Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270108029314/gd3240sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S0108270108029314/gd3240Isup2.hkl |
CCDC reference: 707196
A mixture of CuCl2.2H2O (0.085 g, 0.5 mmol), H3L1 (0.070 g, 0.33 mmol) and QA (0.065 g, 0.5 mmol) was dissolved in 10 ml distilled water; this was followed by the addition of triethylamine until the pH was in the range 5.5–6.3. The resulting solution was stirred for about 1 h at room temperature, sealed in a 23 ml Teflon-lined stainless steel autoclave and heated at 453 K for 5 d under autogenous pressure. Afterwards, the reaction system was slowly cooled to room temperature. Dark-red block crystals of (I) suitable for single-crystal X-ray diffraction analysis were collected from the final reaction system by filtration, washed several times with distilled water and dried in air at ambient temperature (yield: 29% based on Cu).
The carbon-bound H atoms were generated geometrically (C—H = 0.93 Å) and refined as riding, with Uiso(H) = 1.2Ueq(C). No H atoms could be found in the vicinity of the carboxyl or hydroxyl O atoms, consistent with the relevant C—O distances. The small voids within the structure were found to contain no significant electron density.
Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT (Bruker, 1999); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL-Plus (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).
[Cu2(C8H3O5)(C8H6N2)] | F(000) = 868 |
Mr = 436.33 | Dx = 1.974 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 3402 reflections |
a = 5.2011 (2) Å | θ = 1.1–28.3° |
b = 23.5553 (11) Å | µ = 2.93 mm−1 |
c = 12.2402 (6) Å | T = 293 K |
β = 101.719 (1)° | Block, dark red |
V = 1468.33 (11) Å3 | 0.31 × 0.27 × 0.19 mm |
Z = 4 |
Bruker APEX CCD area-detector diffractometer | 3402 independent reflections |
Radiation source: fine-focus sealed tube | 2852 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.029 |
ω scans | θmax = 28.3°, θmin = 1.7° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −6→6 |
Tmin = 0.391, Tmax = 0.575 | k = −31→30 |
8982 measured reflections | l = −16→13 |
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)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.071 | H-atom parameters constrained |
S = 0.96 | w = 1/[σ2(Fo2) + (0.0427P)2] where P = (Fo2 + 2Fc2)/3 |
3402 reflections | (Δ/σ)max = 0.001 |
226 parameters | Δρmax = 0.48 e Å−3 |
0 restraints | Δρmin = −0.29 e Å−3 |
[Cu2(C8H3O5)(C8H6N2)] | V = 1468.33 (11) Å3 |
Mr = 436.33 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 5.2011 (2) Å | µ = 2.93 mm−1 |
b = 23.5553 (11) Å | T = 293 K |
c = 12.2402 (6) Å | 0.31 × 0.27 × 0.19 mm |
β = 101.719 (1)° |
