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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Aug 6;64(Pt 9):m1105. doi: 10.1107/S1600536808024008

Poly[aqua­[μ2-1,1′-(butane-1,4-di­yl)diimidazole](μ2-naphthalene-1,4-dicarboxyl­ato)nickel(II)]

Xian-Zhi Zou a,*
PMCID: PMC2960619  PMID: 21201571

Abstract

In the title compound, [Ni(C12H6O4)(C10H14N4)(H2O)]n, the coordination polyhedron around each NiII atom is a distorted cis-NiN2O4 octa­hedron. The naphthalene-1,4-dicarboxyl­ate and 1,1′-(butane-1,4-di­yl)diimidazole ligands bridge the Ni centres to form a two-dimensional (4,4)-network, and O—H⋯O hydrogen bonds complete the structure.

Related literature

For general background, see: Batten & Robson (1998). For a related structure, see: Ma et al., (2003).graphic file with name e-64-m1105-scheme1.jpg

Experimental

Crystal data

  • [Ni(C12H6O4)(C10H14N4)(H2O)]

  • M r = 481.15

  • Monoclinic, Inline graphic

  • a = 12.4213 (12) Å

  • b = 13.2543 (13) Å

  • c = 13.4328 (13) Å

  • β = 107.361 (2)°

  • V = 2110.8 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.96 mm−1

  • T = 293 (2) K

  • 0.19 × 0.17 × 0.15 mm

Data collection

  • Bruker APEX CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1998) T min = 0.827, T max = 0.866

  • 11720 measured reflections

  • 4157 independent reflections

  • 2982 reflections with I > 2σ(I)

  • R int = 0.063

Refinement

  • R[F 2 > 2σ(F 2)] = 0.049

  • wR(F 2) = 0.097

  • S = 1.05

  • 4157 reflections

  • 297 parameters

  • 3 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.54 e Å−3

  • Δρmin = −0.40 e Å−3

Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); 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/S1600536808024008/hb2770sup1.cif

e-64-m1105-sup1.cif (20.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808024008/hb2770Isup2.hkl

e-64-m1105-Isup2.hkl (199.6KB, hkl)

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

Table 1. Selected bond lengths (Å).

Ni1—O1W 2.125 (2)
Ni1—O2 2.040 (2)
Ni1—O1i 2.116 (2)
Ni1—O3i 2.347 (2)
Ni1—N1 2.060 (3)
Ni1—N4ii 2.099 (3)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—HW12⋯O1iii 0.819 (16) 1.847 (18) 2.661 (3) 172 (3)
O1W—HW11⋯O4 0.83 (4) 1.83 (4) 2.651 (3) 169 (3)

Symmetry code: (iii) Inline graphic.

Acknowledgments

The author thanks Beihua University for supporting this work.

supplementary crystallographic information

Comment

Metal-organic frameworks are currently of great interest because of their interesting structures and potential applications. So far, some interesting interpenetrated or entangled metal-organic networks with bis(imidazole)-containing ligands have been documented (Batten & Robson, 1998). Flexible ligands such as 1,1'-(1,4-butanediyl)bis(imidazole) (L) have been less explored to date (Ma et al., 2003). In this work, we selected 1,4-naphthalenedicarboxylic acid (H2ndc) and L as linkers, generating a new coordination polymer, [Ni(ndc)(L)(H2O)], (I), which is reported here.

In compound (I) each NiII atom is six-coordinated by two N atoms from two different L ligands, and four O atoms from three carboxylate oxygen atoms (one bidentate, one monodentate) and one water molecule in a distorted cis-NiN2O4 octohedral coordination sphere (Fig. 1). The two neighbouring NiII atoms are bridged by the ndc and L ligands to form a two-dimensional (4,4) network (Fig. 2) and O—H···O hydrogen bonds arising from the water molecule (Table 2) complete the structure.

Experimental

A mixture of H2ndc (0.5 mmol), L (0.5 mmol), NaOH (1 mmol) and NiCl2.6H2O (0.5 mmol) was suspended in 12 ml of deionized water and sealed in a 20-ml Teflon-lined autoclave. Upon heating at 433 K for one week, the autoclave was slowly cooled to room temperature. Green blocks of (I) were collected, washed with deionized water and dried.

Refinement

The H atoms on C atoms were generated geometrically and refined as riding with C—H = 0.93Å and Uiso(H) = 1.2Ueq(C). The water H atoms were located in a difference Fourier map and refined with the O—H distance restrained to 0.85±0.01 Å.

Figures

Fig. 1.

