Literature DB >> 23468682

Poly[[μ-N,N'-bis-(2-hy-droxy-eth-yl)-N,N,N',N'-tetra-methyl-propane-1,3-diaminium-κ(2) O:O']tetra-μ-bromido-dibromidodimanganese(II)].

Heikki Rinta1, Anssi Peuronen, Manu Lahtinen.   

Abstract

The asymmetric unit of the title three-dimensional coordination polymer, [Mn2Br6(C11H28N2O2)] n , consists of one Mn(II) cation, half of a dicationic N,N'-bis-(2-hy-droxy-eth-yl)-N,N,N',N'-tetra-methyl-propane-1,3-diaminium ligand (L) (the other half being generated by a twofold rotation axis), and three bromide ions. The Mn(II) cation is coordinated by a single L ligand via the hy-droxy O atom and by five bromide ions, resulting in a distorted octa-hedral MnBr5O coordination geometry. Four of the bromide ions are bridging to two adjacent Mn(II) atoms, thereby forming polymeric chains along the a and b axes. The L units act as links between neighbouring Mn-(μ-Br)2-Mn chains, also forming a polymeric continuum along the c axis, which completes the formation of a three-dimensional network. Classical O-H⋯Br hydrogen bonds are present. The distance between adjacent Mn(II) atoms is 4.022 (1) Å.

Entities:  

Year:  2012        PMID: 23468682      PMCID: PMC3588717          DOI: 10.1107/S1600536812044765

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


Related literature

For related structures of M II transition metal halide one-dimensional coordination polymers, see: Han et al. (2012 ▶); Englert & Schiffers (2006 ▶). For two-dimensional networks, see: Hu & Englert (2006 ▶); Turgunov et al. (2011 ▶). For properties of metal halides, see: Hitchcock et al. (2003 ▶); Wang et al. (2011 ▶). For ligand conformations, see: Kärnä et al. (2010 ▶).

Experimental

Crystal data

[Mn2Br6(C11H28N2O2)] M = 809.69 Tetragonal, a = 8.0163 (4) Å c = 35.3103 (18) Å V = 2269.1 (2) Å3 Z = 4 Mo Kα radiation μ = 11.69 mm−1 T = 123 K 0.25 × 0.25 × 0.20 mm

Data collection

Bruker–NoniusKappa APEXII diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 2008a ▶) T min = 0.440, T max = 0.746 5076 measured reflections 1966 independent reflections 1856 reflections with I > 2σ(I) R int = 0.032

