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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 4;67(Pt 1):m9–m10. doi: 10.1107/S160053681004969X

Bromidotricarbon­yl[2-(pyridin-2-yl-κN)-5-p-tolyl-1,3,4-oxadiazole-κN 3]rhenium(I) dichloro­methane monosolvate

Lin-Fang Shi a,*, Yan-wei Li b, Zhen-jun Si c, Ying Guan a, Hua-ru Cao a
PMCID: PMC3050244  PMID: 21522604

Abstract

In the title compound, [ReBr(C14H11N3O)(CO)3]·CH2Cl2, the coordination geometry of the ReI atom is a distorted ReC3N2Br octa­hedron with the carbonyl C atoms in a fac arrangement. Within the 2-(pyridin-2-yl)-5-p-tolyl-1,3,4-oxadiazole ligand, the dihedral angles between the oxadiazole ring and the pyridine (py) and benzene (bz) rings are 1.7 (2) and 7.1 (2)°, respectively, and the dihedral angle between the py and bz rings is 5.5 (2)°. In the crystal, aromatic π–π stacking between the oxadiazole rings of adjacent mol­ecules [centroid–centroid separation = 3.465 (3) Å] is seen.

Related literature

For backgroud to phospho­resence in Re(I) complexes, see: Ley et al. (1997 ▶); Zhang et al. (2009 ▶). For a related structure, see: Rajendran et al. (2000 ▶). For the synthesis of the ligand, see: Demko & Sharpless (2001 ▶); Tamoto et al. (1997 ▶).graphic file with name e-67-000m9-scheme1.jpg

Experimental

Crystal data

  • [ReBr(C14H11N3O)(CO)3]·CH2Cl2

  • M r = 672.32

  • Monoclinic, Inline graphic

  • a = 12.590 (3) Å

  • b = 19.621 (4) Å

  • c = 17.660 (4) Å

  • β = 101.77 (3)°

  • V = 4270.8 (15) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 7.84 mm−1

  • T = 293 K

  • 0.25 × 0.22 × 0.11 mm

Data collection

  • Bruker SMART CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2002) ▶ T min = 0.149, T max = 0.409

  • 20653 measured reflections

  • 4847 independent reflections

  • 4254 reflections with I > 2σ(I)

  • R int = 0.063

Refinement

  • R[F 2 > 2σ(F 2)] = 0.040

  • wR(F 2) = 0.103

  • S = 1.05

  • 4847 reflections

  • 262 parameters

  • H-atom parameters constrained

  • Δρmax = 2.07 e Å−3

  • Δρmin = −2.88 e Å−3

Data collection: SMART (Bruker, 2002 ▶); cell refinement: SAINT (Bruker, 2002 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681004969X/hb5758sup1.cif

e-67-000m9-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681004969X/hb5758Isup2.hkl

e-67-000m9-Isup2.hkl (237.5KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

Re1—C1 1.887 (6)
Re1—C2 1.921 (5)
Re1—C3 1.890 (5)
Re1—N1 2.228 (4)
Re1—N2 2.169 (4)
Re1—Br1 2.6146 (11)

Acknowledgments

This work was supported by Zhejiang A & F University Science Foundation (2009FR068).

supplementary crystallographic information

Comment

As part of our studies of possible phosphorescent materials containing Re(I) (Ley et al., 1997), we have synthesized the title Re(I) complex, (I), which contain the oxadiazole ligand of 2-(pyridin-2-yl)-5-p-tolyl-1,3,4-oxadiazole and characterized its structure by single-crystal X-ray diffraction analysis. Its luminescent property will be further studied in the coming research.

As shown in Scheme 1 and Figure 1, [Re(CO)3(L)Br].CH2Cl2 is a six-coordinated complex. The coordination geometry at the Re atom is a distorted octahedron with the three carbonyl ligands arranged in a facial fashion. The distances of C(1), C(2), and C(3) to Re(1) are 1.887 (6), 1.921 (5), and 1.890 (5), respectively, and the Re—N bonds distances are 2.228 (4) and 2.169 (4). The bond angles in Table 1 clearly indicate that the CO ligands are linearly coordinated. The bond angles between adjacent CO carbon atoms are 87.8 (3), 89.1 (3) and 89.2 (3) degree, respectively, which is close to 90 degree, but the bond angle between the coordinated nitrogen atoms of ligand is 73.26 (16), which is much less than 90. All other bond distances and angles are comparable to those found for the related Re(I) complexes (Rajendran et al., 2000).