Fig. 1.

The structure of (I), with displacement ellipsoids for the non-hydrogen atoms drawn at the 30% probability level. Symmetry codes: (i) x, y - 1, z; (ii) 1/2 + x, 0.5 - y, z - 1/2.

Fig. 2.

Fig. 2.

View of part of the polymeric layer structure of (I).

Crystal data

[Ni(C12H6O4)(C10H14N4)(H2O)] F000 = 1000
Mr = 481.15 Dx = 1.514 Mg m3
Monoclinic, P21/n Mo Kα radiation λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 4157 reflections
a = 12.4213 (12) Å θ = 1.9–26.1º
b = 13.2543 (13) Å µ = 0.96 mm1
c = 13.4328 (13) Å T = 293 (2) K
β = 107.361 (2)º Block, green
V = 2110.8 (4) Å3 0.19 × 0.17 × 0.15 mm
Z = 4

Data collection

Bruker APEX CCD diffractometer 4157 independent reflections
Radiation source: fine-focus sealed tube 2982 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.063
T = 293(2) K θmax = 26.1º
ω scans θmin = 2.0º
Absorption correction: multi-scan(SADABS; Bruker, 1998) h = −9→15
Tmin = 0.827, Tmax = 0.866 k = −16→14
11720 measured reflections l = −16→16

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)] = 0.049 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.097   w = 1/[σ2(Fo2) + (0.0253P)2] where P = (Fo2 + 2Fc2)/3
S = 1.05 (Δ/σ)max < 0.001
4157 reflections Δρmax = 0.54 e Å3
297 parameters Δρmin = −0.40 e Å3
3 restraints Extinction correction: none
Primary atom site location: structure-invariant direct methods

