supplementary materials


Acta Cryst. (2007). E63, m1562    [ doi:10.1107/S1600536807020831 ]

catena-Poly[[(1,10-phenanthroline-[kappa]2N,N')cadmate(II)]-di-[mu]-bromido]

B.-S. Zhang

Abstract top

The title compound, [CdBr2(C12H8N2)]n, is a 1:1 adduct of cadmium bromide with 1,10-phenanthroline (phen), which contains an infinite chain consisting of Cd2Br2 parallelograms sharing the Cd coners. The chain propagates along the c axis. Both the CdII atom and the phen molecule lie on a twofold rotation axis. The CdII atom is coordinated by two N atoms from a chelating phen ligand and four Br atoms to complete a distorted octahedral geometry. The closest atom-to-atom distance of 3.35 (1) Å between the phen ligands of two adjacent chains indicates the existence of [pi]-[pi] interactions, which result in a two-dimensional layer parallel to the bc plane. The layers are associated through weak C-H...Br hydrogen bonds.

Comment top

Polynuclear d10 metal complexes have been found to exhibit intriguing structural and photoluminescent properties. Cl-bridged CdII polymeric complexes are of considerable interest because they may act as photoactive materials. Structures of Cl-bridged CdII polymeric complexes have been studied (Bell et al., 1982; Bigoli et al., 1983; Bonomo et al., 1989; Huang et al., 1998). However, CdII polymeric complexes with a CdBr2N2 coordination polydedron have been rarely reported. The phosphorescence and zero-field optically detected magnetic resonance studies with powder of CdX2(phen), (phen = 1,10-phenanthroline; X = Cl, Br, and I) (Kimachi et al., 1995) and the crystal structures of CdCl2(phen) and CdCl2 (2,2'-bipyridine) have been reported (Chen et al., 2003; Zhou et al., 2003). We have introduced Br- ion as a bridging ligand, and synthesized the Br-bridged Cd complex, [CdBr2(phen)]n, (I), by a hydrothermal reaction.

The structure of compound (I) (Fig. 1), contains one-dimensional chains extending in the c direction (Fig 2). Both CdII atom and phen molecule lie on the twofold rotation axis. The CdII atom is coordinated by two N atoms from a chelating phen ligand and four Br atoms to complete a distorted CdN2Br4 octahedral geometry. The average Cd—N bond length is 2.350 (3) Å and the bond lengths of Cd—Br are 2.6813 (5)Å and 2.9003 (5) Å. The Cd···Cd distance in the chain is 4.047 (1) Å, which is longer than that of the Cl-bridged Cd complex [3.931 (9) Å]. The closest atom-to-atom distance of 3.35 (1)Å between the phen ligands of two adjacent chains indicates the existence of ππ interactions, which result in a two-dimensional layer parallel to the bc plane (Fig. 3). The layers are associated through weak C—H···Br hydrogen bonds (Table 1).

Related literature top

For related literature, see: Bell et al. (1982); Bigoli et al. (1983); Bonomo et al. (1989); Huang et al. (1998); Kimachi et al. (1995); Chen et al. (2003); Zhou et al. (2003).

Experimental top

Freshly prepared CdCO3 (0.14 g, 0.812 mmol), phen.H2O (0.10 g, 0.505 mmol), 2-bromobenzoic acid (0.10 g, 0.498 mmol), CH3OH/H2O (12 ml; v/v=1:2) were mixed and stirred for 2 h. The resulting suspension was heated in a 23 ml Teflon-lined stainless steel autoclave at 393 K for 7 d. After the autoclave was cooled to room temperature, colorless block crystals suitable for X-ray analysis were obtained.

Refinement top

All H atoms were positioned geometrically and treated as riding atoms, with C—H = 0.96 Å and Uiso(H) = 1.2Ueq(C).