Figure 2 displays inter-molecular face-to-face stacking present in the molecular structure of [Re(CO)3(L)Br].CH2Cl2: the 1,3,4-oxadiazole moiety in one molecule is almost parallel to the other one from another complex molecule (the dihedral angle between the two planes is 1.65 degree), and the approximate distance between the two closest atoms (N2—N3) is only 3.349. Thus the complex molecule achieved a bonded dual-molecule structure which is believed a rigid one and will prevent geometric relaxation effectively (Zhang et al., 2009). This kind of rigid structure is expected possessing excellent luminescent properties.

Experimental

The oxadiazole ligand was synthesized according to the literature method (Demko et al., 2001; Tamoto et al., 1997) with some minor modification.[Re(CO)3(L)Br] was synthesized according to the following procedure: L1 (0.06 g, 0.210 mmol) and Re(CO)5Br (0.08 g, 0.200 mmol) were refluxed in 15 ml of toluene for 6 h. After the mixture was cooled to RT, the solvent was removed in a water bath under reduced pressure. The resulting yellow solid was purified by silica gel column chromatography with acetic acid ethyl ester and dichloromethane (v/v = 10:1). Yellow blocks of (I) were grown from slow evaporation of a CH2Cl2 solution.

Refinement

All H atoms were placed geometrically (N—H = 0.86, C—H = 0.93 Å) and refined as riding with Uiso(H)= 1.2Ueq(carrier).

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of [Re(CO)3(L)Br].CH2Cl2, with displacement ellipsoids drawn at the 30% probability level (arbitrary spheres for the H atoms).

Fig. 2.

Fig. 2.

A view of inter-molecular face-to-face stacking structure of (I).

Crystal data

[ReBr(C14H11N3O)(CO)3]·CH2Cl2 F(000) = 2544
Mr = 672.32 Dx = 2.091 Mg m−3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 4847 reflections
a = 12.590 (3) Å θ = 3.1–24.8°
b = 19.621 (4) Å µ = 7.84 mm−1
c = 17.660 (4) Å T = 293 K
β = 101.77 (3)° Block, yellow
V = 4270.8 (15) Å3 0.25 × 0.22 × 0.11 mm
Z = 8

Data collection

Bruker SMART CCD diffractometer 4847 independent reflections
Radiation source: fine-focus sealed tube 4254 reflections with I > 2σ(I)
graphite Rint = 0.063
phi and ω scans θmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan (SADABS; Bruker, 2002) h = −14→16
Tmin = 0.149, Tmax = 0.409 k = −25→25
20653 measured reflections l = −22→21

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.040 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.103 H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0652P)2 + 4.556P] where P = (Fo2 + 2Fc2)/3
4847 reflections (Δ/σ)max = 0.001
262 parameters Δρmax = 2.07 e Å−3
0 restraints Δρmin = −2.88 e Å−3

Special details

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)