Bruker APEX CCD area-detector diffractometer | 3402 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | 2852 reflections with I > 2σ(I) |
Tmin = 0.391, Tmax = 0.575 | Rint = 0.029 |
8982 measured reflections |
R[F2 > 2σ(F2)] = 0.028 | 0 restraints |
wR(F2) = 0.071 | H-atom parameters constrained |
S = 0.96 | Δρmax = 0.48 e Å−3 |
3402 reflections | Δρmin = −0.29 e Å−3 |
226 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
C1 | 0.3875 (4) | 0.07382 (8) | 0.87479 (16) | 0.0236 (4) | |
C2 | 0.3891 (4) | 0.01664 (8) | 0.81996 (17) | 0.0246 (4) | |
C3 | 0.5985 (4) | −0.02297 (8) | 0.84865 (16) | 0.0239 (4) | |
C4 | 0.5854 (4) | −0.07520 (8) | 0.78954 (17) | 0.0258 (4) | |
C5 | 0.3694 (4) | −0.08508 (9) | 0.70422 (19) | 0.0340 (5) | |
H5 | 0.3614 | −0.1189 | 0.6645 | 0.041* | |
C7 | 0.1646 (5) | −0.04639 (9) | 0.6757 (2) | 0.0372 (5) | |
H7 | 0.0230 | −0.0542 | 0.6179 | 0.045* | |
C8 | 0.1755 (4) | 0.00368 (9) | 0.73481 (19) | 0.0306 (5) | |
H8 | 0.0374 | 0.0294 | 0.7175 | 0.037* | |
C9 | 0.5675 (5) | 0.20908 (9) | 1.08446 (18) | 0.0328 (5) | |
H9 | 0.6585 | 0.1786 | 1.0625 | 0.039* | |
C10 | 0.6686 (4) | 0.23533 (9) | 1.18769 (18) | 0.0320 (5) | |
H10 | 0.8240 | 0.2216 | 1.2309 | 0.038* | |
C11 | 0.3229 (4) | 0.29778 (9) | 1.15748 (17) | 0.0275 (4) | |
C12 | 0.1873 (5) | 0.34460 (9) | 1.19042 (19) | 0.0358 (5) | |
H12 | 0.2490 | 0.3619 | 1.2590 | 0.043* | |
C13 | −0.0349 (5) | 0.36457 (10) | 1.1214 (2) | 0.0412 (6) | |
H13 | −0.1223 | 0.3957 | 1.1433 | 0.049* | |
C14 | −0.1323 (5) | 0.33878 (10) | 1.01838 (19) | 0.0383 (5) | |
H14 | −0.2829 | 0.3530 | 0.9723 | 0.046* | |
C15 | −0.0086 (5) | 0.29320 (9) | 0.98517 (18) | 0.0329 (5) | |
H15 | −0.0764 | 0.2760 | 0.9170 | 0.039* | |
C16 | 0.2213 (4) | 0.27178 (8) | 1.05309 (17) | 0.0271 (4) | |
C6 | 0.7921 (4) | −0.12175 (8) | 0.81325 (18) | 0.0283 (4) | |
N1 | 0.3490 (4) | 0.22601 (7) | 1.01771 (14) | 0.0287 (4) | |
N2 | 0.5513 (4) | 0.27873 (7) | 1.22558 (14) | 0.0292 (4) | |
O1 | 0.1729 (3) | 0.10073 (6) | 0.85540 (13) | 0.0331 (4) | |
O2 | 0.5921 (3) | 0.09585 (6) | 0.93331 (13) | 0.0307 (3) | |
O3 | 0.8022 (3) | −0.01133 (6) | 0.93043 (12) | 0.0282 (3) | |
O4 | 0.7721 (3) | −0.16162 (6) | 0.74691 (13) | 0.0392 (4) | |
O5 | 0.9752 (3) | −0.12024 (6) | 0.90078 (13) | 0.0344 (4) | |
Cu1 | 0.90826 (5) | 0.059211 (10) | 1.00466 (2) | 0.02654 (9) | |
Cu2 | 0.20383 (5) | 0.187416 (11) | 0.87622 (2) | 0.03198 (9) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0264 (10) | 0.0225 (9) | 0.0219 (10) | 0.0013 (8) | 0.0046 (8) | 0.0030 (8) |
C2 | 0.0271 (10) | 0.0211 (9) | 0.0256 (10) | 0.0007 (8) | 0.0053 (8) | 0.0007 (8) |
C3 | 0.0256 (10) | 0.0233 (10) | 0.0224 (10) | −0.0019 (8) | 0.0037 (8) | 0.0011 (8) |
C4 | 0.0273 (11) | 0.0240 (10) | 0.0260 (10) | −0.0008 (8) | 0.0050 (8) | −0.0025 (8) |
