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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Dec 22;69(Pt 1):m63–m64. doi: 10.1107/S1600536812050775

Tris(1,10-phenanthroline-κ2 N,N′)nickel(II) hexa­oxido-μ-peroxido-disulfate­(VI) N,N-dimethyl­formamide disolvate monohydrate

Miguel Angel Harvey a,b,*, Sebastián Suarez c,*, Fabio Doctorovich c, Ricardo Baggio d
PMCID: PMC3588241  PMID: 23476355

Abstract

The asymmetric unit of the title complex, [Ni(C12H8N2)3]S2O8·2C3H7NO·H2O, consists of a complex [Ni(phen)3]2+ cation and one isolated pds anion, with two DMF mol­ecules and one water mol­ecule as solvates (where phen is 1,10-phenanthroline, pds is the hexa­oxido-μ-peroxoido-di­sulf­ate dianion and DMF is dimethyl­formamide). The [Ni(phen)3]2+ cation is regular, with an almost ideal NiII bond-valence sum of 2.07 v.u. The group, as well as the water solvent mol­ecule, are well behaved in terms of crystallographic order, but the remaining three mol­ecules in the structure display different kinds of disorder, viz. the two DMF mol­ecules mimic a twofold splitting and the pds anion has both S atoms clamped at well-determined positions but with a not-too-well-defined central part. These peculiar behaviours are a consequence of the hydrogen-bonding inter­actions: the outermost SO3 parts of the pds anion are heavily connected to the complex cations via C—H⋯O hydrogen bonding, generating an [Ni(phen)3]pds network and providing for the stability of the terminal pds sites. Also, the water solvent mol­ecule is strongly bound to the structure (being a donor of two strong bonds and an acceptor of one) and is accordingly perfectly ordered. The peroxide O atoms in the pds middle region, instead, appear as much less restrained into their sites, which may explain their tendency to disorder. The cation–anion network leaves large embedded holes, amounting to about 28% of the total crystal volume, which are occupied by the DMF mol­ecules. The latter are weakly inter­acting with the rest of the structure, which renders them much more labile and, accordingly, prone to disorder.

Related literature  

For information on structures with coordinated pds, see: Youngme et al. (2007); Manson et al. (2009); Harrison & Hathaway (1980); Blackman et al. (1991); Harvey et al. (2011) and references therein. For examples of structurers with non-coordinating pds groups, see Baffert et al. (2009); Harvey et al. (2004, 2005); Youngme et al. (2008); Singh et al. (2009). For details of bond-valence analysis and the vector bond-valence model, see: Brown & Altermatt (1985) and Harvey et al. (2006), respectively.graphic file with name e-69-00m63-scheme1.jpg

Experimental  

Crystal data  

  • [Ni(C12H8N2)3](S2O8)·2C3H7NO·H2O

  • M r = 955.65

  • Triclinic, Inline graphic

  • a = 10.4832 (3) Å

  • b = 12.2221 (4) Å

  • c = 18.0044 (6) Å

  • α = 79.691 (3)°

  • β = 76.725 (3)°

  • γ = 76.190 (3)°

  • V = 2161.41 (12) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.62 mm−1

  • T = 294 K

  • 0.18 × 0.11 × 0.11 mm

Data collection  

  • Oxford Diffraction Gemini CCD S Ultra diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) T min = 0.945, T max = 0.952

  • 31646 measured reflections

  • 10070 independent reflections

  • 6165 reflections with I > 2σ(I)

