3—Mn1—C828.54 (12)
C4—C5—C6ii119.4 (4)O3—Mn1—O6139.35 (12)
C3—C4—C5120.8 (4)O1—Mn1—O384.42 (11)
C2iv—C1—C7119.5 (4)O1—Mn1—O4142.30 (11)
C6—C1—C7121.1 (4)O1—Mn1—C9109.94 (12)
C6—C1—C2iv119.4 (4)O1—Mn1—O587.79 (11)
C2—C3—C8119.3 (4)O1—Mn1—C8112.94 (12)
C4—C3—C2119.4 (4)O1—Mn1—O6132.37 (11)
C4—C3—C8121.3 (4)O4—Mn1—C998.55 (12)
O3—C8—O4122.1 (4)O4—Mn1—C829.45 (11)
O3—C8—C3120.5 (4)O4—Mn1—O683.60 (11)
O3—C8—Mn160.0 (2)O5—Mn1—O3120.40 (12)
O4—C8—C3117.3 (4)O5—Mn1—O4109.25 (12)
O4—C8—Mn162.5 (2)O5—Mn1—C927.98 (12)
C3—C8—Mn1170.2 (3)O5—Mn1—C8120.40 (13)
C11A—N1A—C10A136 (3)O5—Mn1—O657.17 (11)
C12A—N1A—C11A108.9 (16)C8—Mn1—C9121.79 (13)
C12A—N1A—C10A115 (2)O6—Mn1—C929.25 (12)
N1—C12—C13106.3 (7)O6—Mn1—C8112.59 (12)
C12—C13—N2107.5 (7)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y1/2, z+3/2; (iii) x+3/2, y+1, z1/2; (iv) x+1, y+1/2, z+3/2; (v) x+3/2, y+1, z+1/2.
(c220k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.622 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 1967 reflections
a = 14.7960 (5) Åθ = 2.5–29.4°
b = 12.4275 (4) ŵ = 0.90 mm1
c = 16.6266 (5) ÅT = 220 K
V = 3057.26 (18) Å3Prism, colorless
Z = 80.15 × 0.11 × 0.07 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3673 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2208 reflections with I > 2σ(I)
Detector resolution: 10.3590 pixels mm-1Rint = 0.066
ω scansθmax = 29.5°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1815
Tmin = 0.985, Tmax = 1.000k = 1612
10927 measured reflectionsl = 2219
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)] = 0.066Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.152H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0379P)2 + 6.1843P]
where P = (Fo2 + 2Fc2)/3
3673 reflections(Δ/σ)max = 0.001
212 parametersΔρmax = 0.91 e Å3
275 restraintsΔρmin = 0.63 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.52558 (19)0.3802 (2)0.50406 (16)0.0268 (7)
O20.49860 (19)0.5825 (2)0.62518 (17)0.0279 (7)
C90.7309 (3)0.5764 (4)0.4967 (2)0.0266 (9)
O30.5945 (2)0.3492 (2)0.66820 (17)0.0356 (8)
C10.4036 (3)0.7302 (3)0.5945 (2)0.0224 (9)
C20.5933 (3)0.2693 (3)0.8270 (2)0.0231 (9)
H20.55720.23310.78820.028*
C80.6369 (3)0.4005 (3)0.7191 (2)0.0233 (9)
C100.3934 (8)0.2204 (10)0.6360 (7)0.080 (3)*0.779 (8)
H10A0.44100.16730.64590.120*0.779 (8)
H10B0.41200.26850.59230.120*0.779 (8)
H10C0.33750.18330.62070.120*0.779 (8)
C11A0.3463 (16)0.2276 (16)0.7534 (12)0.032 (5)*0.221 (8)
H11A0.32380.15820.76650.038*0.221 (8)
C12A0.3989 (13)0.3680 (13)0.6860 (12)0.022 (4)*0.221 (8)
H12A0.42230.40930.64270.026*0.221 (8)
C13A0.3829 (16)0.4063 (15)0.7605 (14)0.030 (4)*0.221 (8)
H13A0.38920.47790.77970.035*0.221 (8)
C140.3871 (6)0.5180 (7)0.8286 (5)0.069 (3)*0.779 (8)
H14A0.32710.55090.83810.083*0.779 (8)
H14B0.42060.56380.79000.083*0.779 (8)
C150.4376 (7)0.5101 (9)0.9051 (6)0.102 (4)*0.779 (8)
H15A0.44650.58230.92750.153*0.779 (8)
H15B0.49650.47660.89520.153*0.779 (8)
H15C0.40330.46620.94330.153*0.779 (8)
O40.6725 (2)0.4899 (2)0.70368 (18)0.0352 (8)
C50.7035 (3)0.3706 (3)0.9388 (2)0.0229 (9)
C60.3474 (3)0.7807 (3)0.5390 (3)0.0249 (9)
H60.34360.75380.48560.030*
C30.6418 (3)0.3601 (3)0.8042 (2)0.0232 (9)
C40.6951 (3)0.4115 (3)0.8611 (2)0.0248 (9)
H40.72620.47560.84690.030*
C70.4620 (3)0.6375 (3)0.5702 (2)0.0216 (9)
N10.3777 (4)0.2832 (5)0.7090 (4)0.0434 (16)*0.779 (8)
C120.3443 (5)0.2462 (7)0.7817 (5)0.0455 (18)*0.779 (8)
H120.32540.17450.79200.055*0.779 (8)
C130.3426 (7)0.3232 (7)0.8329 (6)0.059 (2)*0.779 (8)
H130.32130.31930.88670.071*0.779 (8)
C14A0.347 (3)0.369 (4)0.8828 (19)0.132 (16)*0.221 (8)
H14C0.31210.31820.91680.159*0.221 (8)
H14D0.30590.43030.87270.159*0.221 (8)
C15A0.418 (3)0.414 (5)0.938 (3)0.19 (3)*0.221 (8)
H15D0.43330.48720.92220.292*0.221 (8)
H15E0.47270.36860.93530.292*0.221 (8)
H15F0.39550.41370.99370.292*0.221 (8)
C10A0.382 (3)0.199 (3)0.6100 (18)0.068 (11)*0.221 (8)
H10D0.42400.13880.61820.102*0.221 (8)
H10E0.40450.24450.56610.102*0.221 (8)
H10F0.32230.17120.59620.102*0.221 (8)
C110.3962 (5)0.3878 (6)0.7220 (6)0.0480 (18)*0.779 (8)
H110.41970.43680.68350.058*0.779 (8)
N1A0.3766 (14)0.2609 (14)0.6817 (12)0.034 (4)*0.221 (8)
N20.3765 (4)0.4103 (5)0.7960 (4)0.0507 (17)*0.779 (8)
O50.7089 (2)0.4828 (3)0.4860 (2)0.0442 (9)
O60.6984 (2)0.6326 (3)0.55218 (19)0.0415 (8)
N2A0.354 (2)0.3134 (18)0.8033 (13)0.064 (6)*0.221 (8)
Mn10.60452 (4)0.48381 (5)0.57981 (4)0.02102 (19)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0329 (17)0.0274 (16)0.0202 (14)0.0002 (12)0.0008 (13)0.0074 (12)
O20.0337 (16)0.0266 (16)0.0232 (14)0.0095 (13)0.0030 (13)0.0003 (12)
C90.027 (2)0.032 (2)0.0206 (19)0.0001 (17)0.0005 (18)0.0025 (17)
O30.054 (2)0.0314 (17)0.0212 (15)0.0088 (15)0.0055 (15)0.0061 (13)
C10.024 (2)0.019 (2)0.023 (2)0.0002 (16)0.0017 (18)0.0005 (16)
C20.027 (2)0.024 (2)0.0189 (19)0.0015 (16)0.0065 (18)0.0005 (16)
C80.018 (2)0.027 (2)0.0250 (18)0.0007 (16)0.0007 (16)0.0090 (16)
O40.0404 (18)0.0340 (18)0.0312 (16)0.0093 (14)0.0063 (15)0.0116 (14)
C50.024 (2)0.024 (2)0.0207 (19)0.0026 (17)0.0023 (17)0.0020 (16)
C60.030 (2)0.023 (2)0.022 (2)0.0031 (17)0.0014 (19)0.0044 (17)
C30.025 (2)0.023 (2)0.0209 (18)0.0018 (16)0.0018 (16)0.0029 (16)
C40.024 (2)0.022 (2)0.028 (2)0.0033 (17)0.0011 (18)0.0029 (17)
C70.020 (2)0.021 (2)0.024 (2)0.0021 (15)0.0027 (17)0.0032 (16)