C5 | 0.0360 (13) | 0.0284 (11) | 0.0345 (12) | −0.0011 (9) | −0.0005 (10) | −0.0084 (9) |
C7 | 0.0319 (12) | 0.0364 (12) | 0.0376 (13) | 0.0014 (10) | −0.0064 (10) | −0.0088 (10) |
C8 | 0.0281 (11) | 0.0286 (11) | 0.0329 (12) | 0.0023 (9) | 0.0011 (9) | −0.0003 (9) |
C9 | 0.0385 (13) | 0.0255 (11) | 0.0322 (12) | 0.0050 (9) | 0.0020 (10) | −0.0030 (9) |
C10 | 0.0331 (12) | 0.0280 (11) | 0.0302 (11) | 0.0030 (9) | −0.0051 (9) | 0.0016 (8) |
C11 | 0.0327 (12) | 0.0252 (10) | 0.0237 (10) | −0.0006 (8) | 0.0031 (9) | 0.0000 (8) |
C12 | 0.0406 (13) | 0.0343 (12) | 0.0304 (12) | 0.0039 (10) | 0.0021 (10) | −0.0094 (9) |
C13 | 0.0449 (15) | 0.0358 (13) | 0.0419 (14) | 0.0120 (11) | 0.0061 (11) | −0.0070 (10) |
C14 | 0.0365 (13) | 0.0411 (13) | 0.0340 (13) | 0.0119 (10) | −0.0009 (10) | 0.0032 (10) |
C15 | 0.0377 (12) | 0.0319 (12) | 0.0258 (11) | 0.0024 (10) | −0.0010 (9) | −0.0005 (9) |
C16 | 0.0331 (12) | 0.0234 (10) | 0.0241 (10) | 0.0010 (8) | 0.0038 (9) | 0.0007 (8) |
C6 | 0.0302 (11) | 0.0228 (10) | 0.0311 (11) | −0.0009 (8) | 0.0044 (9) | −0.0015 (8) |
N1 | 0.0362 (10) | 0.0230 (9) | 0.0243 (9) | 0.0014 (7) | 0.0001 (8) | −0.0020 (7) |
N2 | 0.0352 (10) | 0.0249 (9) | 0.0247 (9) | −0.0026 (8) | −0.0008 (8) | −0.0010 (7) |
O1 | 0.0305 (8) | 0.0248 (8) | 0.0404 (9) | 0.0066 (6) | −0.0015 (7) | −0.0036 (6) |
O2 | 0.0285 (8) | 0.0225 (7) | 0.0373 (9) | 0.0036 (6) | −0.0027 (7) | −0.0049 (6) |
O3 | 0.0301 (8) | 0.0211 (7) | 0.0292 (8) | 0.0041 (6) | −0.0040 (6) | −0.0055 (6) |
O4 | 0.0450 (10) | 0.0301 (8) | 0.0377 (9) | 0.0054 (7) | −0.0028 (7) | −0.0141 (7) |
O5 | 0.0363 (9) | 0.0240 (7) | 0.0375 (9) | 0.0049 (6) | −0.0054 (7) | −0.0086 (6) |
Cu1 | 0.02696 (15) | 0.02070 (14) | 0.02882 (15) | 0.00291 (10) | −0.00173 (11) | −0.00478 (10) |
Cu2 | 0.03764 (17) | 0.02884 (16) | 0.02625 (16) | 0.00393 (11) | −0.00110 (12) | −0.00446 (10) |
C1—O1 | 1.264 (2) | C11—C16 | 1.419 (3) |
C1—O2 | 1.267 (2) | C12—C13 | 1.369 (3) |
C1—C2 | 1.506 (3) | C12—H12 | 0.9300 |
C2—C8 | 1.394 (3) | C13—C14 | 1.399 (3) |
C2—C3 | 1.423 (3) | C13—H13 | 0.9300 |
C3—O3 | 1.330 (2) | C14—C15 | 1.356 (3) |
C3—C4 | 1.422 (3) | C14—H14 | 0.9300 |
C4—C5 | 1.389 (3) | C15—C16 | 1.404 (3) |
C4—C6 | 1.522 (3) | C15—H15 | 0.9300 |
C5—C7 | 1.392 (3) | C16—N1 | 1.381 (3) |
C5—H5 | 0.9300 | C6—O4 | 1.232 (2) |
C7—C8 | 1.379 (3) | C6—O5 | 1.281 (3) |
C7—H7 | 0.9300 | Cu1—O1i | 2.6852 (16) |
C8—H8 | 0.9300 | Cu1—O2 | 1.9047 (14) |
C9—N1 | 1.320 (3) | Cu1—O3ii | 1.9198 (14) |
C9—C10 | 1.409 (3) | Cu1—O3 | 1.9201 (13) |
C9—H9 | 0.9300 | Cu1—O5ii | 1.8678 (14) |
C10—N2 | 1.322 (3) | Cu2—N2iii | 2.0176 (17) |
C10—H10 | 0.9300 | Cu2—N1 | 1.9659 (17) |
C11—N2 | 1.380 (3) | Cu2—O1 | 2.0599 (14) |
C11—C12 | 1.411 (3) | ||