  • R int = 0.041

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.056

  • wR(F 2) = 0.170

  • S = 1.04

  • 10070 reflections

  • 647 parameters

  • 246 restraints

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

  • Δρmax = 0.65 e Å−3

  • Δρmin = −0.73 e Å−3

Data collection: CrysAlis PRO (Oxford Diffraction, 2009); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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 and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812050775/br2216sup1.cif

e-69-00m63-sup1.cif (48KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050775/br2216Isup2.hkl

e-69-00m63-Isup2.hkl (492.4KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—H1WA⋯O6i 0.85 (5) 2.02 (6) 2.839 (7) 160 (10)
O1W—H1WB⋯O1Di 0.85 (7) 1.90 (7) 2.668 (10) 149 (7)
C3B—H3B⋯O1W ii 0.93 2.54 3.305 (8) 139
C1B—H1B⋯O3ii 0.93 2.55 3.192 (6) 126
C3A—H3A⋯O8 0.93 2.59 3.271 (6) 130
C3C—H3C⋯O1iii 0.93 2.43 3.337 (6) 164
C5A—H5A⋯O3 0.93 2.58 3.505 (7) 170
C5C—H5C⋯O2iii 0.93 2.53 3.365 (7) 150
C6B—H6B⋯O1i 0.93 2.53 3.434 (5) 163
C6C—H6C⋯O2iv 0.93 2.56 3.409 (6) 151
C8C—H8C⋯O3iv 0.93 2.30 3.197 (6) 162
C10A—H10A⋯O8v 0.93 2.48 3.220 (6) 137
C10C—H10C⋯O1E 0.93 2.59 3.228 (19) 126

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

Acknowledgments

The authors acknowledge the ANPCyT (project No. PME 2006–01113) for the purchase of the Oxford Gemini CCD diffractometer and the Spanish Research Council (CSIC) for provision of a free-of-charge license to the Cambridge Structural Database (Allen, 2002).

supplementary crystallographic information

Comment

The binding behavior of peroxodisulfate (pds) towards a number of transition metal metal cations (Cd(II), Hg(II), Cu(II), Mn(III), Zn(II), Ag(II)) has been well documentated in the literature Youngme et al., 2007; Manson et al., 2009., Blackman et al., 1991; Harrison et al., 1980; Harvey et al., 2011, and references therein) but its rather elusive character as a ligand has also been evidenced in many other structures where the anion wouldn't coordinate, thus acting as a balancing counterion or, in occasions, just as a neutral co-crystallization agent in the form of peroxodisulfuric acid. Among the cations being reluctant towards pds coordination it must be mentioned the case of Cd (Harvey et al., 2005); Co(III) (Singh et al., 2009); Zn(II) (Harvey et al., 2004), Cu(II) (Youngme et al., 2008), Mn(IV) (Baffert et al., 2009), and even the more stringent case of Ni, of which no crystal structure with pds had been reported up to date: in particular, all our previous experiments aimed to produce such a complex had so far been unsuccessful.

Therefore, we present herein the first NiII-pds structure, where the anion did not enter into the NiII coordination sphere but behaves instead as a stabilizing counteranion: [Ni(phen)3]2+.(pds).2DMF.(H2O), where (phen: 1,10-phenanthroline; pds: peroxidisulfate dianion; DMF: dimethylformamide).

The asymmetric unit of the complex consists of a globular [Ni(phen)3]2+ nucleus (Fig 1a), one isolated pds anion, two DMF and one water molecules as solvates.

The [Ni(phen)3]2+ cationic centre is absolutely regular and does not differ from the more than 100 similar groups which appear in the v5.33 version of the CSD (Allen, 2002). The Bond Valence Sum for the NiII cation in the title compound (Brown and Altermatt, 1985) is almost ideal (2.07 v.u.), and the regularity in the NiN6 coordination sphere is shown by the tight range of similar parameters (d(Ni-N): 2.087 (3)-2.100 (3)Å; N-Ni-N cis angles: 79.04 (12)-79.71 (12)° (chelating); 92.79 (12)-96.46 (12)° (non-chelating); N-Ni-N trans angles: 172.06 (12)-170.20 (12)°), but it can perhaps be best assessed by the geometric disposition of the three Bond Valence Vectors associated to the three chelating phen ligands (for details, see Harvey et al., 2006) which define an absolute planar array (sum of internal angles: 360.00°), and a theoretical (almost nil) resultant vector ( 0.017 v.u.). The cationic group as well as the water solvate are well behaved in terms of crystallographic order, but the remaining three groups in the structure display different kinds of disorder, as explained in detail in the refinement section, the two DMF mimicking different kinds of two-fold splitting (Figs. 1c,1d) with occupation factors of 0.546 (12)/0.454 (12) and 0.520 (12)/0.480 (12), respectively. In the case of pds this occurs in a more complicated fashion, having both S's "clamped" at two well determined positions (Fig 1b) and a not-so-well-defined central part (Occupation for O4,O5:0.641 (3)).