O50.056 (2)0.0364 (18)0.0406 (19)0.0176 (16)0.0244 (17)0.0046 (15)
O60.055 (2)0.0353 (18)0.0344 (17)0.0084 (16)0.0218 (17)0.0027 (14)
Mn10.0262 (4)0.0198 (3)0.0171 (3)0.0005 (3)0.0017 (3)0.0007 (3)
Geometric parameters (Å, º) top
O1—C7i1.267 (5)C14—N21.453 (10)
O1—Mn12.147 (3)C15—H15A0.9800
O2—C71.263 (5)C15—H15B0.9800
O2—Mn12.129 (3)C15—H15C0.9800
C9—C5ii1.518 (6)O4—Mn12.293 (3)
C9—O51.220 (5)C5—C9v1.518 (6)
C9—O61.253 (5)C5—C6iv1.397 (5)
C9—Mn12.594 (4)C5—C41.393 (6)
O3—C81.231 (5)C6—C5iii1.397 (5)
O3—Mn12.232 (3)C6—H60.9500
C1—C2iii1.395 (5)C3—C41.387 (6)
C1—C61.391 (6)C4—H40.9500
C1—C71.495 (5)C7—O1i1.267 (5)
C2—C1iv1.395 (5)N1—C121.384 (9)
C2—H20.9500N1—C111.345 (9)
C2—C31.390 (5)C12—H120.9500
C8—O41.257 (5)C12—C131.281 (11)
C8—C31.503 (6)C13—H130.9500
C8—Mn12.582 (4)C13—N21.342 (10)
C10—H10A0.9800C14A—H14C0.9900
C10—H10B0.9800C14A—H14D0.9900
C10—H10C0.9800C14A—C15A1.51 (2)
C10—N11.463 (12)C14A—N2A1.495 (18)
C11A—H11A0.9500C15A—H15D0.9800
C11A—C12A2.21 (3)C15A—H15E0.9800
C11A—N1A1.339 (17)C15A—H15F0.9800
C11A—N2A1.357 (18)C10A—H10D0.9800
C12A—H12A0.9500C10A—H10E0.9800
C12A—C13A1.347 (17)C10A—H10F0.9800
C12A—N1A1.374 (16)C10A—N1A1.42 (3)
C13A—H13A0.9500C11—H110.9500
C13A—N2A1.420 (17)C11—N21.295 (10)
C14—H14A0.9900O5—Mn12.195 (3)
C14—H14B0.9900O6—Mn12.358 (3)
C14—C151.479 (12)
C7i—O1—Mn1126.7 (3)C12—N1—C10127.2 (7)
C7—O2—Mn1111.8 (2)C11—N1—C10128.1 (8)
C5ii—C9—Mn1172.6 (3)C11—N1—C12104.7 (7)
O5—C9—C5ii119.5 (4)N1—C12—H12125.1
O5—C9—O6122.4 (4)C13—C12—N1109.8 (8)
O5—C9—Mn157.5 (2)C13—C12—H12125.1
O6—C9—C5ii118.0 (4)C12—C13—H13126.5
O6—C9—Mn165.1 (2)C12—C13—N2106.9 (8)
C8—O3—Mn191.8 (2)N2—C13—H13126.5
C2iii—C1—C7120.1 (4)H14C—C14A—H14D105.6
C6—C1—C2iii118.9 (4)C15A—C14A—H14C104.4
C6—C1—C7121.0 (4)C15A—C14A—H14D104.4
C1iv—C2—H2119.3N2A—C14A—H14C104.4
C3—C2—C1iv121.4 (4)N2A—C14A—H14D104.4
C3—C2—H2119.3N2A—C14A—C15A131 (4)
O3—C8—O4122.1 (4)C14A—C15A—H15D109.5
O3—C8—C3119.9 (4)C14A—C15A—H15E109.5
O3—C8—Mn159.8 (2)C14A—C15A—H15F109.5
O4—C8—C3117.9 (4)H15D—C15A—H15E109.5
O4—C8—Mn162.6 (2)H15D—C15A—H15F109.5
C3—C8—Mn1170.9 (3)H15E—C15A—H15F109.5
H10A—C10—H10B109.5H10D—C10A—H10E109.5
H10A—C10—H10C109.5H10D—C10A—H10F109.5
H10B—C10—H10C109.5H10E—C10A—H10F109.5
N1—C10—H10A109.5N1A—C10A—H10D109.5
N1—C10—H10B109.5N1A—C10A—H10E109.5
N1—C10—H10C109.5N1A—C10A—H10F109.5
C12A—C11A—H11A162.8N1—C11—H11125.8
N1A—C11A—H11A127.1N2—C11—N1108.4 (7)
N1A—C11A—C12A35.8 (9)N2—C11—H11125.8
N1A—C11A—N2A105.8 (17)C11A—N1A—C12A109.4 (16)
N2A—C11A—H11A127.1C11A—N1A—C10A126.8 (19)
N2A—C11A—C12A70.1 (12)C12A—N1A—C10A123.7 (19)
C11A—C12A—H12A159.6C13—N2—C14127.9 (7)
C13A—C12A—C11A75.6 (10)C11—N2—C14121.9 (7)
C13A—C12A—H12A124.8C11—N2—C13110.1 (7)
C13A—C12A—N1A110.4 (15)C9—O5—Mn194.5 (3)
N1A—C12A—C11A34.8 (9)C9—O6—Mn186.1 (3)
N1A—C12A—H12A124.8C11A—N2A—C13A111.0 (17)
C12A—C13A—H13A128.5C11A—N2A—C14A154 (2)
C12A—C13A—N2A103.1 (14)C13A—N2A—C14A95 (2)
N2A—C13A—H13A128.5O1—Mn1—C9110.20 (12)
H14A—C14—H14B108.4O1—Mn1—O384.29 (11)
C15—C14—H14A110.0O1—Mn1—C8112.75 (12)
C15—C14—H14B110.0O1—Mn1—O4141.76 (11)
N2—C14—H14A110.0O1—Mn1—O587.85 (12)
N2—C14—H14B110.0O1—Mn1—O6132.57 (11)
N2—C14—C15108.3 (8)O2—Mn1—O198.81 (11)
C14—C15—H15A109.5O2—Mn1—C9117.63 (13)
C14—C15—H15B109.5O2—Mn1—O398.62 (12)
C14—C15—H15C109.5O2—Mn1—C892.86 (12)
H15A—C15—H15B109.5O2—Mn1—O489.19 (11)
H15A—C15—H15C109.5O2—Mn1—O5140.63 (12)
H15B—C15—H15C109.5O2—Mn1—O692.91 (12)
C8—O4—Mn188.3 (2)O3—Mn1—C9137.00 (13)
C6iv—C5—C9v121.7 (4)O3—Mn1—C828.47 (12)
C4—C5—C9v119.1 (4)O3—Mn1—O457.49 (11)
C4—C5—C6iv119.2 (4)O3—Mn1—O6139.06 (12)
C1—C6—C5iii120.5 (4)C8—Mn1—C9121.49 (13)
C1—C6—H6119.7O4—Mn1—C998.50 (12)
C5iii—C6—H6119.7O4—Mn1—C829.11 (11)
C2—C3—C8120.2 (4)O4—Mn1—O683.72 (11)
C4—C3—C2118.8 (4)O5—Mn1—C927.97 (12)
C4—C3—C8121.0 (4)O5—Mn1—O3120.70 (13)
C5—C4—H4119.5O5—Mn1—C8120.31 (13)
C3—C4—C5121.0 (4)O5—Mn1—O4109.24 (13)
C3—C4—H4119.5O5—Mn1—O656.73 (11)
O1i—C7—C1118.7 (4)O6—Mn1—C928.82 (12)
O2—C7—O1i123.3 (4)O6—Mn1—C8112.34 (13)
O2—C7—C1118.0 (3)
C9v—C5—C4—C3174.4 (4)C5ii—C9—O6—Mn1172.5 (3)
O3—C8—O4—Mn16.1 (4)C6—C1—C7—O1i14.7 (6)
O3—C8—C3—C24.7 (6)C6—C1—C7—O2167.2 (4)
O3—C8—C3—C4174.7 (4)C6iv—C5—C4—C34.4 (6)
C1iv—C2—C3—C8179.9 (4)C3—C8—O4—Mn1169.7 (3)
C1iv—C2—C3—C40.7 (6)C7—C1—C6—C5iii176.7 (4)
C2iii—C1—C6—C5iii1.4 (6)N1—C12—C13—N21.5 (10)
C2iii—C1—C7—O1i163.4 (4)N1—C11—N2—C14178.7 (7)
C2iii—C1—C7—O214.7 (6)N1—C11—N2—C131.7 (9)
C2—C3—C4—C53.0 (6)C12—N1—C11—N20.7 (8)
C8—C3—C4—C5176.4 (4)C12—C13—N2—C14178.8 (8)
C10—N1—C12—C13177.8 (9)C12—C13—N2—C112.0 (10)
C10—N1—C11—N2176.6 (8)C15A—C14A—N2A—C11A114 (7)
C11A—C12A—C13A—N2A3.2 (17)C15A—C14A—N2A—C13A70 (6)
C11A—C12A—N1A—C10A178 (4)C11—N1—C12—C130.5 (9)
C12A—C11A—N1A—C10A178 (4)N1A—C11A—N2A—C13A5 (3)
C12A—C11A—N2A—C13A3.5 (18)N1A—C11A—N2A—C14A178 (6)
C12A—C11A—N2A—C14A180 (7)N1A—C12A—C13A—N2A3 (3)
C12A—C13A—N2A—C11A5 (3)O5—C9—O6—Mn14.6 (4)
C12A—C13A—N2A—C14A176 (2)O6—C9—O5—Mn15.0 (5)
C13A—C12A—N1A—C11A0 (3)N2A—C11A—N1A—C12A3 (3)
C13A—C12A—N1A—C10A177 (3)N2A—C11A—N1A—C10A179 (3)
C15—C14—N2—C1353.0 (12)Mn1—O2—C7—O1i13.3 (5)
C15—C14—N2—C11130.5 (8)Mn1—O2—C7—C1164.7 (3)
O4—C8—C3—C2171.3 (4)Mn1—O3—C8—O46.3 (4)
O4—C8—C3—C49.3 (6)Mn1—O3—C8—C3169.5 (3)
C5ii—C9—O5—Mn1172.1 (3)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+3/2, y+1, z1/2; (iii) x+1, y+1/2, z+3/2; (iv) x+1, y1/2, z+3/2; (v) x+3/2, y+1, z+1/2.
