Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 May 25;67(Pt 6):m796–m797. doi: 10.1107/S1600536811019118

Bis(μ-2-{[2-(1,3-benzothia­zol-2-yl)hydrazinyl­idene]meth­yl}-6-meth­oxy­phenolato)bis­[dinitratodysprosium(III)] methanol disolvate

Xuebin Xu a, Shuai Ding a, Si Shen b, Jinkui Tang b, Zhiliang Liu a,*
PMCID: PMC3120308  PMID: 21754674

Abstract

In the centrosymmetric dinuclear title compound, [Dy2(C15H12N3O2S)2(NO3)4]·2CH3OH, the two DyIII atoms are coordinated by two deprotonated 2-{[2-(1,3-benzothia­zol-2-yl)hydrazinyl­idene]meth­yl}-6-meth­oxy­phenol ligands and four nitrate ions, all of which are chelating. The crystal packing is stabilized by inter­molecular N—H⋯O hydrogen bonds and weak O—H⋯O inter­actions, forming a two-dimensional network parallel to (010).

Related literature

For applications of dysprosium complexes in data storage and processing, see: Lin et al. (2010). For the preparation of the 2-{[2-(1,3-benzothia­zol-2-yl)hydrazinyl­idene]meth­yl}-6-meth­oxy­phenol ligand, see: Patil et al. (2009). For related structures, see: Lin & Hong (2009); Lin et al. (2008); Xu et al. (2010).graphic file with name e-67-0m796-scheme1.jpg

Experimental

Crystal data

  • [Dy2(C15H12N3O2S)2(NO3)4]·2CH4O

  • M r = 1233.82

  • Triclinic, Inline graphic

  • a = 9.6191 (6) Å

  • b = 10.1002 (7) Å

  • c = 11.6151 (8) Å

  • α = 112.045 (1)°

  • β = 105.065 (1)°

  • γ = 93.154 (1)°

  • V = 995.23 (12) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 3.92 mm−1

  • T = 159 K

  • 0.20 × 0.10 × 0.10 mm

Data collection

  • Rigaku Saturn CCD area-detector diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2002) T min = 0.631, T max = 0.676

  • 5083 measured reflections

  • 3502 independent reflections

  • 3162 reflections with I > 2σ(I)

  • R int = 0.016

Refinement

  • R[F 2 > 2σ(F 2)] = 0.025

  • wR(F 2) = 0.057

  • S = 1.07

  • 3502 reflections

  • 292 parameters

  • H-atom parameters constrained

  • Δρmax = 0.83 e Å−3

  • Δρmin = −0.51 e Å−3

Data collection: CrystalClear (Rigaku, 2002); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2006) and XP (Siemens, 1994); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811019118/jj2083sup1.cif

e-67-0m796-sup1.cif (26.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811019118/jj2083Isup2.hkl

e-67-0m796-Isup2.hkl (171.7KB, hkl)

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

Table 1. Selected bond lengths (Å).

Dy1—O2 2.280 (3)
Dy1—O2i 2.374 (2)
Dy1—O1i 2.394 (3)
Dy1—O4 2.422 (3)
Dy1—O3 2.433 (3)
Dy1—N4 2.461 (3)
Dy1—O6 2.471 (3)
Dy1—N5 2.494 (3)
Dy1—O8 2.530 (3)

Symmetry code: (i) Inline graphic.

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

D—H⋯A D—H H⋯A DA D—H⋯A
O9—H9A⋯O3ii 0.84 2.64 3.206 (4) 126
O9—H9A⋯O8iii 0.84 2.24 3.049 (4) 161
N9—H9⋯O9iv 0.88 1.91 2.751 (4) 160

Symmetry codes: (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic.

Acknowledgments

Financial support by the NSFC (20761004, 21061009) and the Inner Mongolia Autonomous Region Fund for Natural Science (2010MS0201) is gratefully acknowledged. This work was supported by the "211 project" of the postgraduate student programme of Inner Mongolia University.

supplementary crystallographic information

Comment

Dysprosium complexes continue to attract significant attention because of their potential applications in data storage and processing (Lin et al. 2010). In order to explore the relationship between these applications and their structures, a series of dinuclear dysprosium coordination compounds have been structural characterized (Lin et al. 2008; Xu et al. 2010). In support of our continued research in this area, we report here a new dinuclear dysprosium complex, [Dy2(C15H12N3O2S)2(NO3)4].CH3OH.

