Abstract
The crystal structure of the title compound, C18H26N2O3, is stabilized by intermolecular N—H⋯O and O—H⋯O hydrogen bonds. One of the methyl groups is disordered with occupancies of 0.51 (3):0.49 (3).
Related literature
For the properties of metallocrowns, see: Alexiou et al. (2002 ▶); Gaynor et al. (2002 ▶); Lah & Pecoraro (1989 ▶); Lehaire et al. (2002 ▶); Liu et al. (2001 ▶, 2008 ▶); Saalfrank et al. (2001 ▶).
Experimental
Crystal data
C18H26N2O3
M r = 318.41
Monoclinic,
a = 16.193 (5) Å
b = 16.194 (5) Å
c = 6.856 (2) Å
β = 97.892 (4)°
V = 1780.8 (9) Å3
Z = 4
Mo Kα radiation
μ = 0.08 mm−1
T = 296 K
0.43 × 0.26 × 0.22 mm
Data collection
Bruker APEXII CCD area-detector diffractometer
Absorption correction: none T min = 0.970, T max = 0.983
8728 measured reflections
6453 independent reflections
3925 reflections with I > 2σ(I)
R int = 0.025
Refinement
R[F 2 > 2σ(F 2)] = 0.080
wR(F 2) = 0.211
S = 1.05
6453 reflections
217 parameters
H-atom parameters constrained
Δρmax = 0.40 e Å−3
Δρmin = −0.60 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); 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: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S160053680900556X/jh2073sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053680900556X/jh2073Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1A⋯O2i | 0.86 | 2.05 | 2.821 (4) | 149 |
| O1—H1B⋯O3 | 0.82 | 1.92 | 2.636 (4) | 145 |
| N2—H2A⋯O3ii | 0.86 | 2.10 | 2.898 (4) | 154 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This project was sponsored by the K. C. Wong Magna Fund of Ningbo University and Ningbo Municipal Natural Science Foundation (2008 A610051)
supplementary crystallographic information
Comment
Metallacrowns are important compounds. Because of their potentially unique properties (Alexiou et al., 2002; Gaynor et al., 2002; Lah & Pecoraro, 1989; Lehaire et al., 2002; Liu et al., 2001; Saalfrank et al., 2001), they have gained increasing attention over the past decade. These compounds can be readily assembled using a trianionic pentadentate ligand,N-acylsalicylhydrazide,having a trivalent octahedral metal ion. The size of the metallacrown can be controlled by modifying the close-contact interaction between the N-acyl residues of the ligands (Liu et al., 2008). We now report structure of a designed pentadentate ligand, N-4-isoPropylcyclohexyl-3-methyl-salicylhydrazide.
A view of the title structure is illustrated in Fig.1. Because of C1 splited into C1 and C1', It made the Ueq of neighbor atoms lower or larger than usual Ueq. The molecular conformation is characterized by N—H···O hydrogen bonds and the crystal packing is stabilized by N—H···O and O—H···O hydrogen bonds(Fig.2).
Experimental
Trimethylaceto chloride (6.025 g, 50.0 mmol) was added to 50 ml chloroform solution of 4-isoPropylcyclohexyl acid with an external ice-water bath and triethylamine(5.200 g, 50.0 mmol). stirred for about 30 min slowly warmed to ambient temperature. To the above solution, 3-methyl-salicylhydrazide (7.636 g, 46.0 mmol)was added and stirred for 30 min. A white suspension began to appear after a while.the resulting white precipitate was filtered and rinsed with chloroform and diethyl ether. The title compound was recrystallized from methanol solution.
Refinement
All H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms (C—H = 0.93%A; N—H = 0.86 Å; O—H = 0.82 Å) and Uiso(H) values weren taken to be equal to 1.2 Ueq(C, N) and 1.5Ueq(O). The C1 atom is disordered. Due to C12 is bonded to C3, which is not disordered. It has a smaller Ueq than other atoms, and thus has less freedom of movement. The larger than normal range of thermal motion is mostly due to the difference between the disordered group and the other atoms which are not disordered. The splited atom was dealed in the .ins file. the C1 atom is splited into C1 and C1', each of which has a half share. Then refinement, anisotropic refinement to convergence use the least-squares method.