O1—C1—O2 | 120.62 (18) | C14—C13—H13 | 119.6 |
O1—C1—C2 | 116.71 (18) | C15—C14—C13 | 120.5 (2) |
O2—C1—C2 | 122.59 (18) | C15—C14—H14 | 119.7 |
C8—C2—C3 | 119.64 (18) | C13—C14—H14 | 119.7 |
C8—C2—C1 | 116.99 (18) | C14—C15—C16 | 120.4 (2) |
C3—C2—C1 | 123.34 (18) | C14—C15—H15 | 119.8 |
O3—C3—C4 | 120.66 (18) | C16—C15—H15 | 119.8 |
O3—C3—C2 | 120.22 (17) | N1—C16—C15 | 120.04 (19) |
C4—C3—C2 | 119.12 (18) | N1—C16—C11 | 120.29 (19) |
C5—C4—C3 | 118.38 (19) | C15—C16—C11 | 119.66 (19) |
C5—C4—C6 | 117.06 (18) | O4—C6—O5 | 121.41 (19) |
C3—C4—C6 | 124.56 (19) | O4—C6—C4 | 117.5 (2) |
C4—C5—C7 | 122.7 (2) | O5—C6—C4 | 121.07 (18) |
C4—C5—H5 | 118.7 | C9—N1—C16 | 116.76 (18) |
C7—C5—H5 | 118.7 | C9—N1—Cu2 | 122.28 (14) |
C8—C7—C5 | 118.7 (2) | C16—N1—Cu2 | 120.94 (15) |
C8—C7—H7 | 120.6 | C10—N2—C11 | 116.20 (18) |
C5—C7—H7 | 120.6 | C10—N2—Cu2iv | 120.17 (15) |
C7—C8—C2 | 121.4 (2) | C11—N2—Cu2iv | 123.63 (14) |
C7—C8—H8 | 119.3 | C1—O1—Cu2 | 115.47 (13) |
C2—C8—H8 | 119.3 | C1—O2—Cu1 | 128.42 (13) |
N1—C9—C10 | 122.7 (2) | C3—O3—Cu1ii | 128.93 (12) |
N1—C9—H9 | 118.6 | C3—O3—Cu1 | 130.02 (12) |
C10—C9—H9 | 118.6 | Cu1ii—O3—Cu1 | 100.76 (6) |
N2—C10—C9 | 122.6 (2) | C6—O5—Cu1ii | 129.19 (13) |
N2—C10—H10 | 118.7 | O5ii—Cu1—O2 | 94.39 (6) |
C9—C10—H10 | 118.7 | O5ii—Cu1—O3ii | 93.86 (6) |
N2—C11—C12 | 120.01 (19) | O2—Cu1—O3ii | 170.96 (6) |
N2—C11—C16 | 121.40 (19) | O5ii—Cu1—O3 | 170.10 (7) |
C12—C11—C16 | 118.6 (2) | O2—Cu1—O3 | 92.11 (6) |
C13—C12—C11 | 120.0 (2) | O3ii—Cu1—O3 | 79.24 (6) |
C13—C12—H12 | 120.0 | N1—Cu2—N2iii | 129.17 (7) |
C11—C12—H12 | 120.0 | N1—Cu2—O1 | 125.01 (7) |
C12—C13—C14 | 120.8 (2) | N2iii—Cu2—O1 | 105.81 (7) |
C12—C13—H13 | 119.6 |
Symmetry codes: (i) x+1, y, z; (ii) −x+2, −y, −z+2; (iii) x−1/2, −y+1/2, z−1/2; (iv) x+1/2, −y+1/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [Cu2(C8H3O5)(C8H6N2)] |
Mr | 436.33 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 293 |
a, b, c (Å) | 5.2011 (2), 23.5553 (11), 12.2402 (6) |
β (°) | 101.719 (1) |
V (Å3) | 1468.33 (11) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 2.93 |
Crystal size (mm) | 0.31 × 0.27 × 0.19 |
Data collection | |
Diffractometer | Bruker APEX CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 1996) |
Tmin, Tmax | 0.391, 0.575 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8982, 3402, 2852 |
Rint | 0.029 |
(sin θ/λ)max (Å−1) | 0.667 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.028, 0.071, 0.96 |
No. of reflections | 3402 |
No. of parameters | 226 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.48, −0.29 |
Computer programs: SMART (Bruker, 1997), SAINT (Bruker, 1999), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL-Plus (Sheldrick, 2008).