In the title compound the asymmetric unit consists of one DyIII ion, one deprotonated 2-[(benzothiazol-2-yl)hydrazonomethyl]-6-methoxyphenol ligand and two nitrate ions (Fig. 1). The centrosymmetric dinuclear complex is composed of two nine-coordinate DyIII ions bridged by phenoxo groups (O2, O2a) from the ligands with a Dy1—O2—Dy1a angle of 106.041 (100) ° and a Dy···Dy distance equal to 3.7184 (3) Å. The central core Dy2O2 appears to be nearly rhombic with the two Dy—O2 distances being 2.37 Å and 2.28 Å, respectively. Crystal packing is stabiized by N—H···O hydrogen bonds and weak O—H···O intermolecular interactions forming a two-dimensional network (Fig. 2).

Experimental

A mixture of Dy(NO3)3.6H2O (0.1 mmol), 2-hydrazino benzothiazole (0.1 mmol), 2-hydroxy-3-methoxy-5-((4-methoxyphenyl)diazenyl)benzaldehyde (0.1 mmol), methanol (10 ml), Et3N (0.3 mmol) was sealed in a glass vessel (20 ml, capacity) and the solution was heated at 363 K for 1 h under autogenous pressure. After the mixture was allowed to cool to room temperature, yellow block single crystals were isolated from the vessel.

Refinement

The H atoms were placed in geometrically idealized positions (C—H = 0.95 Å and O—H = 0.82–0.84 Å), with Uiso(H) = 1.2Ueq(C) and Uiso(H) = 1.5Ueq(O).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, with atom labels and 30% probability displacement ellipsoids. Hydrogen atoms are omitted for clarity.

Fig. 2.

Fig. 2.

Packing diagram of the title compound. Hydrogen bonds are shown as dashed lines.

Crystal data

[Dy2(C15H12N3O2S)2(NO3)4]·2CH4O Z = 1
Mr = 1233.82 F(000) = 602
Triclinic, P1 Dx = 2.059 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 9.6191 (6) Å Cell parameters from 3776 reflections
b = 10.1002 (7) Å θ = 2.3–25.1°
c = 11.6151 (8) Å µ = 3.92 mm1
α = 112.045 (1)° T = 159 K
β = 105.065 (1)° Block, yellow
γ = 93.154 (1)° 0.20 × 0.10 × 0.10 mm
V = 995.23 (12) Å3

Data collection

Rigaku Saturn CCD area-detector diffractometer 3502 independent reflections
Radiation source: rotating anode 3162 reflections with I > 2σ(I)
confocal Rint = 0.016
Detector resolution: 7.31 pixels mm-1 θmax = 25.1°, θmin = 2.0°
ω and φ scans h = −11→11
Absorption correction: multi-scan (CrystalClear; Rigaku, 2002) k = −12→7
Tmin = 0.631, Tmax = 0.676 l = −13→13
5083 measured reflections

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)] = 0.025 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.057 H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0289P)2 + 0.127P] where P = (Fo2 + 2Fc2)/3
3502 reflections (Δ/σ)max = 0.001
292 parameters Δρmax = 0.83 e Å3
0 restraints Δρmin = −0.51 e Å3