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 0.2969 (3) 0.1196 (2) 0.2222 (3) 0.0208 (8)
C2 0.2145 (3) 0.1584 (2) 0.2758 (2) 0.0190 (8)
C3 0.2114 (3) 0.2586 (2) 0.2946 (3) 0.0264 (9)
H3 0.2583 0.3019 0.2721 0.032*
C4 0.1392 (3) 0.2986 (2) 0.3472 (3) 0.0238 (8)
H4 0.1399 0.3677 0.3597 0.029*
C5 0.0674 (3) 0.2376 (2) 0.3805 (2) 0.0203 (8)
C6 −0.0034 (3) 0.2829 (2) 0.4420 (3) 0.0218 (8)
C7 0.0636 (3) 0.1328 (2) 0.3576 (2) 0.0180 (7)
C8 0.1382 (3) 0.0919 (2) 0.3055 (2) 0.0172 (7)
C9 0.1306 (3) −0.0118 (2) 0.2806 (3) 0.0256 (8)
H9 0.1795 −0.0393 0.2473 0.031*
C10 0.0536 (3) −0.0723 (3) 0.3042 (3) 0.0281 (9)
H10 0.0497 −0.1404 0.2868 0.034*
C11 −0.0196 (3) −0.0320 (3) 0.3546 (3) 0.0312 (9)
H11 −0.0722 −0.0738 0.3706 0.037*
C12 −0.0157 (3) 0.0664 (2) 0.3806 (3) 0.0257 (8)
H12 −0.0657 0.0914 0.4141 0.031*
C13 0.1710 (3) 0.2460 (3) −0.1581 (3) 0.0335 (10)
H13 0.1644 0.1937 −0.2056 0.040*
C14 0.1151 (4) 0.3340 (3) −0.1787 (3) 0.0430 (11)
H14 0.0644 0.3537 −0.2418 0.052*
C15 0.2219 (3) 0.3312 (3) −0.0198 (3) 0.0310 (9)
H15 0.2581 0.3510 0.0484 0.037*
C16 0.1118 (3) 0.4914 (2) −0.0714 (3) 0.0274 (9)
H16A 0.1268 0.5024 0.0029 0.033*
H16B 0.0311 0.4976 −0.1039 0.033*
C17 0.1715 (3) 0.5711 (2) −0.1149 (3) 0.0296 (9)
H17A 0.1498 0.5648 −0.1903 0.036*
H17B 0.2523 0.5605 −0.0882 0.036*
C18 0.1434 (3) 0.6771 (2) −0.0863 (3) 0.0293 (9)
H18A 0.0622 0.6862 −0.1083 0.035*
H18B 0.1705 0.6855 −0.0112 0.035*
C19 0.1971 (3) 0.7560 (2) −0.1379 (3) 0.0293 (9)
H19A 0.2754 0.7381 −0.1277 0.035*
H19B 0.1590 0.7559 −0.2123 0.035*
C20 0.1050 (3) 0.9021 (3) −0.0704 (3) 0.0395 (11)
H20 0.0353 0.8734 −0.0749 0.047*
C21 0.2746 (3) 0.9270 (2) −0.0777 (3) 0.0238 (8)
H21 0.3436 0.9163 −0.0898 0.029*
N4 0.2477 (2) 1.01080 (19) −0.0399 (2) 0.0212 (7)
C23 0.1402 (3) 0.9948 (3) −0.0365 (3) 0.0378 (10)
H23 0.0973 1.0419 −0.0137 0.045*
N1 0.2384 (2) 0.2446 (2) −0.0581 (2) 0.0224 (7)
N2 0.1476 (2) 0.38862 (19) −0.0887 (2) 0.0232 (7)
N3 0.1920 (2) 0.8579 (2) −0.0970 (2) 0.0240 (7)
O1 −0.05860 (18) 0.36339 (16) 0.40707 (17) 0.0227 (5)
O2 0.3062 (2) 0.17401 (16) 0.14730 (18) 0.0266 (6)
O1W 0.4733 (2) 0.04150 (17) 0.12115 (19) 0.0208 (6)
O3 −0.00731 (19) 0.24467 (16) 0.52507 (17) 0.0265 (6)
O4 0.35191 (19) 0.04171 (16) 0.25344 (18) 0.0257 (6)
Ni1 0.35134 (4) 0.13565 (3) 0.01819 (3) 0.02231 (14)
HW12 0.495 (2) −0.0135 (16) 0.107 (2) 0.020 (10)*