These peculiar behaviours may be better understood by inspection of Table 1, which gives the H-bonding interactions, and their representation in Fig 2. It is clearly seen therein that the outermost SO3 parts of the pds anion are strongly connected to the cationic centres via H-bonding (10 donors out of 13 correspond to these groups), generating a sort of stable [Ni(phen)3]-pds network and acting as a clamp for the terminal SO3 groups. The oxygens in the pds middle region, instead, are much less restrained to their sites, and this could explain some tendency to disorder. Similar mobility restrictions apply to the water solvate, donor of two strong bonds (Table 1, entries 1 and 2) and acceptor of one (3rd entry). On the other hand, the above cationic-anionic network leaves large embedded holes (about 28% of the total crystal volume, as calculated by PLATON, Spek, 2009). These holes are occupied by the DMF molecules (in light tracing in Fig 2). Analysis of the acceptors in Table 1 and inspection of Figure 2 reaveals that they hardly interact with the rest of the structure, being thus labile and, accordingly, prone to disorder.

Experimental

The title compound was prepared by adding DMF to a solid, equimolar mixture of [Ni(CH3COO)2].4H2O, K2S2O8 and phen.H2O in such a way that phen final concentration was 0.500 M. Crystals suitable for X-ray diffraction developed in a few hours.

Refinement

All C—H atoms were found in a difference map, but treated differently in refinement. Those attached to C were further idealized and finally allowed to ride. CH3 groups were also free to rotate. Water H's were refined with restrained d(O-H). In all cases displacement parameters were taken as Uiso(H) = X×Ueq(host) [d(CH)methyl = 0.96 A°, X = 1.5; d(C—H)arom = 0.93 Å, X = 1.2; O - H = 0.85 (1)Å, X = 1.2].

A rather peculiar characteristic of the structure was its having the two DMF solvates as well as the pds anion disordered, all of them in different ways: in both DMF molecules the disorder mimics a two fold symmetry, with the pseudo two fold axis by force passing throuh the central N; in the case of moieties E (D) this occurs with the pseudo diad being perpendicular (parallel) to one of the to the two C(methyl)—N lines, Fig 1c (1d).

The case of the pds anion was not that clear cut, but interesting anyway: the molecule occupies in the crystal several, slightly offset positons, all of them with the S atoms "clamped" in the S1, S2 reported coordinates (No "ghosts" in their neighbourhood). The central oxygens O4 and O5, instead, presented a clear splitting which needed to be included in the model in order to have a proper refinement. The coresponding outermost minoritarian oxygens, however, could not be clearly disclosed and have to be accordingly disregarded. To compensate for this fact, atoms O1-O3, O6-O8 were given full occupancy. This procedure, fulfilled with some restraints in metrics and in displacement factors, allowed to reduce the R factor by more ~10%, and the s.u.'s for the O4, O5 coordinates in ~30%.

Figures

Fig. 1.

Fig. 1.

Ellipsoid plot of the different constituents of (I), drawn at a 30% displacement factor level. (a): The Ni(phen)3 nucleus. (b): The S2O82- anion. Note the minoritarian S fractions, around O4 and O5. (c) and (d): the two disordered DMF molecules, with different pseudo two-fold symmetry, and the well behaved water solvate.

Fig. 2.

Fig. 2.