(c280k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.611 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 1836 reflections
a = 14.8837 (6) Åθ = 2.5–29.3°
b = 12.4554 (5) ŵ = 0.89 mm1
c = 16.6018 (5) ÅT = 280 K
V = 3077.69 (19) Å3Prism, colorless
Z = 80.15 × 0.11 × 0.07 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3700 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2103 reflections with I > 2σ(I)
Detector resolution: 10.3590 pixels mm-1Rint = 0.069
ω scansθmax = 29.3°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1815
Tmin = 0.981, Tmax = 1.000k = 1216
11023 measured reflectionsl = 1922
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)] = 0.074Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.193H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0707P)2 + 4.4689P]
where P = (Fo2 + 2Fc2)/3
3700 reflections(Δ/σ)max = 0.002
210 parametersΔρmax = 0.86 e Å3
284 restraintsΔρmin = 0.65 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
O10.5270 (2)0.3805 (2)0.50519 (18)0.0322 (8)
O20.4989 (2)0.5849 (3)0.62392 (19)0.0354 (8)
C90.7306 (3)0.5773 (4)0.4984 (3)0.0338 (11)
O30.5934 (3)0.3515 (3)0.6698 (2)0.0436 (9)
C20.5925 (3)0.2700 (4)0.8289 (3)0.0285 (10)
H20.55680.23520.79110.034*
C80.6355 (3)0.4019 (4)0.7204 (3)0.0289 (10)
N2A0.376 (2)0.407 (2)0.8158 (15)0.051 (6)*0.172 (7)
C100.3890 (7)0.2197 (8)0.6293 (6)0.091 (3)*0.828 (7)
H10D0.43630.16860.63760.136*0.828 (7)
H10E0.40470.26660.58560.136*0.828 (7)
H10F0.33430.18260.61650.136*0.828 (7)
C11A0.351 (2)0.299 (2)0.7991 (16)0.045 (6)*0.172 (7)
H11A0.32180.25090.83310.054*0.172 (7)
C12A0.3973 (18)0.3752 (16)0.6819 (14)0.025 (5)*0.172 (7)
H12A0.40800.38400.62710.031*0.172 (7)
C13A0.398 (3)0.4513 (19)0.7431 (17)0.070 (6)*0.172 (7)
H13A0.41130.52350.73560.084*0.172 (7)
C140.3865 (7)0.5203 (9)0.8257 (7)0.098 (4)*0.828 (7)
H14C0.41820.56820.78950.118*0.828 (7)
H14D0.32760.55080.83590.118*0.828 (7)
C150.4362 (9)0.5128 (12)0.9024 (8)0.135 (5)*0.828 (7)
H15D0.49710.49180.89180.202*0.828 (7)
H15E0.40820.46040.93650.202*0.828 (7)
H15F0.43570.58140.92870.202*0.828 (7)
O40.6712 (3)0.4915 (3)0.7051 (2)0.0442 (9)
C50.7031 (3)0.3708 (4)0.9406 (3)0.0305 (11)
C60.3469 (3)0.7812 (4)0.5375 (3)0.0307 (11)
H60.34260.75440.48540.037*
C30.6411 (3)0.3606 (4)0.8063 (3)0.0278 (10)
C40.6943 (3)0.4119 (4)0.8629 (3)0.0290 (10)
H40.72460.47460.84880.035*
C10.4033 (3)0.7311 (4)0.5931 (3)0.0271 (10)
C70.4614 (3)0.6385 (4)0.5689 (3)0.0266 (10)
C120.3451 (5)0.2444 (7)0.7761 (5)0.0533 (19)*0.828 (7)
H120.32780.17430.78760.064*0.828 (7)
C130.3433 (6)0.3250 (7)0.8301 (6)0.070 (2)*0.828 (7)
H130.32520.32370.88370.084*0.828 (7)
C14A0.342 (4)0.401 (5)0.897 (2)0.133 (17)*0.172 (7)
H14A0.31450.33250.90840.159*0.172 (7)
H14B0.30050.45880.90860.159*0.172 (7)
C15A0.429 (4)0.415 (7)0.941 (4)0.17 (2)*0.172 (7)
H15A0.47600.37690.91290.251*0.172 (7)
H15B0.42350.38660.99450.251*0.172 (7)
H15C0.44420.48970.94360.251*0.172 (7)
Mn10.60414 (5)0.48519 (5)0.58091 (4)0.0256 (2)
C10A0.362 (6)0.187 (4)0.673 (4)0.19 (3)*0.172 (7)
H10A0.36250.12430.70620.287*0.172 (7)
H10B0.40900.18210.63340.287*0.172 (7)
H10C0.30510.19320.64630.287*0.172 (7)
C110.3937 (6)0.3847 (7)0.7196 (6)0.060 (2)*0.828 (7)
H110.41850.43310.68320.072*0.828 (7)
N10.3770 (6)0.2791 (6)0.6983 (5)0.067 (2)*0.828 (7)
N1A0.3771 (19)0.2842 (16)0.7239 (14)0.029 (5)*0.172 (7)
O50.7090 (3)0.4841 (3)0.4876 (2)0.0541 (11)
O60.6977 (3)0.6333 (3)0.5527 (2)0.0518 (10)
N20.3754 (6)0.4103 (6)0.7851 (5)0.070 (2)*0.828 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0405 (19)0.0317 (18)0.0243 (16)0.0019 (14)0.0035 (15)0.0046 (14)
O20.0439 (19)0.0310 (18)0.0312 (17)0.0103 (14)0.0018 (15)0.0007 (14)
C90.032 (3)0.044 (3)0.026 (2)0.002 (2)0.000 (2)0.0021 (19)
O30.062 (2)0.043 (2)0.0264 (17)0.0089 (17)0.0065 (17)0.0096 (15)
C20.030 (3)0.029 (2)0.026 (2)0.0036 (18)0.008 (2)0.0002 (19)
C80.024 (2)0.035 (2)0.028 (2)0.0019 (18)0.0035 (18)0.0093 (18)
O40.055 (2)0.041 (2)0.0370 (19)0.0104 (16)0.0105 (17)0.0138 (16)
C50.033 (3)0.032 (3)0.026 (2)0.002 (2)0.005 (2)0.0013 (19)
C60.034 (3)0.033 (3)0.025 (2)0.002 (2)0.007 (2)0.003 (2)
C30.028 (2)0.027 (2)0.029 (2)0.0012 (18)0.0035 (18)0.0038 (17)
C40.029 (2)0.027 (2)0.030 (2)0.0030 (19)0.0022 (19)0.0038 (18)
C10.026 (2)0.025 (2)0.030 (2)0.0029 (17)0.004 (2)0.0016 (18)
C70.026 (2)0.026 (2)0.028 (2)0.0027 (17)0.0025 (19)0.0034 (18)
Mn10.0309 (4)0.0252 (4)0.0206 (4)0.0001 (3)0.0019 (3)0.0012 (3)
O50.063 (3)0.046 (2)0.054 (2)0.0200 (19)0.030 (2)0.0065 (18)
O60.068 (3)0.044 (2)0.043 (2)0.0084 (18)0.026 (2)0.0010 (17)
Geometric parameters (Å, º) top
O1—C7i1.265 (5)C14—C151.475 (15)
O1—Mn12.145 (3)C14—N21.536 (13)
O2—C71.262 (5)O4—Mn12.292 (4)