Figures
Fig. 1.
The structure of (I), showing 30% probability displacement ellipsoids and the atom-numbering scheme. [symmetry code: (i) –X, 0.5+Y, 0.5-Z].
Fig. 2.
Packing diagram of (I). hydrogen bonds are shown as dashed lines.
Crystal data
| C18H26N2O3 | F(000) = 688 |
| Mr = 318.41 | Dx = 1.188 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 5099 reflections |
| a = 16.193 (5) Å | θ = 2.5–26.2° |
| b = 16.194 (5) Å | µ = 0.08 mm−1 |
| c = 6.856 (2) Å | T = 296 K |
| β = 97.892 (4)° | Block, colourless |
| V = 1780.8 (9) Å3 | 0.43 × 0.26 × 0.22 mm |
| Z = 4 |
Data collection
| Bruker APEXII CCD area-detector diffractometer | 3925 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.025 |
| graphite | θmax = 32.5°, θmin = 1.8° |
| φ and ω scans | h = −16→24 |
| 8728 measured reflections | k = −17→24 |
| 6453 independent reflections | l = −7→10 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.080 | H-atom parameters constrained |
| wR(F2) = 0.211 | w = 1/[σ2(Fo2) + (0.0912P)2 + 2.6628P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max = 0.001 |
| 6453 reflections | Δρmax = 0.40 e Å−3 |
| 217 parameters | Δρmin = −0.60 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.016 (5) |
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 | Occ. (<1) | |
| O1 | 0.26649 (17) | 0.4109 (2) | 0.1034 (4) | 0.0739 (9) | |
| H1B | 0.2257 | 0.4290 | 0.1481 | 0.111* | |
| O2 | −0.02604 (18) | 0.29519 (17) | 0.2523 (4) | 0.0721 (9) | |
| O3 | 0.10747 (16) | 0.44725 (15) | 0.0967 (4) | 0.0527 (7) | |
| N1 | 0.01874 (18) | 0.36122 (18) | −0.0854 (5) | 0.0512 (9) | |
| H1A | 0.0117 | 0.3227 | −0.1724 | 0.061* | |
| N2 | −0.04755 (18) | 0.38761 (18) | 0.0058 (5) | 0.0513 (8) | |
| H2A | −0.0782 | 0.4274 | −0.0462 | 0.062* | |
| C1 | −0.458 (2) | 0.3768 (18) | 0.388 (6) | 0.056 (4) | 0.49 (3) |
| H1C | −0.4868 | 0.4194 | 0.3090 | 0.084* | 0.49 (3) |
| H1D | −0.4921 | 0.3564 | 0.4804 | 0.084* | 0.49 (3) |
| H1E | −0.4444 | 0.3325 | 0.3043 | 0.084* | 0.49 (3) |
| C1' | −0.454 (2) | 0.3490 (17) | 0.412 (6) | 0.056 (4) | 0.51 (3) |
| H1'A | −0.5058 | 0.3693 | 0.4471 | 0.084* | 0.51 (3) |
| H1'B | −0.4431 | 0.2950 | 0.4669 | 0.084* | 0.51 (3) |
| H1'C | −0.4580 | 0.3460 | 0.2709 | 0.084* | 0.51 (3) |