HW11 0.440 (3) 0.034 (2) 0.166 (2) 0.053 (15)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.023 (2) 0.0180 (19) 0.0236 (19) −0.0040 (15) 0.0094 (15) −0.0067 (15)
C2 0.025 (2) 0.0174 (19) 0.0172 (18) 0.0032 (14) 0.0099 (15) 0.0011 (14)
C3 0.034 (2) 0.0166 (19) 0.037 (2) −0.0033 (16) 0.0226 (18) 0.0027 (16)
C4 0.033 (2) 0.0108 (18) 0.033 (2) 0.0005 (15) 0.0184 (18) −0.0043 (15)
C5 0.024 (2) 0.0201 (19) 0.0198 (19) 0.0018 (15) 0.0110 (15) 0.0017 (15)
C6 0.023 (2) 0.0178 (19) 0.028 (2) −0.0063 (15) 0.0133 (17) −0.0083 (16)
C7 0.0207 (18) 0.0162 (18) 0.0187 (17) 0.0009 (14) 0.0085 (14) 0.0007 (14)
C8 0.0238 (19) 0.0136 (17) 0.0162 (17) 0.0012 (14) 0.0088 (15) 0.0009 (13)
C9 0.030 (2) 0.021 (2) 0.030 (2) 0.0018 (16) 0.0157 (17) −0.0013 (16)
C10 0.034 (2) 0.0147 (19) 0.039 (2) −0.0018 (16) 0.0167 (19) −0.0041 (16)
C11 0.037 (2) 0.022 (2) 0.041 (2) −0.0094 (17) 0.021 (2) −0.0018 (17)
C12 0.030 (2) 0.025 (2) 0.028 (2) −0.0024 (16) 0.0182 (17) −0.0027 (16)
C13 0.047 (3) 0.023 (2) 0.029 (2) 0.0090 (18) 0.0076 (19) −0.0050 (17)
C14 0.057 (3) 0.035 (2) 0.026 (2) 0.019 (2) −0.004 (2) 0.0003 (18)
C15 0.035 (2) 0.024 (2) 0.027 (2) 0.0056 (17) −0.0011 (18) −0.0046 (16)
C16 0.027 (2) 0.019 (2) 0.037 (2) 0.0056 (15) 0.0124 (18) −0.0005 (16)
C17 0.030 (2) 0.020 (2) 0.039 (2) 0.0018 (16) 0.0105 (18) −0.0001 (17)
C18 0.029 (2) 0.020 (2) 0.039 (2) 0.0005 (16) 0.0105 (18) 0.0004 (17)
C19 0.033 (2) 0.020 (2) 0.036 (2) −0.0053 (16) 0.0123 (18) −0.0043 (17)
C20 0.025 (2) 0.025 (2) 0.074 (3) −0.0038 (17) 0.023 (2) −0.005 (2)
C21 0.019 (2) 0.024 (2) 0.031 (2) −0.0005 (15) 0.0100 (16) 0.0025 (16)
N4 0.0213 (17) 0.0140 (15) 0.0293 (17) −0.0003 (12) 0.0092 (13) −0.0001 (13)
C23 0.025 (2) 0.023 (2) 0.071 (3) −0.0001 (17) 0.023 (2) −0.011 (2)
N1 0.0244 (17) 0.0182 (16) 0.0264 (17) 0.0042 (12) 0.0104 (14) 0.0006 (13)
N2 0.0265 (17) 0.0127 (16) 0.0304 (17) 0.0036 (12) 0.0086 (14) 0.0024 (12)
N3 0.0238 (17) 0.0149 (16) 0.0341 (17) −0.0021 (13) 0.0099 (14) −0.0015 (13)
O1 0.0282 (14) 0.0136 (12) 0.0333 (14) 0.0018 (10) 0.0196 (11) 0.0008 (11)
O2 0.0385 (16) 0.0226 (14) 0.0284 (14) 0.0093 (11) 0.0246 (12) 0.0068 (11)
O1W 0.0230 (15) 0.0157 (14) 0.0277 (15) 0.0028 (11) 0.0138 (12) −0.0024 (11)
O3 0.0388 (16) 0.0215 (13) 0.0276 (14) 0.0028 (11) 0.0226 (12) 0.0014 (11)
O4 0.0309 (15) 0.0202 (14) 0.0316 (14) 0.0091 (11) 0.0178 (12) 0.0062 (11)
Ni1 0.0259 (3) 0.0180 (2) 0.0269 (3) 0.0016 (2) 0.0137 (2) 0.0008 (2)