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 0.5488 (5) −0.1481 (6) 1.3423 (4) 0.0419 (12)
H1A 0.4829 −0.0989 1.3895 0.063*
H1B 0.6488 −0.0946 1.3876 0.063*
H1C 0.5453 −0.2468 1.3387 0.063*
C2 0.3550 (4) −0.2085 (4) 1.1420 (4) 0.0262 (9)
C3 0.2744 (5) −0.3007 (5) 1.1704 (4) 0.0328 (10)
H3 0.3194 −0.3323 1.2363 0.039*
C4 0.1277 (5) −0.3481 (5) 1.1034 (4) 0.0349 (10)
H4 0.0711 −0.4143 1.1208 0.042*
C5 0.0654 (4) −0.2974 (5) 1.0113 (4) 0.0314 (10)
H5 −0.0365 −0.3263 0.9677 0.038*
C6 0.1455 (4) −0.2054 (4) 0.9789 (4) 0.0259 (9)
C7 0.2972 (4) −0.1615 (4) 1.0421 (4) 0.0237 (8)
C8 0.0613 (4) −0.1613 (5) 0.8805 (4) 0.0308 (10)
H8 −0.0395 −0.2025 0.8423 0.037*
C9 0.0364 (4) 0.0701 (5) 0.7244 (4) 0.0285 (9)
C10 0.1564 (4) 0.2767 (4) 0.7467 (4) 0.0265 (9)
C11 0.2636 (4) 0.3998 (5) 0.7988 (4) 0.0309 (10)
H11 0.3530 0.4075 0.8617 0.037*
C12 0.2378 (5) 0.5099 (5) 0.7573 (4) 0.0335 (10)
H12 0.3112 0.5930 0.7904 0.040*
C13 0.1059 (5) 0.5011 (5) 0.6680 (4) 0.0354 (10)
H13 0.0902 0.5791 0.6421 0.042*
C14 −0.0026 (5) 0.3818 (5) 0.6163 (4) 0.0335 (10)
H14 −0.0930 0.3764 0.5557 0.040*
C15 0.0251 (4) 0.2701 (5) 0.6558 (4) 0.0284 (9)
C16 0.2951 (6) 0.3287 (6) 0.4354 (5) 0.0540 (14)
H16A 0.2585 0.3862 0.3858 0.081*
H16C 0.3978 0.3682 0.4862 0.081*
H16B 0.2374 0.3326 0.4945 0.081*
Dy1 0.358298 (18) 0.05304 (2) 0.890365 (17) 0.02346 (8)
N4 0.1097 (3) −0.0726 (4) 0.8405 (3) 0.0283 (8)
N5 0.1632 (3) 0.1587 (4) 0.7829 (3) 0.0274 (8)
N6 0.3542 (4) 0.3093 (4) 1.1063 (3) 0.0345 (9)
N7 0.3601 (4) −0.1898 (4) 0.6517 (3) 0.0327 (8)
N9 0.0038 (3) −0.0478 (4) 0.7456 (3) 0.0327 (8)
H9 −0.0802 −0.1070 0.7020 0.039*
O1 0.5034 (3) −0.1543 (3) 1.2102 (3) 0.0291 (6)
O2 0.3863 (3) −0.0823 (3) 1.0113 (2) 0.0249 (6)
O3 0.2717 (3) 0.1897 (3) 1.0724 (3) 0.0340 (7)
O4 0.4335 (3) 0.3079 (3) 1.0330 (3) 0.0337 (7)
O5 0.3585 (4) 0.4152 (4) 1.2012 (3) 0.0574 (10)
O6 0.2613 (3) −0.1127 (3) 0.6575 (3) 0.0371 (7)
O7 0.3620 (4) −0.2850 (4) 0.5512 (3) 0.0580 (10)
O8 0.4579 (3) −0.1600 (3) 0.7589 (3) 0.0416 (8)
O9 0.2828 (3) 0.1836 (4) 0.3486 (3) 0.0452 (8)
H9A 0.3398 0.1790 0.3038 0.068*
S1 −0.09430 (11) 0.11034 (12) 0.61321 (10) 0.0315 (2)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.033 (2) 0.062 (3) 0.028 (2) 0.002 (2) 0.0030 (19) 0.020 (2)