| C2 | 0.3959 (3) | 0.3661 (4) | −0.0978 (10) | 0.106 (2) | |
| H2B | 0.4317 | 0.3483 | −0.1904 | 0.159* | |
| H2C | 0.4051 | 0.3319 | 0.0176 | 0.159* | |
| H2D | 0.4082 | 0.4225 | −0.0618 | 0.159* | |
| C3 | −0.3787 (3) | 0.4114 (4) | 0.4969 (7) | 0.0834 (15) | |
| H3A | −0.3790 | 0.4699 | 0.4600 | 0.100* | |
| C4 | −0.2983 (3) | 0.3734 (3) | 0.2158 (6) | 0.0757 (14) | |
| H4A | −0.3073 | 0.4287 | 0.1626 | 0.091* | |
| H4B | −0.3448 | 0.3394 | 0.1591 | 0.091* | |
| C5 | −0.3791 (4) | 0.4114 (5) | 0.7111 (8) | 0.119 (2) | |
| H5A | −0.4301 | 0.4355 | 0.7407 | 0.179* | |
| H5B | −0.3326 | 0.4430 | 0.7733 | 0.179* | |
| H5C | −0.3748 | 0.3556 | 0.7591 | 0.179* | |
| C6 | −0.2185 (2) | 0.3391 (3) | 0.1563 (6) | 0.0697 (12) | |
| H6A | −0.2224 | 0.3394 | 0.0138 | 0.084* | |
| H6B | −0.2116 | 0.2824 | 0.2005 | 0.084* | |
| C7 | 0.2006 (3) | 0.3240 (3) | −0.4629 (6) | 0.0659 (12) | |
| H7A | 0.1872 | 0.3061 | −0.5923 | 0.079* | |
| C8 | 0.2827 (3) | 0.3312 (3) | −0.3797 (7) | 0.0722 (13) | |
| H8A | 0.3242 | 0.3168 | −0.4546 | 0.087* | |
| C9 | −0.2194 (3) | 0.4244 (3) | 0.5271 (6) | 0.0668 (12) | |
| H9A | −0.2261 | 0.4820 | 0.4885 | 0.080* | |
| H9B | −0.2155 | 0.4219 | 0.6694 | 0.080* | |
| C10 | 0.3056 (3) | 0.3589 (3) | −0.1909 (7) | 0.0667 (12) | |
| C11 | −0.1385 (2) | 0.3919 (3) | 0.4654 (6) | 0.0639 (11) | |
| H11A | −0.0927 | 0.4272 | 0.5202 | 0.077* | |
| H11B | −0.1278 | 0.3368 | 0.5182 | 0.077* | |
| C12 | −0.2964 (2) | 0.3765 (3) | 0.4368 (6) | 0.0594 (11) | |
| H12A | −0.2903 | 0.3197 | 0.4858 | 0.071* | |
| C13 | 0.1385 (3) | 0.3435 (2) | −0.3521 (5) | 0.0519 (10) | |
| H13A | 0.0829 | 0.3375 | −0.4057 | 0.062* | |
| C14 | −0.0656 (2) | 0.3531 (2) | 0.1735 (5) | 0.0489 (9) | |
| C15 | 0.2426 (2) | 0.3815 (2) | −0.0817 (6) | 0.0525 (10) | |
| C16 | −0.1424 (2) | 0.3893 (2) | 0.2434 (5) | 0.0491 (9) | |
| H16A | −0.1494 | 0.4459 | 0.1934 | 0.059* | |
| C17 | 0.1590 (2) | 0.3722 (2) | −0.1597 (5) | 0.0438 (9) | |
| C18 | 0.0941 (2) | 0.3959 (2) | −0.0379 (5) | 0.0432 (9) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0567 (17) | 0.097 (2) | 0.0653 (19) | −0.0119 (16) | 0.0002 (14) | −0.0117 (16) |
| O2 | 0.078 (2) | 0.0557 (17) | 0.084 (2) | 0.0235 (15) | 0.0142 (16) | 0.0192 (15) |