O2—Mn12.123 (3)C5—C9iv1.521 (7)
C9—C5ii1.521 (7)C5—C6iii1.390 (6)
C9—Mn12.595 (5)C5—C41.395 (6)
C9—O51.218 (6)C6—C5v1.390 (6)
C9—O61.240 (6)C6—C11.394 (6)
O3—C81.221 (6)C3—C41.385 (6)
O3—Mn12.231 (3)C1—C2v1.385 (6)
C2—C31.392 (6)C1—C71.497 (6)
C2—C1iii1.385 (6)C7—O1i1.265 (5)
C8—O41.263 (6)C12—C131.347 (12)
C8—C31.517 (6)C12—N11.442 (11)
C8—Mn12.581 (5)C13—N21.383 (11)
N2A—C11A1.417 (19)C14A—C15A1.49 (3)
N2A—C13A1.367 (18)Mn1—O52.198 (4)
N2A—C14A1.44 (3)Mn1—O62.358 (4)
C10—N11.375 (12)C10A—N1A1.49 (3)
C11A—N1A1.324 (18)C11—N11.384 (11)
C12A—C13A1.389 (18)C11—N21.166 (11)
C12A—N1A1.364 (18)
C7i—O1—Mn1127.6 (3)O1—Mn1—C9110.36 (14)
C7—O2—Mn1113.1 (3)O1—Mn1—O384.03 (12)
C5ii—C9—Mn1172.5 (3)O1—Mn1—C8112.24 (14)
O5—C9—C5ii118.9 (4)O1—Mn1—O4141.40 (12)
O5—C9—Mn157.6 (3)O1—Mn1—O587.90 (14)
O5—C9—O6122.6 (5)O1—Mn1—O6132.47 (13)
O6—C9—C5ii118.4 (5)O2—Mn1—O199.06 (13)
O6—C9—Mn165.1 (3)O2—Mn1—C9117.03 (15)
C8—O3—Mn192.0 (3)O2—Mn1—O399.29 (14)
C1iii—C2—C3120.8 (4)O2—Mn1—C893.83 (14)
O3—C8—O4122.1 (4)O2—Mn1—O489.93 (14)
O3—C8—C3120.1 (4)O2—Mn1—O5139.85 (14)
O3—C8—Mn159.8 (2)O2—Mn1—O692.59 (13)
O4—C8—C3117.7 (4)O3—Mn1—C9136.95 (15)
O4—C8—Mn162.6 (2)O3—Mn1—C828.22 (13)
C3—C8—Mn1171.6 (3)O3—Mn1—O457.43 (12)
C11A—N2A—C14A93 (3)O3—Mn1—O6139.24 (14)
C13A—N2A—C11A105.9 (18)C8—Mn1—C9121.35 (15)
C13A—N2A—C14A158 (3)O4—Mn1—C998.24 (14)
N1A—C11A—N2A103.8 (19)O4—Mn1—C829.29 (13)
N1A—C12A—C13A101.2 (17)O4—Mn1—O683.94 (13)
N2A—C13A—C12A111.6 (18)O5—Mn1—C927.89 (14)
C15—C14—N2112.1 (10)O5—Mn1—O3120.80 (15)
C8—O4—Mn188.2 (3)O5—Mn1—C8120.11 (16)
C6iii—C5—C9iv121.6 (4)O5—Mn1—O4108.95 (16)
C6iii—C5—C4119.1 (4)O5—Mn1—O656.34 (13)
C4—C5—C9iv119.3 (4)O6—Mn1—C928.49 (14)
C5v—C6—C1120.6 (4)O6—Mn1—C8112.72 (15)
C2—C3—C8119.9 (4)N2—C11—N1117.1 (9)
C4—C3—C2119.2 (4)C10—N1—C12128.9 (8)
C4—C3—C8120.8 (4)C10—N1—C11134.5 (9)
C3—C4—C5120.8 (4)C11—N1—C1296.6 (7)
C2v—C1—C6119.3 (4)C11A—N1A—C12A115.5 (18)
C2v—C1—C7119.6 (4)C11A—N1A—C10A127 (3)
C6—C1—C7121.0 (4)C12A—N1A—C10A115 (3)
O1i—C7—C1119.0 (4)C9—O5—Mn194.5 (3)
O2—C7—O1i123.0 (4)C9—O6—Mn186.4 (3)
O2—C7—C1118.0 (4)C13—N2—C14119.0 (9)
C13—C12—N1112.3 (8)C11—N2—C14129.0 (9)
C12—C13—N2101.9 (9)C11—N2—C13112.0 (9)
N2A—C14A—C15A99 (4)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+3/2, y+1, z1/2; (iii) x+1, y1/2, z+3/2; (iv) x+3/2, y+1, z+1/2; (v) x+1, y+1/2, z+3/2.
(c300k) top
Crystal data top
C9H3MnO6·1(C6H11N2)Dx = 1.606 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 1787 reflections
a = 14.9204 (6) Åθ = 2.5–29.4°
b = 12.4737 (5) ŵ = 0.89 mm1
c = 16.5884 (6) ÅT = 300 K
V = 3087.3 (2) Å3Prism, colorless
Z = 80.15 × 0.11 × 0.07 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3708 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2054 reflections with I > 2σ(I)
Detector resolution: 10.3590 pixels mm-1Rint = 0.071
ω scansθmax = 29.4°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1815
Tmin = 0.980, Tmax = 1.000k = 1216
11042 measured reflectionsl = 1922
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)] = 0.066Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.166H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0543P)2 + 2.0156P]
where P = (Fo2 + 2Fc2)/3
3708 reflections(Δ/σ)max = 0.001
213 parametersΔρmax = 0.71 e Å3
283 restraintsΔρmin = 0.66 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C80.6353 (3)0.4028 (3)0.7216 (3)0.0294 (9)
C90.7313 (3)0.5777 (4)0.4990 (3)0.0352 (10)
C70.4613 (3)0.6389 (3)0.5679 (2)0.0275 (9)
O10.5276 (2)0.3805 (2)0.50571 (17)0.0350 (7)
C10.4032 (3)0.7318 (3)0.5925 (2)0.0274 (9)
N1A0.3748 (15)0.2591 (14)0.6764 (13)0.045 (5)*0.214 (8)
C100.3914 (9)0.2210 (11)0.6355 (8)0.108 (4)*0.786 (8)
H10D0.43800.16960.64540.163*0.786 (8)
H10E0.40860.26690.59170.163*0.786 (8)
H10F0.33700.18420.62200.163*0.786 (8)
C11A0.3466 (19)0.2289 (17)0.7496 (14)0.050 (5)*0.214 (8)
H11A0.32510.16120.76280.060*0.214 (8)
C12A0.3957 (13)0.3679 (14)0.6821 (12)0.026 (4)*0.214 (8)
H12A0.41770.40900.63980.031*0.214 (8)
C13A0.3801 (17)0.4054 (16)0.7559 (14)0.038 (5)*0.214 (8)
H13A0.38480.47570.77400.045*0.214 (8)
C140.3853 (6)0.5197 (8)0.8213 (6)0.098 (3)*0.786 (8)
H14C0.41730.56220.78160.118*0.786 (8)
H14D0.32680.55190.82970.118*0.786 (8)
C150.4333 (9)0.5182 (12)0.8943 (9)0.157 (5)*0.786 (8)
H15D0.48820.47920.88710.235*0.786 (8)
H15E0.39790.48390.93520.235*0.786 (8)
H15F0.44660.59030.91050.235*0.786 (8)
O20.4986 (2)0.5854 (2)0.62340 (17)0.0372 (7)
C40.6941 (3)0.4125 (3)0.8639 (2)0.0317 (10)
H40.72440.47500.85000.038*
C50.7030 (3)0.3704 (3)0.9414 (2)0.0305 (10)
C20.5922 (3)0.2710 (3)0.8294 (2)0.0292 (10)
H20.55640.23640.79160.035*
C30.6404 (3)0.3614 (3)0.8073 (2)0.0287 (9)
C60.3476 (3)0.7810 (3)0.5373 (3)0.0318 (10)
H60.34390.75410.48510.038*