C2 0.021 (2) 0.029 (2) 0.027 (2) 0.0045 (17) 0.0058 (17) 0.0110 (18)
C3 0.036 (2) 0.029 (2) 0.033 (2) 0.006 (2) 0.0075 (19) 0.014 (2)
C4 0.033 (2) 0.033 (2) 0.041 (3) 0.002 (2) 0.011 (2) 0.017 (2)
C5 0.022 (2) 0.035 (2) 0.034 (2) 0.0027 (18) 0.0075 (18) 0.011 (2)
C6 0.0188 (19) 0.028 (2) 0.030 (2) 0.0037 (17) 0.0051 (17) 0.0118 (18)
C7 0.0183 (19) 0.022 (2) 0.028 (2) 0.0031 (16) 0.0038 (16) 0.0095 (18)
C8 0.016 (2) 0.037 (3) 0.033 (2) 0.0030 (18) 0.0006 (17) 0.013 (2)
C9 0.019 (2) 0.037 (2) 0.028 (2) 0.0086 (18) 0.0036 (17) 0.013 (2)
C10 0.023 (2) 0.032 (2) 0.024 (2) 0.0070 (18) 0.0049 (17) 0.0117 (18)
C11 0.022 (2) 0.039 (3) 0.030 (2) 0.0060 (19) 0.0039 (17) 0.014 (2)
C12 0.029 (2) 0.035 (2) 0.032 (2) 0.003 (2) 0.0046 (19) 0.012 (2)
C13 0.039 (2) 0.039 (3) 0.031 (2) 0.011 (2) 0.006 (2) 0.019 (2)
C14 0.031 (2) 0.042 (3) 0.028 (2) 0.012 (2) 0.0021 (19) 0.019 (2)
C15 0.020 (2) 0.038 (2) 0.022 (2) 0.0059 (18) 0.0028 (16) 0.0086 (19)
C16 0.043 (3) 0.069 (4) 0.044 (3) 0.009 (3) 0.011 (2) 0.018 (3)
Dy1 0.01390 (10) 0.03118 (12) 0.02375 (11) 0.00321 (8) 0.00021 (7) 0.01318 (9)
N4 0.0175 (16) 0.033 (2) 0.0301 (18) −0.0005 (15) −0.0019 (14) 0.0156 (16)
N5 0.0207 (17) 0.0310 (19) 0.0281 (18) 0.0054 (15) 0.0046 (14) 0.0110 (16)
N6 0.033 (2) 0.039 (2) 0.029 (2) 0.0144 (18) 0.0035 (17) 0.0152 (19)
N7 0.0199 (18) 0.036 (2) 0.031 (2) 0.0019 (16) −0.0010 (15) 0.0067 (18)
N9 0.0144 (16) 0.045 (2) 0.0347 (19) −0.0018 (16) −0.0072 (14) 0.0229 (18)
O1 0.0195 (13) 0.0415 (17) 0.0277 (15) 0.0034 (13) 0.0010 (11) 0.0199 (14)
O2 0.0146 (13) 0.0316 (16) 0.0279 (14) 0.0016 (12) 0.0007 (11) 0.0156 (13)
O3 0.0291 (16) 0.0430 (19) 0.0312 (16) 0.0091 (15) 0.0063 (13) 0.0177 (15)
O4 0.0285 (15) 0.0393 (18) 0.0298 (15) 0.0044 (14) 0.0036 (13) 0.0138 (14)
O5 0.086 (3) 0.041 (2) 0.041 (2) 0.021 (2) 0.0250 (19) 0.0073 (18)
O6 0.0229 (15) 0.0449 (19) 0.0318 (16) 0.0119 (14) −0.0016 (13) 0.0087 (15)
O7 0.0373 (19) 0.066 (3) 0.037 (2) 0.0132 (18) −0.0008 (16) −0.0066 (19)
O8 0.0351 (17) 0.0463 (19) 0.0321 (16) 0.0152 (15) −0.0033 (14) 0.0117 (15)
O9 0.0258 (17) 0.057 (2) 0.046 (2) −0.0010 (16) 0.0079 (14) 0.0163 (18)
S1 0.0212 (5) 0.0388 (6) 0.0302 (5) 0.0037 (5) −0.0020 (4) 0.0161 (5)