| O3 | 0.0640 (16) | 0.0435 (14) | 0.0507 (15) | −0.0001 (12) | 0.0089 (12) | −0.0073 (12) |
| N1 | 0.0474 (18) | 0.0430 (17) | 0.065 (2) | −0.0004 (14) | 0.0150 (15) | −0.0112 (14) |
| N2 | 0.0483 (18) | 0.0446 (17) | 0.063 (2) | 0.0103 (14) | 0.0156 (15) | 0.0052 (15) |
| C1 | 0.052 (4) | 0.062 (15) | 0.054 (8) | 0.001 (11) | 0.007 (5) | −0.002 (10) |
| C1' | 0.052 (4) | 0.062 (15) | 0.054 (8) | 0.001 (11) | 0.007 (5) | −0.002 (10) |
| C2 | 0.049 (3) | 0.133 (5) | 0.137 (5) | −0.003 (3) | 0.021 (3) | 0.000 (4) |
| C3 | 0.066 (3) | 0.111 (4) | 0.078 (3) | 0.003 (3) | 0.026 (2) | −0.003 (3) |
| C4 | 0.052 (2) | 0.114 (4) | 0.060 (3) | 0.003 (2) | 0.005 (2) | −0.012 (2) |
| C5 | 0.089 (4) | 0.182 (7) | 0.091 (4) | −0.019 (4) | 0.029 (3) | −0.020 (4) |
| C6 | 0.055 (2) | 0.094 (3) | 0.060 (2) | −0.002 (2) | 0.0059 (19) | −0.022 (2) |
| C7 | 0.091 (3) | 0.052 (2) | 0.060 (2) | −0.007 (2) | 0.028 (2) | −0.0087 (19) |
| C8 | 0.077 (3) | 0.061 (3) | 0.087 (3) | 0.001 (2) | 0.041 (3) | −0.007 (2) |
| C9 | 0.066 (3) | 0.080 (3) | 0.056 (2) | −0.004 (2) | 0.013 (2) | −0.015 (2) |
| C10 | 0.052 (2) | 0.064 (3) | 0.087 (3) | −0.0014 (19) | 0.021 (2) | 0.004 (2) |
| C11 | 0.055 (2) | 0.079 (3) | 0.057 (2) | −0.007 (2) | 0.0021 (19) | −0.006 (2) |
| C12 | 0.059 (2) | 0.062 (2) | 0.058 (2) | −0.0005 (19) | 0.0116 (19) | 0.0021 (19) |
| C13 | 0.062 (2) | 0.042 (2) | 0.052 (2) | −0.0038 (17) | 0.0107 (18) | −0.0033 (16) |
| C14 | 0.050 (2) | 0.039 (2) | 0.058 (2) | 0.0026 (17) | 0.0056 (17) | 0.0026 (17) |
| C15 | 0.051 (2) | 0.049 (2) | 0.058 (2) | −0.0037 (17) | 0.0101 (18) | 0.0030 (17) |
| C16 | 0.052 (2) | 0.043 (2) | 0.053 (2) | 0.0033 (16) | 0.0103 (17) | 0.0060 (16) |
| C17 | 0.049 (2) | 0.0339 (18) | 0.050 (2) | −0.0022 (15) | 0.0113 (16) | 0.0022 (15) |
| C18 | 0.052 (2) | 0.0313 (17) | 0.046 (2) | 0.0023 (15) | 0.0077 (16) | 0.0037 (16) |
Geometric parameters (Å, °)
| O1—C15 | 1.360 (5) | C4—H4B | 0.9700 |
| O1—H1B | 0.8200 | C5—H5A | 0.9600 |
| O2—C14 | 1.220 (4) | C5—H5B | 0.9600 |
| O3—C18 | 1.239 (4) | C5—H5C | 0.9600 |
| N1—C18 | 1.342 (5) | C6—C16 | 1.527 (6) |
| N1—N2 | 1.382 (4) | C6—H6A | 0.9700 |
| N1—H1A | 0.8600 | C6—H6B | 0.9700 |
| N2—C14 | 1.346 (5) | C7—C13 | 1.376 (6) |
| N2—H2A | 0.8600 | C7—C8 | 1.378 (7) |
| C1—C3 | 1.50 (4) | C7—H7A | 0.9300 |