x y z Uiso*/Ueq
C1 0.3443 (5) 0.4519 (3) 0.2015 (4) 0.0487 (13)
C2 0.3684 (5) 0.3907 (2) 0.3391 (3) 0.0382 (11)
C3 0.1818 (5) 0.4511 (3) 0.2734 (3) 0.0489 (13)
C4 0.1120 (4) 0.2916 (3) 0.3248 (3) 0.0423 (12)
H4 0.0859 0.3334 0.3378 0.051*
C5 0.0700 (4) 0.2331 (3) 0.3493 (3) 0.0472 (13)
H5 0.0174 0.2355 0.3793 0.057*
C6 0.1068 (4) 0.1700 (3) 0.3287 (3) 0.0462 (12)
H6 0.0786 0.1298 0.3444 0.055*
C7 0.1858 (4) 0.1681 (3) 0.2847 (3) 0.0407 (11)
H7 0.2118 0.1269 0.2700 0.049*
C8 0.2249 (3) 0.2291 (3) 0.2634 (2) 0.0329 (10)
C9 0.3108 (4) 0.2358 (2) 0.2196 (2) 0.0301 (9)
C10 0.4329 (4) 0.2180 (2) 0.1553 (2) 0.0303 (9)
C11 0.5036 (4) 0.1774 (2) 0.1171 (2) 0.0312 (9)
C12 0.5080 (5) 0.1071 (3) 0.1248 (3) 0.0465 (13)
H12 0.4660 0.0851 0.1550 0.056*
C13 0.5751 (5) 0.0698 (3) 0.0873 (3) 0.0534 (14)
H13 0.5771 0.0226 0.0924 0.064*
C14 0.6396 (5) 0.1012 (3) 0.0422 (3) 0.0490 (14)
C15 0.6340 (4) 0.1714 (3) 0.0361 (3) 0.0436 (12)
H15 0.6765 0.1933 0.0062 0.052*
C16 0.5678 (4) 0.2104 (2) 0.0728 (3) 0.0356 (10)
H16 0.5662 0.2576 0.0679 0.043*
C17 0.7105 (7) 0.0591 (4) 0.0005 (4) 0.078 (2)
H17A 0.7491 0.0888 −0.0277 0.117*
H17B 0.6659 0.0285 −0.0348 0.117*
H17C 0.7614 0.0334 0.0375 0.117*
C18 0.1644 (7) 0.1149 (3) 0.0205 (5) 0.068 (2)
H18A 0.2392 0.1028 0.0209 0.082*
H18B 0.1226 0.1075 −0.0314 0.082*
N1 0.1910 (3) 0.2908 (2) 0.2820 (2) 0.0339 (8)
N2 0.3461 (3) 0.2940 (2) 0.2029 (2) 0.0327 (8)
N3 0.4270 (3) 0.2836 (2) 0.1605 (2) 0.0338 (8)
O1 0.3910 (5) 0.4950 (3) 0.1764 (3) 0.0831 (16)
O2 0.4232 (4) 0.3958 (2) 0.3981 (3) 0.0620 (12)
O3 0.1276 (5) 0.4934 (3) 0.2913 (3) 0.094 (2)
O4 0.3618 (3) 0.18424 (16) 0.19223 (18) 0.0326 (7)
Br1 0.12760 (5) 0.36874 (3) 0.11151 (3) 0.04326 (14)
Re1 0.268376 (15) 0.382313 (9) 0.241699 (11) 0.03283 (10)
Cl1 0.1140 (3) 0.06259 (12) 0.08553 (18) 0.1191 (10)
Cl2 0.15734 (14) 0.20035 (8) 0.04467 (9) 0.0578 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.058 (3) 0.034 (3) 0.056 (3) 0.000 (2) 0.015 (3) −0.004 (2)