Geometric parameters (Å, °)

C1—O1 1.459 (5) C13—H13 0.9500
C1—H1A 0.9800 C14—C15 1.384 (6)
C1—H1B 0.9800 C14—H14 0.9500
C1—H1C 0.9800 C15—S1 1.752 (4)
C2—C3 1.364 (6) C16—O9 1.410 (6)
C2—O1 1.402 (4) C16—H16A 0.9800
C2—C7 1.410 (5) C16—H16C 0.9800
C3—C4 1.379 (6) C16—H16B 0.9800
C3—H3 0.9500 Dy1—O2 2.280 (3)
C4—C5 1.370 (6) Dy1—O2i 2.374 (2)
C4—H4 0.9500 Dy1—O1i 2.394 (3)
C5—C6 1.390 (5) Dy1—O4 2.422 (3)
C5—H5 0.9500 Dy1—O3 2.433 (3)
C6—C7 1.412 (5) Dy1—N4 2.461 (3)
C6—C8 1.451 (5) Dy1—O6 2.471 (3)
C7—O2 1.342 (4) Dy1—N5 2.494 (3)
C8—N4 1.270 (5) Dy1—O8 2.530 (3)
C8—H8 0.9500 Dy1—Dy1i 3.7184 (4)
C9—N5 1.320 (5) N4—N9 1.402 (4)
C9—N9 1.340 (5) N6—O5 1.203 (5)
C9—S1 1.738 (4) N6—O3 1.273 (5)
C10—C11 1.395 (6) N6—O4 1.279 (4)
C10—C15 1.399 (5) N7—O7 1.208 (5)
C10—N5 1.405 (5) N7—O6 1.261 (4)
C11—C12 1.379 (6) N7—O8 1.266 (4)
C11—H11 0.9500 N9—H9 0.8800
C12—C13 1.388 (6) O1—Dy1i 2.394 (3)
C12—H12 0.9500 O2—Dy1i 2.374 (2)
C13—C14 1.376 (6) O9—H9A 0.8400
O1—C1—H1A 109.5 O4—Dy1—O3 52.63 (10)
O1—C1—H1B 109.5 O2—Dy1—N4 75.53 (10)
H1A—C1—H1B 109.5 O2i—Dy1—N4 149.07 (10)
O1—C1—H1C 109.5 O1i—Dy1—N4 138.80 (10)
H1A—C1—H1C 109.5 O4—Dy1—N4 121.11 (11)
H1B—C1—H1C 109.5 O3—Dy1—N4 74.17 (11)
C3—C2—O1 122.0 (4) O2—Dy1—O6 108.45 (10)
C3—C2—C7 123.2 (4) O2i—Dy1—O6 116.45 (9)
O1—C2—C7 114.8 (3) O1i—Dy1—O6 76.95 (10)
C2—C3—C4 120.1 (4) O4—Dy1—O6 141.79 (10)
C2—C3—H3 120.0 O3—Dy1—O6 139.92 (10)
C4—C3—H3 120.0 N4—Dy1—O6 69.16 (10)
C5—C4—C3 118.5 (4) O2—Dy1—N5 139.17 (10)
C5—C4—H4 120.8 O2i—Dy1—N5 144.17 (10)
C3—C4—H4 120.8 O1i—Dy1—N5 81.46 (10)
C4—C5—C6 122.6 (4) O4—Dy1—N5 79.22 (10)
C4—C5—H5 118.7 O3—Dy1—N5 79.08 (10)
C6—C5—H5 118.7 N4—Dy1—N5 66.52 (11)
C5—C6—C7 119.6 (4) O6—Dy1—N5 72.05 (10)
C5—C6—C8 115.0 (4) O2—Dy1—O8 77.32 (10)
C7—C6—C8 125.3 (4) O2i—Dy1—O8 70.22 (9)
O2—C7—C2 119.8 (3) O1i—Dy1—O8 76.42 (10)
O2—C7—C6 124.3 (3) O4—Dy1—O8 140.65 (10)
C2—C7—C6 115.8 (3) O3—Dy1—O8 153.86 (10)
N4—C8—C6 126.1 (4) N4—Dy1—O8 98.23 (11)
N4—C8—H8 117.0 O6—Dy1—O8 50.52 (9)
C6—C8—H8 117.0 N5—Dy1—O8 121.51 (10)
N5—C9—N9 123.9 (4) O2—Dy1—Dy1i 37.86 (6)
N5—C9—S1 117.3 (3) O2i—Dy1—Dy1i 36.10 (6)
N9—C9—S1 118.8 (3) O1i—Dy1—Dy1i 103.10 (6)
C11—C10—C15 119.0 (4) O4—Dy1—Dy1i 92.27 (7)
C11—C10—N5 125.8 (3) O3—Dy1—Dy1i 90.23 (7)
C15—C10—N5 115.2 (4) N4—Dy1—Dy1i 113.24 (8)
C12—C11—C10 118.9 (4) O6—Dy1—Dy1i 118.59 (7)