| C1—H1C | 0.9600 | C8—C10 | 1.372 (6) |
| C1—H1D | 0.9600 | C8—H8A | 0.9300 |
| C1—H1E | 0.9600 | C9—C11 | 1.525 (6) |
| C1'—C3 | 1.63 (4) | C9—C12 | 1.526 (6) |
| C1'—H1'A | 0.9600 | C9—H9A | 0.9700 |
| C1'—H1'B | 0.9600 | C9—H9B | 0.9700 |
| C1'—H1'C | 0.9600 | C10—C15 | 1.394 (6) |
| C2—C10 | 1.518 (7) | C11—C16 | 1.515 (5) |
| C2—H2B | 0.9600 | C11—H11A | 0.9700 |
| C2—H2C | 0.9600 | C11—H11B | 0.9700 |
| C2—H2D | 0.9600 | C12—H12A | 0.9800 |
| C3—C5 | 1.469 (7) | C13—C17 | 1.395 (5) |
| C3—C12 | 1.554 (6) | C13—H13A | 0.9300 |
| C3—H3A | 0.9800 | C14—C16 | 1.511 (5) |
| C4—C12 | 1.512 (6) | C15—C17 | 1.395 (5) |
| C4—C6 | 1.514 (6) | C16—H16A | 0.9800 |
| C4—H4A | 0.9700 | C17—C18 | 1.479 (5) |
| C15—O1—H1B | 109.5 | H6A—C6—H6B | 107.9 |
| C18—N1—N2 | 119.8 (3) | C13—C7—C8 | 119.2 (4) |
| C18—N1—H1A | 120.1 | C13—C7—H7A | 120.4 |
| N2—N1—H1A | 120.1 | C8—C7—H7A | 120.4 |
| C14—N2—N1 | 122.1 (3) | C10—C8—C7 | 122.6 (4) |
| C14—N2—H2A | 118.9 | C10—C8—H8A | 118.7 |
| N1—N2—H2A | 118.9 | C7—C8—H8A | 118.7 |
| C3—C1—H1C | 109.5 | C11—C9—C12 | 113.4 (3) |
| C3—C1—H1D | 109.5 | C11—C9—H9A | 108.9 |
| C3—C1—H1E | 109.5 | C12—C9—H9A | 108.9 |
| C3—C1'—H1'A | 109.5 | C11—C9—H9B | 108.9 |
| C3—C1'—H1'B | 109.5 | C12—C9—H9B | 108.9 |
| H1'A—C1'—H1'B | 109.5 | H9A—C9—H9B | 107.7 |
| C3—C1'—H1'C | 109.5 | C8—C10—C15 | 118.0 (4) |
| H1'A—C1'—H1'C | 109.5 | C8—C10—C2 | 122.8 (4) |
| H1'B—C1'—H1'C | 109.5 | C15—C10—C2 | 119.2 (4) |
| C10—C2—H2B | 109.5 | C16—C11—C9 | 111.7 (3) |
| C10—C2—H2C | 109.5 | C16—C11—H11A | 109.3 |
| H2B—C2—H2C | 109.5 | C9—C11—H11A | 109.3 |
| C10—C2—H2D | 109.5 | C16—C11—H11B | 109.3 |
| H2B—C2—H2D | 109.5 | C9—C11—H11B | 109.3 |
| H2C—C2—H2D | 109.5 | H11A—C11—H11B | 107.9 |
| C5—C3—C1 | 112.2 (16) | C4—C12—C9 | 109.0 (4) |
| C5—C3—C12 | 112.8 (4) | C4—C12—C3 | 112.2 (4) |
| C1—C3—C12 | 115.8 (16) | C9—C12—C3 | 112.9 (4) |
| C5—C3—C1' | 104.6 (14) | C4—C12—H12A | 107.5 |
| C1—C3—C1' | 17.0 (13) | C9—C12—H12A | 107.5 |
| C12—C3—C1' | 107.9 (14) | C3—C12—H12A | 107.5 |
| C5—C3—H3A | 104.9 | C7—C13—C17 | 120.1 (4) |
| C1—C3—H3A | 104.9 | C7—C13—H13A | 119.9 |
| C12—C3—H3A | 104.9 | C17—C13—H13A | 119.9 |
| C1'—C3—H3A | 121.9 | O2—C14—N2 | 122.3 (3) |
| C12—C4—C6 | 112.4 (4) | O2—C14—C16 | 124.3 (3) |