Geometric parameters (Å, °)

C1—O4 1.240 (4) C16—C17 1.505 (5)
C1—O2 1.270 (4) C16—H16A 0.9700
C1—C2 1.508 (4) C16—H16B 0.9700
C2—C3 1.356 (4) C17—C18 1.525 (4)
C2—C8 1.434 (4) C17—H17A 0.9700
C3—C4 1.400 (4) C17—H17B 0.9700
C3—H3 0.9300 C18—C19 1.515 (4)
C4—C5 1.375 (4) C18—H18A 0.9700
C4—H4 0.9300 C18—H18B 0.9700
C5—C7 1.420 (4) C19—N3 1.466 (4)
C5—C6 1.500 (4) C19—H19A 0.9700
C6—O3 1.240 (4) C19—H19B 0.9700
C6—O1 1.279 (4) C20—C23 1.338 (5)
C7—C12 1.421 (4) C20—N3 1.368 (4)
C7—C8 1.424 (4) C20—H20 0.9300
C8—C9 1.412 (4) C21—N4 1.306 (4)
C9—C10 1.356 (4) C21—N3 1.341 (4)
C9—H9 0.9300 C21—H21 0.9300
C10—C11 1.392 (5) N4—C23 1.367 (4)
C10—H10 0.9300 N4—Ni1i 2.099 (3)
C11—C12 1.347 (4) C23—H23 0.9300
C11—H11 0.9300 O1—Ni1ii 2.116 (2)
C12—H12 0.9300 O1W—HW12 0.819 (16)
C13—C14 1.343 (5) O1W—HW11 0.83 (4)
C13—N1 1.355 (4) O3—Ni1ii 2.347 (2)
C13—H13 0.9300 Ni1—O1W 2.125 (2)
C14—N2 1.363 (4) Ni1—O2 2.040 (2)
C14—H14 0.9300 Ni1—O1iii 2.116 (2)
C15—N1 1.299 (4) Ni1—O3iii 2.347 (2)
C15—N2 1.334 (4) Ni1—N1 2.060 (3)
C15—H15 0.9300 Ni1—N4iv 2.099 (3)
C16—N2 1.472 (4)
O4—C1—O2 124.8 (3) H17A—C17—H17B 107.9
O4—C1—C2 120.4 (3) C19—C18—C17 110.8 (3)
O2—C1—C2 114.8 (3) C19—C18—H18A 109.5
C3—C2—C8 119.5 (3) C17—C18—H18A 109.5
C3—C2—C1 118.9 (3) C19—C18—H18B 109.5
C8—C2—C1 121.5 (3) C17—C18—H18B 109.5
C2—C3—C4 121.6 (3) H18A—C18—H18B 108.1
C2—C3—H3 119.2 N3—C19—C18 113.0 (3)
C4—C3—H3 119.2 N3—C19—H19A 109.0
C5—C4—C3 121.1 (3) C18—C19—H19A 109.0
C5—C4—H4 119.5 N3—C19—H19B 109.0
C3—C4—H4 119.5 C18—C19—H19B 109.0
C4—C5—C7 119.2 (3) H19A—C19—H19B 107.8
C4—C5—C6 119.1 (3) C23—C20—N3 106.2 (3)
C7—C5—C6 121.7 (3) C23—C20—H20 126.9
O3—C6—O1 120.7 (3) N3—C20—H20 126.9
O3—C6—C5 121.2 (3) N4—C21—N3 112.7 (3)
O1—C6—C5 118.1 (3) N4—C21—H21 123.6
C5—C7—C12 122.5 (3) N3—C21—H21 123.6
C5—C7—C8 119.6 (3) C21—N4—C23 104.3 (3)
C12—C7—C8 117.8 (3) C21—N4—Ni1i 128.0 (2)
C9—C8—C7 118.6 (3) C23—N4—Ni1i 127.4 (2)
C9—C8—C2 122.4 (3) C20—C23—N4 110.8 (3)
C7—C8—C2 118.9 (3) C20—C23—H23 124.6
C10—C9—C8 121.5 (3) N4—C23—H23 124.6
C10—C9—H9 119.2 C15—N1—C13 104.8 (3)
C8—C9—H9 119.2 C15—N1—Ni1 126.0 (2)
C9—C10—C11 119.7 (3) C13—N1—Ni1 129.1 (2)
C9—C10—H10 120.2 C15—N2—C14 105.8 (3)
C11—C10—H10 120.2 C15—N2—C16 126.7 (3)
C12—C11—C10 121.3 (3) C14—N2—C16 127.5 (3)
C12—C11—H11 119.4 C21—N3—C20 106.0 (3)
C10—C11—H11 119.4 C21—N3—C19 125.8 (3)
C11—C12—C7 121.1 (3) C20—N3—C19 128.1 (3)
C11—C12—H12 119.5 C6—O1—Ni1ii 94.87 (19)
C7—C12—H12 119.5 C1—O2—Ni1 130.1 (2)
C14—C13—N1 110.2 (3) Ni1—O1W—HW12 126 (2)
C14—C13—H13 124.9 Ni1—O1W—HW11 97 (3)
N1—C13—H13 124.9 HW12—O1W—HW11 110 (2)
C13—C14—N2 106.3 (3) C6—O3—Ni1ii 85.3 (2)
C13—C14—H14 126.9 O2—Ni1—N1 85.93 (10)
N2—C14—H14 126.9 O2—Ni1—N4iv 102.65 (10)
N1—C15—N2 112.9 (3) N1—Ni1—N4iv 96.70 (11)
N1—C15—H15 123.6 O2—Ni1—O1iii 159.34 (9)
N2—C15—H15 123.6 N1—Ni1—O1iii 94.01 (10)
N2—C16—C17 112.4 (3) N4iv—Ni1—O1iii 97.87 (10)
N2—C16—H16A 109.1 O2—Ni1—O1W 85.20 (9)
C17—C16—H16A 109.1 N1—Ni1—O1W 169.33 (10)
N2—C16—H16B 109.1 N4iv—Ni1—O1W 91.03 (10)
C17—C16—H16B 109.1 O1iii—Ni1—O1W 92.20 (9)
H16A—C16—H16B 107.9 O2—Ni1—O3iii 100.97 (9)
C16—C17—C18 111.9 (3) N1—Ni1—O3iii 86.35 (10)
C16—C17—H17A 109.2 N4iv—Ni1—O3iii 156.33 (9)
C18—C17—H17A 109.2 O1iii—Ni1—O3iii 58.47 (8)
C16—C17—H17B 109.2 O1W—Ni1—O3iii 89.53 (8)
C18—C17—H17B 109.2

Symmetry codes: (i) x, y+1, z; (ii) x−1/2, −y+1/2, z+1/2; (iii) x+1/2, −y+1/2, z−1/2; (iv) x, y−1, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1W—HW12···O1v 0.819 (16) 1.847 (18) 2.661 (3) 172 (3)
O1W—HW11···O4 0.83 (4) 1.83 (4) 2.651 (3) 169 (3)

Symmetry codes: (v) −x+1/2, y−1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB2770).

References

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  2. Bruker (1998). SMART, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
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  4. 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/S1600536808024008/hb2770sup1.cif

e-64-m1105-sup1.cif (20.3KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808024008/hb2770Isup2.hkl

e-64-m1105-Isup2.hkl (199.6KB, hkl)

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


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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