A packing view of (I) drawn down b and showing the way in which the cationic-anionic H-bonding network builds up. DMF units (in light lining) appear in the structural voids, with almost no connections to the rest. Only H atoms involved in H-bonding have been represented.

Crystal data

[Ni(C12H8N2)3](S2O8)·2C3H7NO·H2O Z = 2
Mr = 955.65 F(000) = 992
Triclinic, P1 Dx = 1.468 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 10.4832 (3) Å Cell parameters from 11752 reflections
b = 12.2221 (4) Å θ = 3.7–28.8°
c = 18.0044 (6) Å µ = 0.62 mm1
α = 79.691 (3)° T = 294 K
β = 76.725 (3)° Block, light brown
γ = 76.190 (3)° 0.18 × 0.11 × 0.11 mm
V = 2161.41 (12) Å3

Data collection

Oxford Diffraction Gemini CCD S Ultra diffractometer 10070 independent reflections
Radiation source: fine-focus sealed tube 6165 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.041
ω scans, thick slices θmax = 28.9°, θmin = 3.7°
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) h = −14→14
Tmin = 0.945, Tmax = 0.952 k = −15→16
31646 measured reflections l = −24→24

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)] = 0.056 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.170 H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.096P)2] where P = (Fo2 + 2Fc2)/3
10070 reflections (Δ/σ)max = 0.007
647 parameters Δρmax = 0.65 e Å3
246 restraints Δρmin = −0.73 e Å3