C12—C11—H11 120.6 N5—Dy1—Dy1i 169.00 (8)
C10—C11—H11 120.6 O8—Dy1—Dy1i 69.47 (6)
C11—C12—C13 120.9 (4) C8—N4—N9 114.2 (3)
C11—C12—H12 119.5 C8—N4—Dy1 131.6 (3)
C13—C12—H12 119.5 N9—N4—Dy1 114.1 (2)
C14—C13—C12 121.5 (4) C9—N5—C10 109.1 (3)
C14—C13—H13 119.3 C9—N5—Dy1 113.1 (3)
C12—C13—H13 119.3 C10—N5—Dy1 136.6 (2)
C13—C14—C15 117.4 (4) O5—N6—O3 122.4 (4)
C13—C14—H14 121.3 O5—N6—O4 122.6 (4)
C15—C14—H14 121.3 O3—N6—O4 115.0 (3)
C14—C15—C10 122.3 (4) O7—N7—O6 122.5 (4)
C14—C15—S1 127.6 (3) O7—N7—O8 122.2 (4)
C10—C15—S1 109.9 (3) O6—N7—O8 115.2 (3)
O9—C16—H16A 109.5 C9—N9—N4 117.0 (3)
O9—C16—H16C 109.5 C9—N9—H9 121.5
H16A—C16—H16C 109.5 N4—N9—H9 121.5
O9—C16—H16B 109.5 C2—O1—C1 114.9 (3)
H16A—C16—H16B 109.5 C2—O1—Dy1i 116.7 (2)
H16C—C16—H16B 109.5 C1—O1—Dy1i 127.7 (2)
O2—Dy1—O2i 73.96 (10) C7—O2—Dy1 136.2 (2)
O2—Dy1—O1i 139.27 (9) C7—O2—Dy1i 117.7 (2)
O2i—Dy1—O1i 68.12 (9) Dy1—O2—Dy1i 106.04 (10)
O2—Dy1—O4 109.76 (9) N6—O3—Dy1 95.9 (2)
O2i—Dy1—O4 74.78 (9) N6—O4—Dy1 96.3 (2)
O1i—Dy1—O4 74.29 (10) N7—O6—Dy1 98.6 (2)
O2—Dy1—O3 76.56 (10) N7—O8—Dy1 95.6 (2)
O2i—Dy1—O3 103.27 (9) C16—O9—H9A 109.5
O1i—Dy1—O3 125.83 (10) C9—S1—C15 88.36 (19)
O1—C2—C3—C4 178.1 (4) C8—N4—N9—C9 162.8 (4)
C7—C2—C3—C4 −2.5 (7) Dy1—N4—N9—C9 −20.4 (4)
C2—C3—C4—C5 −1.7 (6) C3—C2—O1—C1 −25.7 (5)
C3—C4—C5—C6 2.8 (7) C7—C2—O1—C1 154.9 (4)
C4—C5—C6—C7 0.2 (6) C3—C2—O1—Dy1i 162.7 (3)
C4—C5—C6—C8 −179.3 (4) C7—C2—O1—Dy1i −16.7 (4)
C3—C2—C7—O2 −173.5 (4) C2—C7—O2—Dy1 −167.5 (3)
O1—C2—C7—O2 6.0 (5) C6—C7—O2—Dy1 13.8 (6)
C3—C2—C7—C6 5.3 (6) C2—C7—O2—Dy1i 7.9 (5)
O1—C2—C7—C6 −175.2 (3) C6—C7—O2—Dy1i −170.8 (3)
C5—C6—C7—O2 174.7 (4) O2i—Dy1—O2—C7 175.7 (4)
C8—C6—C7—O2 −6.0 (6) O1i—Dy1—O2—C7 −162.4 (3)
C5—C6—C7—C2 −4.1 (6) O4—Dy1—O2—C7 108.9 (3)
C8—C6—C7—C2 175.3 (4) O3—Dy1—O2—C7 67.4 (3)
C5—C6—C8—N4 176.4 (4) N4—Dy1—O2—C7 −9.4 (3)
C7—C6—C8—N4 −3.0 (7) O6—Dy1—O2—C7 −71.2 (3)
C15—C10—C11—C12 −1.1 (6) N5—Dy1—O2—C7 12.5 (4)
N5—C10—C11—C12 −176.9 (4) O8—Dy1—O2—C7 −111.5 (3)
C10—C11—C12—C13 1.8 (6) Dy1i—Dy1—O2—C7 175.7 (4)
C11—C12—C13—C14 −1.0 (7) O2i—Dy1—O2—Dy1i 0.0
C12—C13—C14—C15 −0.5 (6) O1i—Dy1—O2—Dy1i 21.83 (19)
C13—C14—C15—C10 1.2 (6) O4—Dy1—O2—Dy1i −66.82 (12)
C13—C14—C15—S1 176.6 (3) O3—Dy1—O2—Dy1i −108.32 (12)
C11—C10—C15—C14 −0.5 (6) N4—Dy1—O2—Dy1i 174.87 (13)
N5—C10—C15—C14 175.8 (4) O6—Dy1—O2—Dy1i 113.12 (11)