C120.3438 (6)0.2491 (7)0.7805 (5)0.062 (2)*0.786 (8)
H120.32630.17900.79130.074*0.786 (8)
C130.3404 (7)0.3252 (8)0.8300 (7)0.081 (3)*0.786 (8)
H130.31840.32200.88240.097*0.786 (8)
C14A0.359 (3)0.362 (4)0.8825 (18)0.150 (15)*0.214 (8)
H14A0.34960.30130.91770.180*0.214 (8)
H14B0.30270.40170.88450.180*0.214 (8)
C15A0.422 (3)0.435 (5)0.934 (3)0.19 (2)*0.214 (8)
H15A0.39700.50560.93710.281*0.214 (8)
H15B0.47980.43730.90970.281*0.214 (8)
H15C0.42650.40520.98740.281*0.214 (8)
O50.7082 (2)0.4849 (3)0.4887 (2)0.0574 (10)
C10A0.381 (3)0.199 (3)0.6064 (18)0.076 (11)*0.214 (8)
H10A0.43380.15520.60840.113*0.214 (8)
H10B0.38420.24600.56070.113*0.214 (8)
H10C0.32910.15390.60150.113*0.214 (8)
C110.3944 (6)0.3879 (7)0.7191 (6)0.060 (2)*0.786 (8)
H110.41680.43470.68040.072*0.786 (8)
O30.5928 (2)0.3525 (3)0.67086 (18)0.0472 (9)
O40.6704 (2)0.4915 (3)0.70604 (19)0.0475 (9)
N10.3773 (4)0.2851 (5)0.7074 (4)0.0569 (18)*0.786 (8)
N20.3751 (5)0.4134 (5)0.7929 (5)0.0669 (19)*0.786 (8)
N2A0.354 (2)0.3119 (19)0.8011 (13)0.075 (6)*0.214 (8)
O60.6983 (2)0.6336 (3)0.5535 (2)0.0567 (10)
Mn10.60400 (4)0.48558 (5)0.58142 (4)0.0271 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C80.026 (2)0.033 (2)0.0295 (19)0.0001 (17)0.0041 (17)0.0088 (17)
C90.036 (2)0.044 (3)0.026 (2)0.0003 (19)0.0027 (19)0.0044 (19)
C70.030 (2)0.024 (2)0.028 (2)0.0015 (16)0.0003 (18)0.0034 (17)
O10.0449 (19)0.0333 (17)0.0267 (15)0.0009 (13)0.0016 (14)0.0064 (13)
C10.032 (2)0.022 (2)0.028 (2)0.0011 (16)0.0004 (19)0.0013 (17)
O20.0446 (18)0.0362 (17)0.0307 (16)0.0127 (14)0.0015 (14)0.0005 (13)
C40.035 (2)0.027 (2)0.032 (2)0.0037 (18)0.0034 (19)0.0011 (18)
C50.031 (2)0.033 (2)0.028 (2)0.0014 (19)0.0055 (19)0.0016 (18)
C20.032 (2)0.029 (2)0.027 (2)0.0023 (17)0.0086 (19)0.0002 (18)
C30.032 (2)0.027 (2)0.0271 (19)0.0000 (17)0.0039 (17)0.0012 (16)
C60.036 (3)0.030 (2)0.029 (2)0.0015 (19)0.004 (2)0.0026 (18)
O50.071 (2)0.049 (2)0.052 (2)0.0222 (18)0.0304 (19)0.0074 (17)
O30.071 (2)0.0433 (19)0.0276 (16)0.0121 (16)0.0102 (16)0.0095 (14)
O40.059 (2)0.0448 (19)0.0388 (18)0.0119 (16)0.0100 (16)0.0158 (15)
O60.071 (2)0.049 (2)0.050 (2)0.0092 (18)0.0296 (19)0.0006 (16)
Mn10.0333 (4)0.0266 (4)0.0215 (3)0.0006 (3)0.0021 (3)0.0009 (3)
Geometric parameters (Å, º) top
C8—C31.514 (6)C14—C151.409 (15)
C8—O31.226 (5)C14—N21.415 (10)
C8—O41.251 (5)O2—Mn12.123 (3)
C8—Mn12.587 (4)C4—C51.395 (6)
C9—C5i1.514 (6)C4—C31.390 (6)
C9—O51.220 (5)C5—C9iv1.514 (6)
C9—O61.243 (5)C5—C6v1.392 (6)
C9—Mn12.607 (5)C2—C1v1.386 (5)
C7—O1ii1.256 (5)C2—C31.388 (6)
C7—C11.504 (5)C6—C5iii1.392 (6)
C7—O21.265 (5)C12—C131.257 (12)
O1—C7ii1.256 (5)C12—N11.387 (9)
O1—Mn12.143 (3)C13—N21.362 (11)
C1—C2iii1.386 (5)C14A—C15A1.56 (3)
C1—C61.380 (6)C14A—N2A1.49 (2)
N1A—C11A1.339 (17)O5—Mn12.187 (3)
N1A—C12A1.396 (16)C11—N11.321 (9)
N1A—C10A1.39 (3)C11—N21.297 (10)
C10—N11.450 (13)O3—Mn12.232 (3)
C11A—N2A1.347 (17)O4—Mn12.293 (3)
C12A—C13A1.330 (17)O6—Mn12.368 (3)
C13A—N2A1.438 (18)
C3—C8—Mn1171.5 (3)C8—O3—Mn192.2 (3)
O3—C8—C3119.8 (4)C8—O4—Mn188.7 (3)
O3—C8—O4121.8 (4)C12—N1—C10126.3 (8)
O3—C8—Mn159.6 (2)C11—N1—C10128.9 (9)
O4—C8—C3118.3 (4)C11—N1—C12104.8 (7)
O4—C8—Mn162.4 (2)C13—N2—C14130.3 (9)
C5i—C9—Mn1172.3 (3)C11—N2—C14121.3 (8)
O5—C9—C5i120.0 (4)C11—N2—C13108.3 (8)
O5—C9—O6121.5 (4)C11A—N2A—C13A108.4 (16)
O5—C9—Mn156.6 (2)C11A—N2A—C14A154 (2)
O6—C9—C5i118.4 (4)C13A—N2A—C14A97 (2)
O6—C9—Mn165.0 (2)C9—O6—Mn186.6 (3)
O1ii—C7—C1119.2 (4)C8—Mn1—C9121.06 (14)
O1ii—C7—O2123.2 (4)O1—Mn1—C8112.23 (13)
O2—C7—C1117.5 (3)O1—Mn1—C9110.47 (13)
C7ii—O1—Mn1128.1 (3)O1—Mn1—O587.91 (12)
C2iii—C1—C7119.8 (4)O1—Mn1—O383.98 (11)
C6—C1—C7120.6 (4)O1—Mn1—O4141.03 (11)
C6—C1—C2iii119.5 (4)O1—Mn1—O6132.70 (12)
C11A—N1A—C12A106.3 (16)O2—Mn1—C894.18 (12)
C11A—N1A—C10A129 (2)O2—Mn1—C9116.93 (14)
C10A—N1A—C12A124.7 (19)O2—Mn1—O199.04 (11)
N1A—C11A—N2A109.4 (18)O2—Mn1—O5139.41 (13)
C13A—C12A—N1A111.4 (15)O2—Mn1—O399.37 (12)
C12A—C13A—N2A104.0 (15)O2—Mn1—O490.30 (12)
C15—C14—N2109.2 (10)O2—Mn1—O692.69 (12)
C7—O2—Mn1113.3 (3)O5—Mn1—C8120.17 (14)
C3—C4—C5120.4 (4)O5—Mn1—C927.75 (12)
C4—C5—C9iv118.8 (4)O5—Mn1—O3121.18 (14)
C6v—C5—C9iv122.2 (4)O5—Mn1—O4109.10 (14)
C6v—C5—C4118.9 (4)O5—Mn1—O656.13 (12)
C1v—C2—C3120.6 (4)O3—Mn1—C828.26 (12)
C4—C3—C8120.5 (4)O3—Mn1—C9136.94 (14)
C2—C3—C8120.0 (4)O3—Mn1—O457.12 (11)
C2—C3—C4119.5 (4)O3—Mn1—O6138.98 (13)
C1—C6—C5iii120.9 (4)O4—Mn1—C828.92 (12)
C13—C12—N1109.9 (9)O4—Mn1—C998.27 (13)
C12—C13—N2107.4 (10)O4—Mn1—O683.97 (12)
N2A—C14A—C15A140 (4)O6—Mn1—C8112.36 (14)
C9—O5—Mn195.6 (3)O6—Mn1—C928.41 (12)
N2—C11—N1109.5 (8)
Symmetry codes: (i) x+3/2, y+1, z1/2; (ii) x+1, y+1, z+1; (iii) x+1, y+1/2, z+3/2; (iv) x+3/2, y+1, z+1/2; (v) x+1, y1/2, z+3/2.