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Ni1 0.21814 (5) 0.29652 (4) 0.27142 (3) 0.04038 (18)
N1A 0.3061 (3) 0.4386 (3) 0.25528 (18) 0.0449 (8)
N2A 0.4160 (3) 0.2281 (3) 0.22251 (18) 0.0441 (8)
C1A 0.2489 (5) 0.5435 (4) 0.2693 (3) 0.0564 (11)
H1A 0.1571 0.5607 0.2880 0.068*
C2A 0.3211 (6) 0.6290 (4) 0.2570 (3) 0.0707 (14)
H2A 0.2781 0.7014 0.2690 0.085*
C3A 0.4549 (6) 0.6067 (4) 0.2273 (3) 0.0678 (14)
H3A 0.5037 0.6636 0.2191 0.081*
C4A 0.5186 (5) 0.4977 (4) 0.2092 (2) 0.0552 (11)
C5A 0.6573 (5) 0.4663 (5) 0.1758 (3) 0.0713 (14)
H5A 0.7109 0.5198 0.1667 0.086*
C6A 0.7116 (5) 0.3623 (5) 0.1573 (3) 0.0770 (16)
H6A 0.8021 0.3451 0.1349 0.092*
C7A 0.6338 (4) 0.2757 (4) 0.1711 (3) 0.0603 (12)
C8A 0.6837 (5) 0.1661 (5) 0.1533 (3) 0.0751 (15)
H8A 0.7735 0.1447 0.1307 0.090*
C9A 0.6032 (5) 0.0890 (4) 0.1684 (3) 0.0722 (14)
H9A 0.6366 0.0158 0.1554 0.087*
C10A 0.4690 (5) 0.1224 (4) 0.2038 (3) 0.0576 (11)
H10A 0.4143 0.0696 0.2150 0.069*
C11A 0.4973 (4) 0.3038 (4) 0.2064 (2) 0.0457 (9)
C12A 0.4382 (4) 0.4166 (3) 0.2246 (2) 0.0441 (9)
N1B 0.0317 (3) 0.3791 (3) 0.32722 (18) 0.0429 (7)
N2B 0.2391 (3) 0.2495 (3) 0.38604 (18) 0.0448 (8)
C1B −0.0697 (4) 0.4466 (4) 0.2978 (3) 0.0546 (11)
H1B −0.0617 0.4583 0.2446 0.066*
C2B −0.1862 (4) 0.5002 (4) 0.3420 (3) 0.0588 (12)
H2B −0.2541 0.5467 0.3187 0.071*
C3B −0.2005 (4) 0.4843 (4) 0.4201 (3) 0.0571 (11)
H3B −0.2777 0.5206 0.4505 0.068*
C4B −0.0975 (4) 0.4125 (4) 0.4541 (2) 0.0496 (10)
C5B −0.1039 (5) 0.3901 (4) 0.5355 (3) 0.0626 (12)
H5B −0.1807 0.4218 0.5685 0.075*
C6B 0.0010 (5) 0.3229 (4) 0.5651 (2) 0.0597 (12)
H6B −0.0056 0.3088 0.6182 0.072*
C7B 0.1210 (5) 0.2737 (4) 0.5163 (2) 0.0517 (10)
C8B 0.2324 (5) 0.2047 (4) 0.5435 (3) 0.0658 (13)
H8B 0.2316 0.1898 0.5961 0.079*
C9B 0.3413 (5) 0.1598 (5) 0.4931 (3) 0.0715 (14)
H9B 0.4154 0.1135 0.5108 0.086*
C10B 0.3418 (5) 0.1835 (4) 0.4142 (3) 0.0598 (11)
H10B 0.4171 0.1519 0.3801 0.072*
C11B 0.1296 (4) 0.2931 (3) 0.4367 (2) 0.0415 (9)
C12B 0.0175 (4) 0.3637 (3) 0.4050 (2) 0.0407 (8)
N1C 0.1500 (3) 0.1494 (3) 0.26890 (19) 0.0473 (8)
N2C 0.1687 (3) 0.3320 (3) 0.16241 (18) 0.0460 (8)
C1C 0.1412 (5) 0.0598 (4) 0.3217 (3) 0.0600 (12)
H1C 0.1629 0.0600 0.3690 0.072*
C2C 0.1005 (5) −0.0353 (4) 0.3093 (3) 0.0705 (14)
H2C 0.0949 −0.0967 0.3479 0.085*
C3C 0.0693 (5) −0.0374 (4) 0.2410 (4) 0.0704 (14)
H3C 0.0424 −0.1004 0.2323 0.084*
C4C 0.0774 (4) 0.0547 (4) 0.1836 (3) 0.0570 (11)
C5C 0.0484 (5) 0.0587 (5) 0.1095 (3) 0.0703 (14)
H5C 0.0206 −0.0022 0.0982 0.084*
C6C 0.0606 (5) 0.1494 (5) 0.0558 (3) 0.0718 (15)
H6C 0.0429 0.1490 0.0075 0.086*
C7C 0.0999 (4) 0.2462 (4) 0.0706 (2) 0.0591 (12)
C8C 0.1121 (5) 0.3444 (5) 0.0179 (3) 0.0732 (15)