| C12—C4—H4A | 109.1 | N2—C14—C16 | 113.3 (3) |
| C6—C4—H4A | 109.1 | O1—C15—C10 | 117.2 (4) |
| C12—C4—H4B | 109.1 | O1—C15—C17 | 122.1 (3) |
| C6—C4—H4B | 109.1 | C10—C15—C17 | 120.6 (4) |
| H4A—C4—H4B | 107.8 | C14—C16—C11 | 114.0 (3) |
| C3—C5—H5A | 109.5 | C14—C16—C6 | 108.9 (3) |
| C3—C5—H5B | 109.5 | C11—C16—C6 | 109.1 (3) |
| H5A—C5—H5B | 109.5 | C14—C16—H16A | 108.2 |
| C3—C5—H5C | 109.5 | C11—C16—H16A | 108.2 |
| H5A—C5—H5C | 109.5 | C6—C16—H16A | 108.2 |
| H5B—C5—H5C | 109.5 | C15—C17—C13 | 119.4 (3) |
| C4—C6—C16 | 111.9 (4) | C15—C17—C18 | 118.9 (3) |
| C4—C6—H6A | 109.2 | C13—C17—C18 | 121.7 (3) |
| C16—C6—H6A | 109.2 | O3—C18—N1 | 121.5 (3) |
| C4—C6—H6B | 109.2 | O3—C18—C17 | 122.0 (3) |
| C16—C6—H6B | 109.2 | N1—C18—C17 | 116.5 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···O2i | 0.86 | 2.05 | 2.821 (4) | 149 |
| O1—H1B···O3 | 0.82 | 1.92 | 2.636 (4) | 145 |
| N2—H2A···O3ii | 0.86 | 2.10 | 2.898 (4) | 154 |
Symmetry codes: (i) x, −y+1/2, z−1/2; (ii) −x, −y+1, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JH2073).
References
- Alexiou, M., Dendrinou-Samara, C., Raptopoulou, C. P., Terzis, A. & Kessissoglou, D. P. (2002). Inorg. Chem.41, 4732–4738. [DOI] [PubMed]
- Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
- Gaynor, D., Starikova, Z. A., Ostrovsky, S., Haase, W. & Nolan, K. B. (2002). Chem. Commun. pp. 506–507. [DOI] [PubMed]
- Lah, M. S. & Pecoraro, V. L. (1989). J. Am. Chem. Soc.111, 7258–7259.
- Lehaire, M. L., Scopelliti, R., Piotrowski, H. & Severin, K. (2002). Angew. Chem. Int. Ed.41, 1419–1421. [DOI] [PubMed]
- Liu, W., Lee, K., Park, M., John, R. P., Moon, D., Zou, Y., Liu, X., Ri, H.-C., Kim, G. H. & Lah, M. S. (2008). Inorg. Chem.47, 8807–8812. [DOI] [PubMed]
- Liu, S. X., Lin, S., Lin, B. Z., Lin, C. C. & Huang, J. Q. (2001). Angew. Chem. Int. Ed.40, 1084–1087.
- Saalfrank, R. W., Bernt, I., Chowdhry, M. M., Hampel, F. & Vaughan, G. B. M. (2001). Chem. Eur. J.7, 2765–2768. [DOI] [PubMed]
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [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/S160053680900556X/jh2073sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S160053680900556X/jh2073Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