C11—C10—C15—S1 −176.5 (3) N5—Dy1—O2—Dy1i −163.24 (12)
N5—C10—C15—S1 −0.2 (4) O8—Dy1—O2—Dy1i 72.77 (11)
C6—C8—N4—N9 −179.2 (4) O5—N6—O3—Dy1 −175.9 (4)
C6—C8—N4—Dy1 4.8 (7) O4—N6—O3—Dy1 3.2 (3)
O2—Dy1—N4—C8 0.1 (4) O2—Dy1—O3—N6 126.4 (2)
O2i—Dy1—N4—C8 9.7 (5) O2i—Dy1—O3—N6 56.8 (2)
O1i—Dy1—N4—C8 153.4 (3) O1i—Dy1—O3—N6 −15.6 (2)
O4—Dy1—N4—C8 −104.5 (4) O4—Dy1—O3—N6 −1.92 (19)
O3—Dy1—N4—C8 −79.8 (4) N4—Dy1—O3—N6 −155.1 (2)
O6—Dy1—N4—C8 116.7 (4) O6—Dy1—O3—N6 −130.8 (2)
N5—Dy1—N4—C8 −164.5 (4) N5—Dy1—O3—N6 −86.6 (2)
O8—Dy1—N4—C8 74.6 (4) O8—Dy1—O3—N6 128.8 (3)
Dy1i—Dy1—N4—C8 3.5 (4) Dy1i—Dy1—O3—N6 90.8 (2)
O2—Dy1—N4—N9 −176.0 (3) O5—N6—O4—Dy1 175.9 (4)
O2i—Dy1—N4—N9 −166.4 (2) O3—N6—O4—Dy1 −3.2 (3)
O1i—Dy1—N4—N9 −22.7 (3) O2—Dy1—O4—N6 −52.3 (2)
O4—Dy1—N4—N9 79.4 (3) O2i—Dy1—O4—N6 −118.6 (2)
O3—Dy1—N4—N9 104.2 (3) O1i—Dy1—O4—N6 170.4 (2)
O6—Dy1—N4—N9 −59.4 (3) O3—Dy1—O4—N6 1.91 (19)
N5—Dy1—N4—N9 19.4 (2) N4—Dy1—O4—N6 32.4 (2)
O8—Dy1—N4—N9 −101.4 (3) O6—Dy1—O4—N6 127.8 (2)
Dy1i—Dy1—N4—N9 −172.6 (2) N5—Dy1—O4—N6 86.3 (2)
N9—C9—N5—C10 −175.2 (4) O8—Dy1—O4—N6 −146.3 (2)
S1—C9—N5—C10 5.1 (4) Dy1i—Dy1—O4—N6 −86.6 (2)
N9—C9—N5—Dy1 15.4 (5) O7—N7—O6—Dy1 −176.6 (4)
S1—C9—N5—Dy1 −164.29 (19) O8—N7—O6—Dy1 3.1 (4)
C11—C10—N5—C9 173.0 (4) O2—Dy1—O6—N7 −56.8 (2)
C15—C10—N5—C9 −3.0 (5) O2i—Dy1—O6—N7 24.1 (3)
C11—C10—N5—Dy1 −21.3 (6) O1i—Dy1—O6—N7 81.2 (2)
C15—C10—N5—Dy1 162.7 (3) O4—Dy1—O6—N7 123.1 (2)
O2—Dy1—N5—C9 −40.9 (3) O3—Dy1—O6—N7 −147.7 (2)
O2i—Dy1—N5—C9 167.3 (2) N4—Dy1—O6—N7 −122.6 (2)
O1i—Dy1—N5—C9 135.7 (3) N5—Dy1—O6—N7 166.3 (3)
O4—Dy1—N5—C9 −148.7 (3) O8—Dy1—O6—N7 −1.8 (2)
O3—Dy1—N5—C9 −95.1 (3) Dy1i—Dy1—O6—N7 −16.8 (2)
N4—Dy1—N5—C9 −17.7 (3) O7—N7—O8—Dy1 176.7 (4)
O6—Dy1—N5—C9 56.8 (3) O6—N7—O8—Dy1 −3.0 (4)
O8—Dy1—N5—C9 67.5 (3) O2—Dy1—O8—N7 129.1 (2)
Dy1i—Dy1—N5—C9 −108.9 (4) O2i—Dy1—O8—N7 −153.6 (3)
O2—Dy1—N5—C10 153.8 (3) O1i—Dy1—O8—N7 −82.3 (2)
O2i—Dy1—N5—C10 2.0 (5) O4—Dy1—O8—N7 −125.1 (2)
O1i—Dy1—N5—C10 −29.6 (4) O3—Dy1—O8—N7 126.7 (3)
O4—Dy1—N5—C10 46.0 (4) N4—Dy1—O8—N7 56.0 (2)
O3—Dy1—N5—C10 99.6 (4) O6—Dy1—O8—N7 1.8 (2)
N4—Dy1—N5—C10 177.0 (4) N5—Dy1—O8—N7 −11.4 (3)
O6—Dy1—N5—C10 −108.5 (4) Dy1i—Dy1—O8—N7 167.8 (3)
O8—Dy1—N5—C10 −97.8 (4) N5—C9—S1—C15 −4.6 (3)
Dy1i—Dy1—N5—C10 85.8 (5) N9—C9—S1—C15 175.7 (4)
N5—C9—N9—N4 3.2 (6) C14—C15—S1—C9 −173.3 (4)
S1—C9—N9—N4 −177.1 (3) C10—C15—S1—C9 2.4 (3)