Extended frameworks of coordination polymers, based on complexes of transition metals and multifunctional bridging ligands, are of great research interest (Eddaoudi et al., 2001; Hagrman et al., 1999; Noveron et al., 2002; Batten & Robson, 1998). The hydro(solvo)thermal method is a useful technique for the construction of highly stable robust metal–organic frameworks (Chen & Liu, 2002; Yang et al., 2007; Tong et al., 2000). It has been found that in situ reactions, such as ligand oxidative coupling, hydrolysis, substitution and the redox process of copper, can occur under hydro(solvo)thermal conditions (Maji et al., 2004). These reactions represent promising new routes for constructing novel coordination polymers.
The chemistry of mixed-valence CuI,II complexes is of great importance. We are interested in developing mixed-valence CuI,II complexes under hydrothermal conditions because of their superior electronic, optical and magnetic properties (Maji et al., 2004). In consideration of the fact that several CuI,II complexes contain N-heterocycle and carboxylate ligands, we postu that benzene-1,2,3-tricarboxylic acid (H3L1) and quinoxaline (QA) are possibly good ligands for the construction of mixed-valence CuI,II complexes (Zhang & Fang, 2005). In this work, the hydrothermal reaction of H3L1, QA and divalent copper(II) salts resulted in a new mixed-valence CuI,II coordination polymer, the title compound, [CuICuII(L)(QA)]n, (I), where L1 was transformed into 2-hydroxyisophthalate (L).
Compound (I) was obtained under hydrothermal conditions at 453 K. Once formed, the compound is insoluble in most solvents, including water. As shown in Fig. 1, the asymmetric unit of (I) contains two crystallographically unique Cu atoms, one unique QA and one unique L. Atom Cu1 is primarily coordinated to four O atoms [O2, O3, O3i and O5i; symmetry code: (i) 2 - x, -y, 2 - z] in a distorted square geometry, of which two belong to two phenoxo groups and the other two to carboxylate groups of two L ligands. In addition, atom Cu1 interacts weakly with atom O1iii [2.6852 (16) Å; symmetry code: (iii) 1 + x, y, z], which belongs to an L ligand in an adjacent layer. Therefore, Cu1 has square-pyramidal coordination geometry. Atom Cu2 is trigonally coordinated by two N atoms [N1 and N2ii; symmetry code: (ii) -1/2 + x, 1/2 - y, -1/2 + z] from two QA molecules and one O atom (O1) from an L carboxylate group.
CuII ions with d9 configurations tend to have a square-pyramidal or axially elongated octahedral coordination geometry, while CuI ions with d10 configurations often adopt a trigonal or tetrahedral coordination geometry (Zhang & Fang, 2005). The coordination geometry of the copper centres, in combination with the charge balance, indicates that in compound (I) atom Cu1 is di-positive and atom Cu2 is uni-positive. The CuI ions are bridged by QA ligands to give a chain along the c axis. Two CuII ions and two L ligands form a [Cu2(L)2]2- `metallo-ligand', which coordinates two CuI ions. Thus, the chains of CuI and QA units are linked by the [Cu2(L)2]2- metallo-ligand to yield a (6,3) sheet in the (101) plane (Fig. 2). These sheets are further linked by the Cu1—O1 interaction into a three-dimensional framework.
It is worth noting that a new in situ reaction occurs in the CuCl2.2H2O/H3L1/QA system under hydrothermal conditions. The ligand L1 was transformed into L via decarboxylation and hydroxylation steps. The in situ reaction from L1 to L in the present system has rarely been observed before, although a similar reaction process whereby mixed-valence CuI,II species and in situ synthesis of L are simultaneously generated under the hydrothermal reaction of isophthalate and 4,4'-bipyridine with Cu(NO3).3H2O has been reported (Tao et al., 2002). So far, a few novel in situ reactions such as ligand oxidative coupling, hydrolysis and substitution have been observed during the hydrothermal process (Tao et al., 2002), in which many factors, including the nature of the metal ion and the temperature, pressure and pH, have been found to influence the reaction outcome significantly. As far as the present system is concerned, the pH value may play a key role in the transformation of L1.