C2 0.046 (3) 0.026 (2) 0.040 (3) 0.0082 (19) 0.005 (2) −0.0054 (18)
C3 0.049 (3) 0.046 (3) 0.051 (3) 0.009 (3) 0.009 (3) −0.013 (2)
C4 0.037 (3) 0.056 (3) 0.037 (3) 0.008 (2) 0.014 (2) −0.006 (2)
C5 0.046 (3) 0.058 (3) 0.041 (3) −0.001 (2) 0.017 (2) 0.004 (2)
C6 0.045 (3) 0.048 (3) 0.049 (3) −0.009 (2) 0.017 (2) 0.006 (2)
C7 0.046 (3) 0.036 (3) 0.043 (3) −0.001 (2) 0.014 (2) 0.004 (2)
C8 0.036 (3) 0.034 (3) 0.030 (2) 0.0017 (17) 0.008 (2) 0.0021 (16)
C9 0.037 (2) 0.025 (2) 0.029 (2) 0.0035 (17) 0.0067 (18) −0.0018 (16)
C10 0.036 (2) 0.030 (2) 0.026 (2) 0.0008 (18) 0.0081 (17) 0.0001 (15)
C11 0.041 (2) 0.029 (2) 0.025 (2) 0.0047 (18) 0.0100 (18) −0.0011 (15)
C12 0.066 (4) 0.029 (3) 0.052 (3) 0.005 (2) 0.029 (3) 0.004 (2)
C13 0.076 (4) 0.032 (3) 0.057 (3) 0.014 (3) 0.025 (3) −0.003 (2)
C14 0.059 (3) 0.053 (3) 0.040 (3) 0.017 (3) 0.023 (3) −0.007 (2)
C15 0.048 (3) 0.052 (3) 0.035 (3) 0.007 (2) 0.019 (2) 0.005 (2)
C16 0.045 (3) 0.031 (2) 0.033 (2) 0.005 (2) 0.013 (2) 0.0034 (18)
C17 0.099 (5) 0.083 (5) 0.061 (4) 0.044 (4) 0.038 (4) −0.010 (3)
C18 0.074 (5) 0.059 (4) 0.077 (5) 0.004 (3) 0.028 (4) −0.018 (3)
N1 0.035 (2) 0.036 (2) 0.032 (2) 0.0047 (17) 0.0108 (17) −0.0038 (16)
N2 0.034 (2) 0.031 (2) 0.035 (2) 0.0007 (16) 0.0111 (17) −0.0032 (15)
N3 0.040 (2) 0.031 (2) 0.033 (2) 0.0015 (16) 0.0155 (17) −0.0033 (15)
O1 0.093 (4) 0.054 (3) 0.105 (4) −0.023 (3) 0.028 (3) 0.019 (3)
O2 0.065 (3) 0.059 (3) 0.054 (3) 0.013 (2) −0.005 (2) −0.014 (2)
O3 0.112 (5) 0.079 (4) 0.093 (4) 0.055 (4) 0.025 (3) −0.022 (3)
O4 0.0407 (17) 0.0271 (16) 0.0328 (16) 0.0012 (13) 0.0144 (14) −0.0017 (12)
Br1 0.0496 (3) 0.0390 (3) 0.0394 (3) −0.0001 (2) 0.0049 (2) 0.00145 (19)
Re1 0.03905 (14) 0.02488 (12) 0.03580 (14) 0.00306 (6) 0.01052 (10) −0.00546 (6)
Cl1 0.176 (3) 0.0556 (13) 0.142 (2) 0.0091 (15) 0.072 (2) 0.0206 (13)
Cl2 0.0680 (9) 0.0531 (9) 0.0511 (8) 0.0077 (7) 0.0089 (7) 0.0014 (6)