(c320k) top
Crystal data top
C9H3MnO6·C6H11N2Dx = 1.599 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 1768 reflections
a = 14.9773 (6) Åθ = 2.5–29.4°
b = 12.5017 (5) ŵ = 0.89 mm1
c = 16.5629 (6) ÅT = 320 K
V = 3101.3 (2) Å3Prism, colorless
Z = 80.15 × 0.11 × 0.07 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3720 independent reflections
Radiation source: SuperNova (Mo) X-ray Source2006 reflections with I > 2σ(I)
Detector resolution: 10.3590 pixels mm-1Rint = 0.071
ω scansθmax = 29.4°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1815
Tmin = 0.982, Tmax = 1.000k = 1216
11091 measured reflectionsl = 1922
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)] = 0.073Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.200H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0672P)2 + 5.9635P]
where P = (Fo2 + 2Fc2)/3
3720 reflections(Δ/σ)max < 0.001
212 parametersΔρmax = 0.79 e Å3
287 restraintsΔρmin = 0.56 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C90.7317 (4)0.5786 (5)0.5008 (3)0.0398 (12)
O10.5281 (2)0.3808 (3)0.50679 (19)0.0382 (9)
C80.6341 (3)0.4040 (4)0.7228 (3)0.0326 (11)
O20.4992 (2)0.5867 (3)0.6227 (2)0.0414 (9)
C20.5918 (3)0.2721 (4)0.8306 (3)0.0328 (11)
H20.55600.23780.79270.039*
C70.4615 (3)0.6389 (4)0.5668 (3)0.0297 (11)
N1A0.374 (3)0.2788 (19)0.7178 (18)0.057 (6)*0.189 (8)
Mn10.60384 (5)0.48631 (6)0.58239 (4)0.0298 (3)
C100.3894 (9)0.2173 (11)0.6263 (8)0.112 (4)*0.811 (8)
H10D0.43500.16490.63600.167*0.811 (8)
H10E0.40700.26260.58230.167*0.811 (8)
H10F0.33450.18180.61300.167*0.811 (8)
C11A0.352 (2)0.288 (2)0.7950 (18)0.052 (6)*0.189 (8)
H11A0.32640.23620.82790.062*0.189 (8)
C12A0.395 (2)0.3746 (19)0.6805 (15)0.038 (5)*0.189 (8)
H12A0.40640.38810.62620.046*0.189 (8)
C13A0.394 (3)0.444 (2)0.7444 (18)0.079 (6)*0.189 (8)
H13A0.40540.51730.73990.095*0.189 (8)
C140.3838 (9)0.5212 (11)0.8169 (8)0.126 (5)*0.811 (8)
H14C0.41540.56730.77940.151*0.811 (8)
H14D0.32500.55160.82620.151*0.811 (8)
C150.4324 (12)0.5159 (15)0.8928 (11)0.187 (7)*0.811 (8)
H15D0.39620.48120.93280.280*0.811 (8)
H15E0.44670.58700.91050.280*0.811 (8)
H15F0.48650.47610.88520.280*0.811 (8)
O30.5930 (3)0.3536 (3)0.6717 (2)0.0525 (11)
C50.7026 (3)0.3697 (4)0.9428 (3)0.0353 (12)
C60.3475 (3)0.7806 (4)0.5357 (3)0.0361 (12)
H60.34310.75320.48360.043*
C30.6400 (3)0.3615 (4)0.8084 (3)0.0317 (11)
C40.6939 (3)0.4122 (4)0.8650 (3)0.0343 (11)
H40.72420.47450.85120.041*
C10.4036 (3)0.7325 (4)0.5906 (3)0.0314 (11)
C120.3439 (6)0.2451 (8)0.7727 (6)0.067 (2)*0.811 (8)
H120.32590.17550.78400.081*0.811 (8)
C130.3420 (7)0.3251 (9)0.8256 (7)0.081 (3)*0.811 (8)
H130.32350.32370.87910.097*0.811 (8)
C14A0.342 (4)0.415 (5)0.899 (2)0.152 (17)*0.189 (8)
H14A0.29520.36450.91350.183*0.189 (8)
H14B0.31790.48670.90260.183*0.189 (8)
C15A0.421 (5)0.402 (7)0.953 (5)0.21 (2)*0.189 (8)
H15A0.40370.36501.00160.313*0.189 (8)
H15B0.44420.47140.96740.313*0.189 (8)
H15C0.46670.36180.92610.313*0.189 (8)
O60.6989 (3)0.6345 (3)0.5547 (3)0.0636 (12)
N20.3745 (7)0.4116 (7)0.7813 (6)0.081 (2)*0.811 (8)
C10A0.365 (5)0.190 (4)0.661 (3)0.16 (2)*0.189 (8)
H10A0.36090.21730.60730.246*0.189 (8)
H10B0.31210.15020.67400.246*0.189 (8)
H10C0.41620.14400.66560.246*0.189 (8)
C110.3933 (7)0.3829 (8)0.7153 (7)0.072 (3)*0.811 (8)
H110.41830.42960.67780.086*0.811 (8)
O40.6695 (3)0.4928 (3)0.7080 (2)0.0538 (11)
O50.7075 (3)0.4864 (3)0.4896 (3)0.0619 (12)
N10.3771 (8)0.2800 (7)0.6966 (6)0.077 (3)*0.811 (8)
N2A0.374 (2)0.393 (2)0.8165 (16)0.072 (6)*0.189 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C90.037 (3)0.047 (3)0.035 (3)0.003 (2)0.002 (2)0.003 (2)
O10.049 (2)0.038 (2)0.0272 (17)0.0002 (16)0.0023 (16)0.0060 (15)
C80.029 (3)0.037 (3)0.031 (2)0.0001 (19)0.0045 (19)0.0082 (18)
O20.047 (2)0.040 (2)0.0367 (19)0.0122 (16)0.0019 (16)0.0011 (16)
C20.038 (3)0.031 (3)0.029 (2)0.004 (2)0.007 (2)0.000 (2)
C70.029 (2)0.025 (2)0.035 (3)0.0023 (18)0.003 (2)0.0038 (19)
Mn10.0358 (5)0.0297 (4)0.0240 (4)0.0009 (3)0.0017 (3)0.0011 (3)
O30.076 (3)0.050 (2)0.0314 (18)0.0133 (19)0.0128 (19)0.0118 (16)
C50.034 (3)0.038 (3)0.033 (2)0.004 (2)0.007 (2)0.002 (2)
C60.042 (3)0.038 (3)0.028 (3)0.006 (2)0.006 (2)0.006 (2)
C30.034 (3)0.030 (2)0.031 (2)0.0001 (19)0.006 (2)0.0046 (18)
C40.033 (3)0.033 (3)0.037 (2)0.006 (2)0.004 (2)0.003 (2)
C10.034 (3)0.029 (2)0.031 (2)0.0031 (19)0.003 (2)0.003 (2)
O60.081 (3)0.054 (2)0.056 (2)0.012 (2)0.035 (2)0.0026 (19)
O40.067 (3)0.049 (2)0.046 (2)0.0156 (19)0.012 (2)0.0177 (17)
O50.075 (3)0.052 (2)0.059 (2)0.023 (2)0.034 (2)0.0080 (19)
Geometric parameters (Å, º) top
C9—Mn12.612 (5)C14—H14C0.9700
C9—C5i1.520 (7)C14—H14D0.9700
C9—O61.237 (6)C14—C151.454 (18)
C9—O51.222 (6)C14—N21.499 (14)
O1—C7ii1.253 (5)C15—H15D0.9600
O1—Mn12.144 (3)C15—H15E0.9600
C8—Mn12.583 (5)C15—H15F0.9600
C8—O31.222 (6)C5—C9iv1.520 (7)
C8—C31.516 (7)C5—C6iii1.389 (7)
C8—O41.254 (6)C5—C41.400 (7)
O2—C71.266 (6)C6—C5v1.389 (7)
O2—Mn12.116 (3)C6—H60.9300
C2—H20.9300C6—C11.377 (7)
C2—C31.381 (7)C3—C41.390 (7)
C2—C1iii1.397 (6)C4—H40.9300
C7—O1ii1.253 (5)C1—C2v1.397 (6)
C7—C11.510 (6)C12—H120.9300
N1A—C11A1.328 (19)C12—C131.329 (13)
N1A—C12A1.382 (19)C12—N11.423 (12)
N1A—C10A1.46 (3)C13—H130.9300
Mn1—O32.228 (4)C13—N21.394 (13)
Mn1—O62.381 (4)C14A—H14A0.9700
Mn1—O42.303 (4)C14A—H14B0.9700
Mn1—O52.185 (4)C14A—C15A1.50 (2)
C10—H10D0.9600C14A—N2A1.470 (19)
C10—H10E0.9600C15A—H15A0.9600
C10—H10F0.9600C15A—H15B0.9600
C10—N11.416 (14)C15A—H15C0.9600
C11A—H11A0.9300N2—C111.185 (12)
C11A—N2A1.400 (19)C10A—H10A0.9600
C12A—H12A0.9300C10A—H10B0.9600
C12A—C13A1.372 (18)C10A—H10C0.9600