Symmetry codes: (i) −x+1, −y, −z+2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O9—H9A···O3ii 0.84 2.64 3.206 (4) 126
O9—H9A···O8iii 0.84 2.24 3.049 (4) 161
N9—H9···O9iv 0.88 1.91 2.751 (4) 160

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JJ2083).

References

  1. Brandenburg, K. & Putz, H. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  2. Lin, P.-H., Burchell, T. J., Clérac, R. & Murugesu, M. (2008). Angew. Chem. Int. Ed. 47, 8848–8851. [DOI] [PubMed]
  3. Lin, S.-Y., Guo, Y.-N., Xu, G.-F. & Tang, J.-K. (2010). Chin. J. Appl. Chem. 27, 1365–1371.
  4. Lin, Y.-C. & Hong, F.-E. (2009). Acta Cryst. E65, m1077. [DOI] [PMC free article] [PubMed]
  5. Patil, S. A., Weng, C.-M., Huang, P.-C. & Hong, F.-E. (2009). Tetrahedron, 65, 2889–2897.
  6. Rigaku (2002). CrystalClear Rigaku Corporation, Tokyo, Japan.
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  8. Siemens (1994). XP Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.
  9. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
  10. Xu, G.-F., Wang, Q.-L., Gamez, P., Ma, Y., Clérac, R., Tang, J.-K., Yan, S.-P., Cheng, P. & Liao, D.-Z. (2010). Chem. Commun. 46, 1506–1508. [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 I, global. DOI: 10.1107/S1600536811019118/jj2083sup1.cif

e-67-0m796-sup1.cif (26.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811019118/jj2083Isup2.hkl

e-67-0m796-Isup2.hkl (171.7KB, 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

RESOURCES