Geometric parameters (Å, °)

Re1—C1 1.887 (6) C10—N3 1.293 (6)
Re1—C2 1.921 (5) C10—O4 1.380 (5)
Re1—C3 1.890 (5) C10—C11 1.459 (6)
Re1—N1 2.228 (4) C11—C12 1.385 (6)
Re1—N2 2.169 (4) C11—C16 1.395 (6)
Re1—Br1 2.6146 (11) C12—C13 1.384 (7)
C1—O1 1.168 (7) C12—H12 0.9300
C2—O2 1.131 (7) C13—C14 1.392 (9)
C3—O3 1.159 (7) C13—H13 0.9300
C4—N1 1.366 (6) C14—C15 1.383 (8)
C4—C5 1.369 (8) C14—C17 1.512 (7)
C4—H4 0.9300 C15—C16 1.386 (7)
C5—C6 1.397 (8) C15—H15 0.9300
C5—H5 0.9300 C16—H16 0.9300
C6—C7 1.381 (7) C17—H17A 0.9600
C6—H6 0.9300 C17—H17B 0.9600
C7—C8 1.374 (7) C17—H17C 0.9600
C7—H7 0.9300 C18—Cl2 1.737 (6)
C8—N1 1.346 (6) C18—Cl1 1.753 (8)
C8—C9 1.459 (7) C18—H18A 0.9700
C9—N2 1.283 (6) C18—H18B 0.9700
C9—O4 1.339 (5) N2—N3 1.396 (5)
O1—C1—Re1 179.8 (7) C15—C16—C11 118.5 (5)
O2—C2—Re1 176.8 (5) C15—C16—H16 120.7
O3—C3—Re1 178.6 (6) C11—C16—H16 120.7
N1—C4—C5 122.5 (5) C14—C17—H17A 109.5
N1—C4—H4 118.8 C14—C17—H17B 109.5
C5—C4—H4 118.8 H17A—C17—H17B 109.5
C4—C5—C6 119.4 (5) C14—C17—H17C 109.5
C4—C5—H5 120.3 H17A—C17—H17C 109.5
C6—C5—H5 120.3 H17B—C17—H17C 109.5
C7—C6—C5 119.0 (5) Cl2—C18—Cl1 111.1 (4)
C7—C6—H6 120.5 Cl2—C18—H18A 109.4
C5—C6—H6 120.5 Cl1—C18—H18A 109.4
C8—C7—C6 118.1 (5) Cl2—C18—H18B 109.4
C8—C7—H7 121.0 Cl1—C18—H18B 109.4
C6—C7—H7 121.0 H18A—C18—H18B 108.0
N1—C8—C7 124.5 (4) C8—N1—C4 116.6 (4)
N1—C8—C9 110.8 (4) C8—N1—Re1 117.8 (3)
C7—C8—C9 124.7 (4) C4—N1—Re1 125.6 (4)
N2—C9—O4 112.1 (4) C9—N2—N3 108.5 (4)
N2—C9—C8 122.1 (4) C9—N2—Re1 116.1 (3)
O4—C9—C8 125.9 (4) N3—N2—Re1 135.4 (3)
N3—C10—O4 113.1 (4) C10—N3—N2 104.1 (4)
N3—C10—C11 128.8 (4) C9—O4—C10 102.3 (3)
O4—C10—C11 118.2 (4) C1—Re1—C3 87.8 (3)
C12—C11—C16 120.1 (4) C1—Re1—C2 89.1 (3)
C12—C11—C10 121.0 (4) C3—Re1—C2 89.2 (2)
C16—C11—C10 118.9 (4) C1—Re1—N2 99.4 (2)
C13—C12—C11 119.7 (5) C3—Re1—N2 171.4 (2)
C13—C12—H12 120.1 C2—Re1—N2 95.53 (18)
C11—C12—H12 120.1 C1—Re1—N1 172.65 (19)
C12—C13—C14 121.6 (5) C3—Re1—N1 99.5 (2)
C12—C13—H13 119.2 C2—Re1—N1 91.87 (19)
C14—C13—H13 119.2 N2—Re1—N1 73.26 (16)
C15—C14—C13 117.3 (5) C1—Re1—Br1 92.72 (19)
C15—C14—C17 122.1 (6) C3—Re1—Br1 90.28 (18)
C13—C14—C17 120.6 (6) C2—Re1—Br1 178.05 (17)
C14—C15—C16 122.7 (5) N2—Re1—Br1 84.79 (11)
C14—C15—H15 118.6 N1—Re1—Br1 86.38 (10)
C16—C15—H15 118.6

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB5758).

References

  1. Bruker (2002). SMART, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Demko, Z.-P. & Sharpless, K.-B. (2001). J. Org. Chem. 66, 7945–7950. [DOI] [PubMed]
  3. Ley, K.-D., Whittle, C.-E., Bartberger, M.-D. & Schanze, K.-S. (1997). J. Am. Chem. Soc. 119, 3423–3424.
  4. Rajendran, T., Manimaran, B., Lee, F.-Y., Lee, G.-H., Peng, S.-M., Wang, C.-C. & Lu, K.-L. (2000). Inorg. Chem. 39, 2016–2017. [DOI] [PubMed]
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Tamoto, N., Adachi, C. & Ngai, K. (1997). Chem. Mater. 9, 1077–1085.
  7. Zhang, L.-M., Li, B. & Su, Z.-M. (2009). Langmuir, 25, 2068–2074. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053681004969X/hb5758sup1.cif

e-67-000m9-sup1.cif (18.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053681004969X/hb5758Isup2.hkl

e-67-000m9-Isup2.hkl (237.5KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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