Refinement

R[F 2 > 2σ(F 2)] = 0.021 wR(F 2) = 0.047 S = 1.02 1966 reflections 111 parameters 1 restraint H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.36 e Å−3 Δρmin = −0.41 e Å−3 Absolute structure: Flack (1983 ▶), 690 Friedel pairs Flack parameter: 0.048 (14) Data collection: COLLECT (Bruker, 2008 ▶); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997 ▶); data reduction: DENZO-SMN; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008b ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008b ▶); molecular graphics: Mercury (Macrae et al., 2008 ▶); software used to prepare material for publication: SHELXL97. Click here for additional data file. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812044765/fj2604sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812044765/fj2604Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Mn2Br6(C11H28N2O2)]Dx = 2.370 Mg m3
Mr = 809.69Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P43212Cell parameters from 1871 reflections
Hall symbol: P 4nw 2abwθ = 0.4–27.9°
a = 8.0163 (4) ŵ = 11.69 mm1
c = 35.3103 (18) ÅT = 123 K
V = 2269.1 (2) Å3Block, violet
Z = 40.25 × 0.25 × 0.20 mm
F(000) = 1536
Bruker–NoniusKappa APEXII diffractometer1966 independent reflections
Radiation source: fine-focus sealed tube1856 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.032
Detector resolution: 9 pixels mm-1θmax = 25.0°, θmin = 2.8°
φ and ω scansh = −9→9
Absorption correction: multi-scan (SADABS; Sheldrick, 2008a)k = −4→9
Tmin = 0.440, Tmax = 0.746l = −22→41
5076 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.021H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.047w = 1/[σ2(Fo2) + (0.P)2] where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
1966 reflectionsΔρmax = 0.36 e Å3
111 parametersΔρmin = −0.41 e Å3
1 restraintAbsolute structure: Flack (1983), 690 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.048 (14)
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/UeqOcc. (<1)
C20.8227 (5)0.8960 (5)0.15487 (11)0.0158 (9)
H2A0.83790.85070.12900.019*
H2B0.70310.92360.15800.019*
C30.8705 (5)0.7633 (5)0.18350 (10)0.0143 (9)
H3A0.83400.65380.17350.017*
H3B0.99370.76050.18530.017*
C50.6146 (5)0.7687 (6)0.22206 (11)0.0197 (10)
H5A0.58250.66440.20950.030*
H5B0.56800.86340.20810.030*
H5C0.57130.76930.24800.030*
C60.8652 (5)0.6412 (5)0.24628 (11)0.0172 (10)
H6A0.82500.65310.27240.026*
H6B0.98740.64230.24610.026*
H6C0.82500.53560.23570.026*
C70.8412 (5)0.9495 (5)0.24099 (11)0.0116 (9)
H7A0.77640.96030.26470.014*
H7B0.80491.03960.22370.014*
C81.0268 (5)0.9732 (5)0.25000.0140 (13)
H8A1.05940.90390.27200.017*0.50
H8B1.09610.94060.22800.017*0.50
N40.8013 (4)0.7825 (4)0.22294 (9)0.0130 (8)
O10.9205 (3)1.0470 (4)0.15874 (8)0.0140 (6)
Br10.61915 (5)1.32320 (5)0.175357 (11)0.01348 (10)
Br21.13256 (5)1.39037 (5)0.167113 (10)0.01205 (10)
Br30.81111 (5)1.55274 (5)0.090982 (11)0.01279 (11)
Mn10.87136 (8)1.27065 (7)0.124710 (17)0.01152 (14)
H11.010 (3)1.021 (5)0.1575 (13)0.017*
U11U22U33U12U13U23
C20.024 (2)0.0120 (19)0.011 (2)−0.004 (2)−0.003 (2)−0.0030 (18)