C13A—H13A0.9300C11—H110.9300
C13A—N2A1.388 (19)C11—N11.346 (12)
C5i—C9—Mn1171.8 (4)C15—C14—H14C109.6
O6—C9—Mn165.5 (3)C15—C14—H14D109.6
O6—C9—C5i118.2 (5)C15—C14—N2110.2 (12)
O5—C9—Mn156.3 (3)N2—C14—H14C109.6
O5—C9—C5i119.8 (5)N2—C14—H14D109.6
O5—C9—O6121.7 (5)C14—C15—H15D109.5
C7ii—O1—Mn1128.5 (3)C14—C15—H15E109.5
O3—C8—Mn159.5 (3)C14—C15—H15F109.5
O3—C8—C3119.8 (4)H15D—C15—H15E109.5
O3—C8—O4122.2 (5)H15D—C15—H15F109.5
C3—C8—Mn1172.5 (4)H15E—C15—H15F109.5
O4—C8—Mn163.0 (3)C8—O3—Mn192.3 (3)
O4—C8—C3117.9 (5)C6iii—C5—C9iv121.9 (5)
C7—O2—Mn1113.9 (3)C6iii—C5—C4119.4 (5)
C3—C2—H2119.7C4—C5—C9iv118.7 (5)
C3—C2—C1iii120.6 (4)C5v—C6—H6119.7
C1iii—C2—H2119.7C1—C6—C5v120.6 (5)
O1ii—C7—O2123.7 (4)C1—C6—H6119.7
O1ii—C7—C1118.5 (4)C2—C3—C8120.1 (4)
O2—C7—C1117.7 (4)C2—C3—C4119.5 (4)
C11A—N1A—C12A114.2 (19)C4—C3—C8120.3 (4)
C11A—N1A—C10A131 (3)C5—C4—H4119.9
C12A—N1A—C10A113 (3)C3—C4—C5120.1 (5)
O1—Mn1—C9110.94 (16)C3—C4—H4119.9
O1—Mn1—C8111.93 (15)C2v—C1—C7119.4 (4)
O1—Mn1—O383.72 (13)C6—C1—C2v119.6 (4)
O1—Mn1—O6133.08 (14)C6—C1—C7121.1 (4)
O1—Mn1—O4140.83 (13)C13—C12—H12124.5
O1—Mn1—O588.03 (15)C13—C12—N1111.1 (9)
C8—Mn1—C9120.88 (16)N1—C12—H12124.5
O2—Mn1—C9116.38 (16)C12—C13—H13128.3
O2—Mn1—O199.06 (14)C12—C13—N2103.3 (9)
O2—Mn1—C894.70 (15)N2—C13—H13128.3
O2—Mn1—O3100.25 (15)H14A—C14A—H14B108.7
O2—Mn1—O692.40 (15)C15A—C14A—H14A110.5
O2—Mn1—O490.57 (15)C15A—C14A—H14B110.5
O2—Mn1—O5138.42 (16)N2A—C14A—H14A110.5
O3—Mn1—C9136.53 (17)N2A—C14A—H14B110.5
O3—Mn1—C828.21 (14)N2A—C14A—C15A106 (5)
O3—Mn1—O6138.66 (16)C14A—C15A—H15A109.5
O3—Mn1—O457.16 (13)C14A—C15A—H15B109.5
O6—Mn1—C928.20 (15)C14A—C15A—H15C109.5
O6—Mn1—C8112.23 (16)H15A—C15A—H15B109.5
O4—Mn1—C998.01 (16)H15A—C15A—H15C109.5
O4—Mn1—C829.02 (14)H15B—C15A—H15C109.5
O4—Mn1—O683.76 (15)C9—O6—Mn186.3 (3)
O5—Mn1—C927.72 (15)C13—N2—C14122.3 (11)
O5—Mn1—C8120.60 (17)C11—N2—C14128.2 (11)
O5—Mn1—O3121.29 (17)C11—N2—C13109.5 (10)
O5—Mn1—O655.90 (14)N1A—C10A—H10A109.5
O5—Mn1—O4109.42 (17)N1A—C10A—H10B109.5
H10D—C10—H10E109.5N1A—C10A—H10C109.5
H10D—C10—H10F109.5H10A—C10A—H10B109.5
H10E—C10—H10F109.5H10A—C10A—H10C109.5
N1—C10—H10D109.5H10B—C10A—H10C109.5
N1—C10—H10E109.5N2—C11—H11121.4
N1—C10—H10F109.5N2—C11—N1117.2 (11)
N1A—C11A—H11A127.2N1—C11—H11121.4
N1A—C11A—N2A106 (2)C8—O4—Mn188.0 (3)
N2A—C11A—H11A127.2C9—O5—Mn196.0 (3)
N1A—C12A—H12A129.1C10—N1—C12127.2 (10)
C13A—C12A—N1A101.8 (17)C11—N1—C10134.0 (11)
C13A—C12A—H12A129.1C11—N1—C1298.8 (9)
C12A—C13A—H13A124.0C11A—N2A—C14A109 (3)
C12A—C13A—N2A111.9 (18)C13A—N2A—C11A105.3 (18)
N2A—C13A—H13A124.0C13A—N2A—C14A142 (3)
H14C—C14—H14D108.1
C9iv—C5—C4—C3174.7 (5)C5v—C6—C1—C2v1.8 (8)
O1ii—C7—C1—C2v164.5 (5)C5v—C6—C1—C7177.1 (4)
O1ii—C7—C1—C614.5 (7)C6iii—C5—C4—C34.1 (8)
C8—C3—C4—C5176.8 (5)C3—C8—O3—Mn1171.3 (4)
O2—C7—C1—C2v13.3 (7)C3—C8—O4—Mn1171.6 (4)
O2—C7—C1—C6167.7 (5)C1iii—C2—C3—C8179.7 (5)
C2—C3—C4—C53.1 (7)C1iii—C2—C3—C40.4 (7)
N1A—C11A—N2A—C13A10 (4)C12—C13—N2—C14179.5 (10)
N1A—C11A—N2A—C14A174 (4)C12—C13—N2—C111.5 (12)
N1A—C12A—C13A—N2A0 (4)C13—C12—N1—C10179.3 (13)
Mn1—O2—C7—O1ii13.2 (6)C13—C12—N1—C111.1 (12)
Mn1—O2—C7—C1164.4 (3)C13—N2—C11—N12.5 (15)
C11A—N1A—C12A—C13A7 (5)C15A—C14A—N2A—C11A99 (6)
C12A—N1A—C11A—N2A11 (5)C15A—C14A—N2A—C13A107 (7)
C12A—C13A—N2A—C11A7 (4)O6—C9—O5—Mn12.8 (6)
C12A—C13A—N2A—C14A161 (5)N2—C11—N1—C10179.7 (14)
C14—N2—C11—N1178.6 (11)N2—C11—N1—C122.2 (14)
C15—C14—N2—C1351.0 (16)C10A—N1A—C11A—N2A178 (6)
C15—C14—N2—C11127.7 (15)C10A—N1A—C12A—C13A176 (5)
O3—C8—C3—C26.4 (8)O4—C8—O3—Mn15.9 (6)
O3—C8—C3—C4173.5 (5)O4—C8—C3—C2170.9 (5)
O3—C8—O4—Mn15.7 (5)O4—C8—C3—C49.2 (7)
C5i—C9—O6—Mn1171.8 (4)O5—C9—O6—Mn12.6 (6)
C5i—C9—O5—Mn1171.5 (4)N1—C12—C13—N20.1 (11)
Symmetry codes: (i) x+3/2, y+1, z1/2; (ii) x+1, y+1, z+1; (iii) x+1, y1/2, z+3/2; (iv) x+3/2, y+1, z+1/2; (v) x+1, y+1/2, z+3/2.
(c340k) top
Crystal data top
C9H3MnO6·1(C6H11N2)Dx = 1.591 Mg m3
Mr = 373.22Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 1712 reflections
a = 15.0401 (7) Åθ = 2.4–29.3°
b = 12.5366 (5) ŵ = 0.88 mm1
c = 16.5320 (6) ÅT = 340 K
V = 3117.1 (2) Å3Prism, colorless
Z = 80.15 × 0.11 × 0.07 mm
F(000) = 1528
Data collection top
SuperNova, Single source at offset), Atlas
diffractometer
3747 independent reflections
Radiation source: SuperNova (Mo) X-ray Source1947 reflections with I > 2σ(I)
Detector resolution: 10.3590 pixels mm-1Rint = 0.073
ω scansθmax = 29.4°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro, Agilent Technologies, Version 1.171.35.8 (release 07-03-2011 CrysAlis171 .NET) (compiled Mar 7 2011,18:06:32) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1815
Tmin = 0.979, Tmax = 1.000k = 1613
11134 measured reflectionsl = 2219
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)] = 0.070Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.193H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0694P)2 + 1.6376P]
where P = (Fo2 + 2Fc2)/3
3747 reflections(Δ/σ)max = 0.006
213 parametersΔρmax = 0.56 e Å3
288 restraintsΔρmin = 0.53 e Å3
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
C90.7312 (3)0.5796 (4)0.5019 (3)0.0422 (12)
O10.5287 (2)0.3808 (2)0.50790 (18)0.0405 (8)
C80.6333 (3)0.4053 (4)0.7246 (3)0.0332 (10)
O20.4999 (2)0.5892 (2)0.62165 (19)0.0441 (8)
C20.5915 (3)0.2729 (3)0.8326 (3)0.0346 (11)
H20.55560.23900.79470.042*
C70.4612 (3)0.6398 (3)0.5662 (3)0.0324 (10)
N1A0.3739 (16)0.2614 (15)0.6707 (13)0.066 (5)*0.255 (9)
Mn10.60380 (5)0.48718 (5)0.58350 (4)0.0313 (3)
C10A0.377 (3)0.200 (3)0.6014 (18)0.090 (11)*0.255 (9)
H10A0.38430.24570.55520.136*0.255 (9)
H10B0.32350.15980.59630.136*0.255 (9)