Computing details top

Data collection: SMART (Bruker, 1998); cell refinement: SMART; data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Bruker, 1998); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. The structure of (I), showing the coordination geometry of Cd II atom. Displacement ellipsoids are drawn at the 40% probability level. H atoms have been omitted for clarity. [symmetry codes: (i) 1 - x, y, 1/2 - z; (ii) 1 - x, 1 - y, 1 - z; (iii) 1 - x, 1 - y, -z; (iv) x, 1 - y, z - 1/2.]
[Figure 2] Fig. 2. A view of the one-dimensional chain along the c axis in (I). H atoms have been omitted for clarity.
[Figure 3] Fig. 3. A packing diagram for (I), viewed down the c axis. Dashed lines indicate hydrogen bonds.
catena-Poly[[(1,10-phenanthroline-κ2N,N')cadmate(II)]-di-µ-bromido] top
Crystal data top
[CdBr2(C12H8N2)]F(000) = 848
Mr = 452.42Dx = 2.368 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 961 reflections
a = 16.7781 (7) Åθ = 2.3–26.0°
b = 10.7594 (7) ŵ = 7.99 mm1
c = 7.4213 (3) ÅT = 290 K
β = 108.664 (4)°Block, colourless
V = 1269.26 (11) Å30.23 × 0.12 × 0.10 mm
Z = 4
Data collection top
Bruker SMART CCD area-detector
diffractometer
1247 independent reflections
Radiation source: fine-focus sealed tube998 reflections with I > 2σ(I)
graphiteRint = 0.039
φ and ω scansθmax = 26.0°, θmin = 2.3°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 2018
Tmin = 0.340, Tmax = 0.511k = 1310
7231 measured reflectionsl = 99
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.029H-atom parameters constrained
wR(F2) = 0.067 w = 1/[σ2(Fo2) + 3.3613P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
1247 reflectionsΔρmax = 0.59 e Å3
79 parametersΔρmin = 0.46 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00093 (19)
Crystal data top
[CdBr2(C12H8N2)]V = 1269.26 (11) Å3
Mr = 452.42Z = 4
Monoclinic, C2/cMo Kα radiation
a = 16.7781 (7) ŵ = 7.99 mm1
b = 10.7594 (7) ÅT = 290 K
c = 7.4213 (3) Å0.23 × 0.12 × 0.10 mm
β = 108.664 (4)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
1247 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
998 reflections with I > 2σ(I)
Tmin = 0.340, Tmax = 0.511Rint = 0.039
7231 measured reflectionsθmax = 26.0°
Refinement top
R[F2 > 2σ(F2)] = 0.029H-atom parameters constrained
wR(F2) = 0.067Δρmax = 0.59 e Å3
S = 1.06Δρmin = 0.46 e Å3
1247 reflectionsAbsolute structure: ?
79 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Cd10.50000.42497 (3)0.25000.04136 (18)
Br10.60185 (3)0.58225 (4)0.49961 (6)0.04905 (19)
N10.4258 (2)0.2472 (3)0.1038 (5)0.0462 (9)
C10.3527 (3)0.2477 (6)0.0359 (8)0.0699 (15)
H10.32910.32530.09190.084*
C20.3095 (5)0.1378 (9)0.1055 (11)0.105 (3)
H20.25630.14060.20500.125*
C30.3414 (7)0.0289 (8)0.0353 (13)0.112 (4)
H30.30950.04520.08120.135*
C40.4194 (6)0.0225 (5)0.1050 (10)0.085 (2)
C50.4646 (8)0.0905 (4)0.1855 (12)0.131 (7)
H50.43910.16950.14170.157*
C60.4603 (3)0.1372 (4)0.1760 (6)0.0534 (13)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cd10.0494 (3)0.0298 (2)0.0357 (3)0.0000.00083 (19)0.000
Br10.0535 (4)0.0480 (3)0.0414 (3)0.0127 (2)0.0092 (2)0.00875 (17)
N10.049 (2)0.044 (2)0.051 (2)0.0127 (17)0.0228 (18)0.0174 (16)
C10.053 (3)0.093 (4)0.065 (3)0.018 (3)0.021 (3)0.037 (3)
C20.074 (5)0.157 (7)0.096 (5)0.061 (5)0.044 (4)0.083 (5)
C30.150 (8)0.110 (6)0.120 (6)0.090 (6)0.103 (6)0.083 (6)
C40.149 (7)0.049 (3)0.099 (5)0.049 (4)0.098 (5)0.039 (3)
C50.29 (2)0.032 (3)0.151 (11)0.038 (5)0.178 (12)0.027 (3)
C60.082 (4)0.035 (2)0.064 (3)0.018 (2)0.052 (2)0.0149 (19)
Geometric parameters (Å, °) top
Cd1—N12.349 (3)C1—H10.9600
Cd1—N1i2.349 (3)C2—C31.323 (12)
Cd1—Br12.6813 (5)C2—H20.9600
Cd1—Br1i2.6813 (5)C3—C41.389 (11)
Cd1—Br1ii2.9003 (5)C3—H30.9600
Cd1—Br1iii2.9003 (5)C4—C61.429 (7)
Br1—Cd1ii2.9003 (5)C4—C51.456 (11)
N1—C11.328 (6)C5—C5i1.27 (2)
N1—C61.351 (6)C5—H50.9600
C1—C21.396 (8)C6—C6i1.429 (10)
N1—Cd1—N1i71.03 (19)N1—C1—C2121.7 (6)
N1—Cd1—Br1163.57 (9)N1—C1—H1119.4
N1i—Cd1—Br193.92 (10)C2—C1—H1118.9
N1—Cd1—Br1i93.92 (10)C3—C2—C1120.5 (7)
N1i—Cd1—Br1i163.57 (9)C3—C2—H2119.3
Br1—Cd1—Br1i101.73 (2)C1—C2—H2120.2
N1—Cd1—Br1ii86.58 (9)C2—C3—C4120.3 (6)
N1i—Cd1—Br1ii90.92 (9)C2—C3—H3119.1
Br1—Cd1—Br1ii87.145 (15)C4—C3—H3120.6
Br1i—Cd1—Br1ii94.797 (16)C3—C4—C6117.4 (7)
N1—Cd1—Br1iii90.92 (9)C3—C4—C5126.3 (7)
N1i—Cd1—Br1iii86.58 (9)C6—C4—C5116.4 (8)
Br1—Cd1—Br1iii94.797 (16)C5i—C5—C4123.4 (5)
Br1i—Cd1—Br1iii87.145 (15)C5i—C5—H5117.7
Br1ii—Cd1—Br1iii176.93 (2)C4—C5—H5118.9
Cd1—Br1—Cd1ii92.855 (15)N1—C6—C6i118.7 (3)
C1—N1—C6119.0 (4)N1—C6—C4121.1 (6)
C1—N1—Cd1125.3 (3)C6i—C6—C4120.2 (4)
C6—N1—Cd1115.7 (3)
Symmetry codes: (i) −x+1, y, −z+1/2; (ii) −x+1, −y+1, −z+1; (iii) x, −y+1, z−1/2.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C2—H2···Br1iv0.962.883.816 (12)166
C5—H5···Br1v0.962.873.815 (5)167
Symmetry codes: (iv) x−1/2, y−1/2, z−1; (v) −x+1, y−1, −z+1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C2—H2···Br1i0.962.883.816 (12)166
C5—H5···Br1ii0.962.873.815 (5)167
Symmetry codes: (i) x−1/2, y−1/2, z−1; (ii) −x+1, y−1, −z+1/2.
Acknowledgements top

The author gratefully acknowledges the financial support of the Education Office of Zhejiang Province (grant No. 20051316).

references
References top

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