C30.021 (2)0.014 (2)0.009 (2)0.001 (2)0.0015 (19)0.0001 (17)
C50.013 (2)0.025 (2)0.021 (2)−0.001 (2)0.001 (2)−0.006 (2)
C60.023 (2)0.013 (2)0.015 (2)−0.0018 (19)−0.0049 (19)0.0016 (18)
C70.015 (2)0.0074 (18)0.012 (2)−0.0020 (19)−0.0027 (18)−0.0025 (17)
C80.0114 (19)0.0114 (19)0.019 (3)0.002 (3)0.0015 (19)0.0015 (19)
N40.0139 (16)0.0157 (17)0.0094 (17)0.0011 (16)−0.0017 (14)0.0004 (15)
O10.0105 (14)0.0137 (14)0.0178 (15)0.0010 (13)0.0016 (14)0.0026 (14)
Br10.01241 (19)0.0168 (2)0.01122 (19)−0.00105 (19)0.00124 (18)−0.00200 (18)
Br20.01210 (19)0.01371 (19)0.01035 (19)0.00068 (18)0.00073 (16)0.00004 (17)
Br30.01400 (19)0.01200 (19)0.0124 (2)−0.00096 (19)−0.00056 (18)0.00178 (17)
Mn10.0117 (3)0.0115 (3)0.0113 (3)−0.0001 (3)0.0003 (3)0.0014 (3)
C2—O11.449 (5)C7—C81.533 (5)
C2—C31.517 (5)C7—H7A0.9900
C2—H2A0.9900C7—H7B0.9900
C2—H2B0.9900C8—C7i1.533 (5)
C3—N41.507 (4)C8—H8A0.9900
C3—H3A0.9900C8—H8B0.9900
C3—H3B0.9900O1—Mn12.194 (3)
C5—N41.501 (5)O1—H10.748 (19)
C5—H5A0.9800Br1—Mn12.7319 (7)
C5—H5B0.9800Br1—Mn1ii2.7635 (7)
C5—H5C0.9800Br2—Mn1iii2.7407 (7)
C6—N41.491 (5)Br2—Mn12.7472 (8)
C6—H6A0.9800Br3—Mn12.6010 (7)
C6—H6B0.9800Mn1—Br2ii2.7407 (7)
C6—H6C0.9800Mn1—Br1iii2.7635 (7)
C7—N41.517 (5)
O1—C2—C3112.7 (3)C7i—C8—H8A110.4
O1—C2—H2A109.0C7—C8—H8A110.4
C3—C2—H2A109.0C7i—C8—H8B110.4
O1—C2—H2B109.0C7—C8—H8B110.4
C3—C2—H2B109.0H8A—C8—H8B108.6
H2A—C2—H2B107.8C6—N4—C5107.3 (3)
N4—C3—C2116.8 (3)C6—N4—C3107.9 (3)
N4—C3—H3A108.1C5—N4—C3109.9 (3)
C2—C3—H3A108.1C6—N4—C7111.4 (3)
N4—C3—H3B108.1C5—N4—C7106.5 (3)
C2—C3—H3B108.1C3—N4—C7113.6 (3)
H3A—C3—H3B107.3C2—O1—Mn1122.3 (2)
N4—C5—H5A109.5C2—O1—H1106 (4)
N4—C5—H5B109.5Mn1—O1—H1112 (4)
H5A—C5—H5B109.5Mn1—Br1—Mn1ii94.082 (12)
N4—C5—H5C109.5Mn1iii—Br2—Mn194.254 (12)
H5A—C5—H5C109.5O1—Mn1—Br3174.03 (8)
H5B—C5—H5C109.5O1—Mn1—Br184.28 (8)
N4—C6—H6A109.5Br3—Mn1—Br191.62 (2)
N4—C6—H6B109.5O1—Mn1—Br2ii92.05 (8)
H6A—C6—H6B109.5Br3—Mn1—Br2ii91.89 (2)
N4—C6—H6C109.5Br1—Mn1—Br2ii84.75 (2)
H6A—C6—H6C109.5O1—Mn1—Br281.38 (8)
H6B—C6—H6C109.5Br3—Mn1—Br295.01 (2)
N4—C7—C8113.7 (3)Br1—Mn1—Br298.83 (2)
N4—C7—H7A108.8Br2ii—Mn1—Br2172.12 (3)
C8—C7—H7A108.8O1—Mn1—Br1iii89.94 (8)
N4—C7—H7B108.8Br3—Mn1—Br1iii94.43 (2)
C8—C7—H7B108.8Br1—Mn1—Br1iii173.07 (2)
H7A—C7—H7B107.7Br2ii—Mn1—Br1iii91.67 (2)
C7i—C8—C7106.5 (4)Br2—Mn1—Br1iii84.03 (2)
O1—C2—C3—N479.7 (4)C2—O1—Mn1—Br2179.1 (3)
N4—C7—C8—C7i167.0 (4)C2—O1—Mn1—Br1iii−96.9 (3)
C2—C3—N4—C6−179.3 (3)Mn1ii—Br1—Mn1—O1−105.44 (8)
C2—C3—N4—C564.0 (5)Mn1ii—Br1—Mn1—Br378.92 (2)
C2—C3—N4—C7−55.2 (5)Mn1ii—Br1—Mn1—Br2ii−12.838 (12)
C8—C7—N4—C654.1 (4)Mn1ii—Br1—Mn1—Br2174.24 (3)
C8—C7—N4—C5170.8 (3)Mn1iii—Br2—Mn1—O178.06 (8)
C8—C7—N4—C3−68.1 (4)Mn1iii—Br2—Mn1—Br3−106.73 (2)
C3—C2—O1—Mn1−175.3 (2)Mn1iii—Br2—Mn1—Br1160.85 (3)
C2—O1—Mn1—Br179.3 (3)Mn1iii—Br2—Mn1—Br1iii−12.785 (11)
C2—O1—Mn1—Br2ii−5.2 (3)
D—H···AD—HH···AD···AD—H···A
O1—H1···Br3iii0.75 (2)2.49 (2)3.232 (3)175 (5)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
O1—H1⋯Br3i 0.75 (2)2.49 (2)3.232 (3)175 (5)

Symmetry code: (i) .

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