H10C0.42710.15220.60460.136*0.255 (9)
C120.3439 (7)0.2539 (9)0.7807 (6)0.070 (3)*0.745 (9)
H120.32820.18480.79510.084*0.745 (9)
C130.3394 (8)0.3301 (9)0.8245 (8)0.086 (3)*0.745 (9)
H130.31610.33050.87660.103*0.745 (9)
C140.3810 (9)0.5205 (11)0.8100 (9)0.135 (5)*0.745 (9)
H14D0.40990.56150.76780.162*0.745 (9)
H14C0.32220.55030.81870.162*0.745 (9)
C150.4303 (13)0.5274 (17)0.8812 (13)0.221 (8)*0.745 (9)
H15D0.49210.51610.86930.331*0.745 (9)
H15E0.41030.47400.91860.331*0.745 (9)
H15F0.42260.59680.90470.331*0.745 (9)
O30.5928 (3)0.3554 (3)0.6734 (2)0.0594 (11)
C50.7018 (3)0.3698 (4)0.9444 (3)0.0372 (11)
C60.3477 (3)0.7807 (4)0.5345 (3)0.0377 (11)
H60.34310.75320.48240.045*
C30.6395 (3)0.3634 (4)0.8098 (3)0.0336 (10)
C40.6934 (3)0.4125 (4)0.8671 (3)0.0359 (11)
H40.72420.47430.85360.043*
C10.4037 (3)0.7323 (4)0.5894 (3)0.0315 (10)
C12A0.3994 (14)0.3687 (14)0.6734 (13)0.046 (5)*0.255 (9)
H12A0.42390.40530.62980.055*0.255 (9)
C13A0.3847 (17)0.4127 (15)0.7459 (14)0.048 (5)*0.255 (9)
H13A0.38720.48410.76080.058*0.255 (9)
C14A0.353 (4)0.349 (3)0.8789 (16)0.195 (16)*0.255 (9)
H14A0.36030.28250.90820.234*0.255 (9)
H14B0.29120.36950.88540.234*0.255 (9)
C15A0.407 (4)0.432 (5)0.924 (3)0.21 (2)*0.255 (9)
H15A0.46290.40110.94030.319*0.255 (9)
H15B0.37510.45450.97130.319*0.255 (9)
H15C0.41790.49190.88960.319*0.255 (9)
O60.6998 (3)0.6354 (3)0.5569 (2)0.0687 (12)
N20.3735 (5)0.4140 (7)0.7857 (6)0.075 (2)*0.745 (9)
C110.3922 (7)0.3850 (9)0.7118 (7)0.072 (3)*0.745 (9)
H110.41330.42960.67110.086*0.745 (9)
C11A0.3474 (18)0.2376 (18)0.7475 (14)0.063 (5)*0.255 (9)
H11A0.32210.17380.76480.075*0.255 (9)
O40.6680 (3)0.4933 (3)0.7097 (2)0.0569 (10)
O50.7069 (3)0.4888 (3)0.4906 (3)0.0674 (12)
N10.3765 (5)0.2846 (6)0.7046 (5)0.064 (2)*0.745 (9)
N2A0.365 (2)0.3236 (19)0.7937 (13)0.101 (6)*0.255 (9)
C100.3917 (12)0.2136 (15)0.6349 (11)0.144 (6)*0.745 (9)
H10D0.44150.16790.64590.217*0.745 (9)
H10E0.40380.25560.58770.217*0.745 (9)
H10F0.33970.17090.62580.217*0.745 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C90.041 (3)0.050 (3)0.035 (2)0.000 (2)0.001 (2)0.004 (2)
O10.053 (2)0.0370 (18)0.0317 (18)0.0033 (15)0.0030 (16)0.0078 (14)
C80.031 (2)0.037 (2)0.031 (2)0.0011 (18)0.0054 (18)0.0101 (18)
O20.055 (2)0.0401 (19)0.0375 (18)0.0163 (15)0.0052 (16)0.0034 (15)
C20.039 (3)0.034 (3)0.031 (2)0.0052 (19)0.007 (2)0.000 (2)
C70.035 (2)0.029 (2)0.033 (3)0.0022 (18)0.003 (2)0.0018 (19)
Mn10.0378 (4)0.0311 (4)0.0248 (4)0.0009 (3)0.0024 (3)0.0019 (3)
O30.091 (3)0.055 (2)0.0320 (17)0.0172 (19)0.0122 (19)0.0103 (16)
C50.038 (3)0.041 (3)0.033 (2)0.003 (2)0.010 (2)0.002 (2)
C60.046 (3)0.037 (3)0.029 (2)0.007 (2)0.007 (2)0.003 (2)
C30.032 (2)0.039 (3)0.030 (2)0.0024 (19)0.0007 (19)0.0056 (18)
C40.038 (3)0.033 (3)0.037 (2)0.004 (2)0.002 (2)0.0014 (19)
C10.035 (2)0.029 (2)0.030 (2)0.0008 (18)0.002 (2)0.0020 (19)
O60.090 (3)0.058 (2)0.059 (2)0.013 (2)0.040 (2)0.0002 (19)
O40.073 (3)0.053 (2)0.045 (2)0.0158 (18)0.0111 (19)0.0173 (17)
O50.084 (3)0.057 (2)0.061 (2)0.029 (2)0.036 (2)0.0077 (19)
Geometric parameters (Å, º) top
C9—Mn12.614 (5)Mn1—O52.182 (4)
C9—C5i1.523 (7)C12—C131.200 (14)
C9—O61.240 (6)C12—N11.404 (11)
C9—O51.211 (6)C13—N21.334 (13)
O1—C7ii1.261 (5)C14—C151.39 (2)
O1—Mn12.148 (3)C14—N21.399 (14)
C8—Mn12.587 (4)C5—C9iv1.523 (7)
C8—O31.215 (5)C5—C6iii1.388 (6)
C8—C31.507 (6)C5—C41.391 (6)
C8—O41.245 (5)C6—C5v1.388 (6)
O2—C71.257 (5)C6—C11.379 (6)
O2—Mn12.116 (3)C3—C41.390 (6)
C2—C31.396 (6)C1—C2v1.389 (6)
C2—C1iii1.389 (6)C12A—C13A1.338 (17)
C7—O1ii1.261 (5)C13A—N2A1.401 (17)
C7—C11.496 (6)C14A—C15A1.52 (2)
N1A—C10A1.38 (3)C14A—N2A1.455 (17)
N1A—C12A1.401 (17)N2—C111.306 (12)
N1A—C11A1.364 (18)C11—N11.286 (11)
Mn1—O32.228 (3)C11A—N2A1.346 (17)
Mn1—O62.394 (4)N1—C101.473 (18)
Mn1—O42.300 (4)
C5i—C9—Mn1172.4 (4)O4—Mn1—C998.38 (15)
O6—C9—Mn166.0 (3)O4—Mn1—C828.77 (13)
O6—C9—C5i118.3 (5)O4—Mn1—O683.55 (14)
O5—C9—Mn156.0 (3)O5—Mn1—C927.39 (14)
O5—C9—C5i119.7 (5)O5—Mn1—C8121.09 (16)
O5—C9—O6121.9 (5)O5—Mn1—O3121.94 (16)
C7ii—O1—Mn1129.0 (3)O5—Mn1—O655.60 (13)
O3—C8—Mn159.4 (2)O5—Mn1—O4109.88 (16)
O3—C8—C3120.2 (4)C13—C12—N1110.0 (10)
O3—C8—O4121.9 (4)C12—C13—N2108.4 (12)
C3—C8—Mn1172.8 (3)C15—C14—N2110.1 (14)
O4—C8—Mn162.7 (2)C8—O3—Mn192.6 (3)
O4—C8—C3117.9 (4)C6iii—C5—C9iv122.2 (4)
C7—O2—Mn1115.4 (3)C6iii—C5—C4119.5 (4)
C1iii—C2—C3121.5 (4)C4—C5—C9iv118.3 (4)
O1ii—C7—C1118.5 (4)C1—C6—C5v121.1 (4)
O2—C7—O1ii123.3 (4)C2—C3—C8120.3 (4)
O2—C7—C1118.2 (4)C4—C3—C8121.2 (4)
C10A—N1A—C12A123.4 (19)C4—C3—C2118.5 (4)
C11A—N1A—C10A132 (2)C3—C4—C5120.6 (4)
C11A—N1A—C12A105.1 (16)C2v—C1—C7119.4 (4)
O1—Mn1—C9111.11 (15)C6—C1—C2v118.8 (4)
O1—Mn1—C8111.61 (14)C6—C1—C7121.7 (4)
O1—Mn1—O383.62 (13)C13A—C12A—N1A112.3 (16)
O1—Mn1—O6133.78 (13)C12A—C13A—N2A102.3 (15)
O1—Mn1—O4140.27 (12)N2A—C14A—C15A124 (4)
O1—Mn1—O588.26 (14)C9—O6—Mn185.8 (3)
C8—Mn1—C9121.04 (15)C13—N2—C14130.3 (11)
O2—Mn1—C9115.31 (15)C11—N2—C13108.2 (9)
O2—Mn1—O199.21 (12)C11—N2—C14121.1 (10)
O2—Mn1—C895.62 (14)N1—C11—N2108.6 (9)
O2—Mn1—O3101.20 (14)N2A—C11A—N1A107.3 (18)
O2—Mn1—O691.80 (14)C8—O4—Mn188.5 (3)
O2—Mn1—O491.11 (14)C9—O5—Mn196.6 (3)
O2—Mn1—O5136.81 (15)C12—N1—C10126.1 (10)
O3—Mn1—C9136.67 (16)C11—N1—C12104.4 (9)
O3—Mn1—C827.99 (13)C11—N1—C10129.5 (11)
O3—Mn1—O6137.97 (15)C13A—N2A—C14A113.4 (18)
O3—Mn1—O456.70 (13)C11A—N2A—C13A111.1 (16)
O6—Mn1—C928.24 (14)C11A—N2A—C14A135 (2)
O6—Mn1—C8111.74 (15)
Symmetry codes: (i) x+3/2, y+1, z1/2; (ii) x+1, y+1, z+1; (iii) x+1, y1/2, z+3/2; (iv) x+3/2, y+1, z+1/2; (v) x+1, y+1/2, z+3/2.
 

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