H8C 0.0942 0.3494 −0.0310 0.088*
C9C 0.1498 (5) 0.4320 (5) 0.0378 (3) 0.0720 (14)
H9C 0.1572 0.4973 0.0030 0.086*
C10C 0.1774 (5) 0.4233 (4) 0.1108 (2) 0.0576 (11)
H10C 0.2030 0.4840 0.1239 0.069*
C11C 0.1301 (4) 0.2445 (4) 0.1436 (2) 0.0458 (9)
C12C 0.1190 (4) 0.1469 (3) 0.2003 (2) 0.0457 (9)
O1W 0.5525 (6) 0.4757 (5) 0.5714 (3) 0.1193 (17)
H1WA 0.547 (10) 0.410 (3) 0.596 (4) 0.179*
H1WB 0.516 (10) 0.522 (5) 0.604 (4) 0.179*
S1 0.87231 (13) 0.74846 (10) 0.19276 (6) 0.0597 (3)
S2 0.51188 (14) 0.84299 (10) 0.32020 (7) 0.0632 (3)
O1 0.9510 (4) 0.7297 (3) 0.2484 (2) 0.0913 (12)
O2 0.8815 (4) 0.8464 (3) 0.13880 (19) 0.0892 (12)
O3 0.8770 (5) 0.6481 (3) 0.1618 (2) 0.0980 (12)
O4 0.7174 (4) 0.7544 (4) 0.2327 (3) 0.0779 (13) 0.617 (3)
O5 0.6654 (4) 0.8441 (5) 0.2768 (3) 0.0797 (14) 0.617 (3)
O6 0.5143 (6) 0.7390 (3) 0.3684 (2) 0.1142 (16)
O7 0.5037 (4) 0.9379 (3) 0.3577 (2) 0.0915 (12)
O8 0.4358 (4) 0.8641 (3) 0.2626 (2) 0.0968 (13)
N1D 0.7290 (6) 0.1726 (5) 0.4231 (3) 0.0937 (15)
O1D' 0.5753 (9) 0.3293 (7) 0.3748 (5) 0.106 (4) 0.544 (12)
C1D 0.6338 (8) 0.2719 (7) 0.4278 (5) 0.106 (2)
H1DD 0.6100 0.2998 0.4750 0.127* 0.544 (12)
H1DA 0.6247 0.2977 0.4765 0.159* 0.456 (12)
H1DB 0.5495 0.2585 0.4233 0.159* 0.456 (12)
H1DC 0.6608 0.3288 0.3869 0.159* 0.456 (12)
O1D" 0.8949 (16) 0.0480 (15) 0.4893 (8) 0.167 (7) 0.456 (12)
C2D 0.7955 (10) 0.1257 (8) 0.4819 (5) 0.128 (3)
H2DB 0.7639 0.1718 0.5230 0.192* 0.544 (12)
H2DC 0.8898 0.1219 0.4636 0.192* 0.544 (12)
H2DD 0.7796 0.0505 0.5004 0.192* 0.544 (12)
H2DA 0.7581 0.1594 0.5265 0.154* 0.456 (12)
C3D 0.7575 (9) 0.1204 (9) 0.3550 (5) 0.156 (4)
H3D1 0.7890 0.1720 0.3115 0.235*
H3D2 0.6777 0.1016 0.3479 0.235*
H3D3 0.8253 0.0525 0.3594 0.235*
N1E 0.4039 (7) 0.7569 (6) 0.0434 (4) 0.1133 (18)
C1E' 0.506 (2) 0.689 (2) 0.0074 (13) 0.166 (9) 0.524 (12)
H1EA 0.5868 0.7140 0.0062 0.250* 0.524 (12)
H1EB 0.4951 0.6906 −0.0443 0.250* 0.524 (12)
H1EC 0.5112 0.6132 0.0339 0.250* 0.524 (12)
C2E' 0.399 (3) 0.8651 (17) 0.0685 (14) 0.173 (8) 0.524 (12)
H2EA 0.4886 0.8776 0.0610 0.259* 0.524 (12)
H2EB 0.3585 0.8633 0.1221 0.259* 0.524 (12)
H2EC 0.3475 0.9255 0.0391 0.259* 0.524 (12)
C3E' 0.265 (2) 0.7430 (19) 0.0550 (11) 0.128 (5) 0.524 (12)
H3EA 0.1969 0.7961 0.0796 0.154* 0.524 (12)
O1E' 0.238 (2) 0.6704 (15) 0.0354 (9) 0.171 (6) 0.524 (12)
C1E" 0.296 (3) 0.826 (3) 0.0685 (15) 0.179 (10) 0.476 (12)
H1ED 0.2207 0.7918 0.0722 0.268* 0.476 (12)
H1EE 0.2879 0.8951 0.0337 0.268* 0.476 (12)
H1EF 0.2989 0.8412 0.1184 0.268* 0.476 (12)
C2E" 0.539 (2) 0.797 (2) 0.0370 (14) 0.164 (8) 0.476 (12)
H2ED 0.5188 0.8739 0.0485 0.246* 0.476 (12)
H2EE 0.5904 0.7939 −0.0143 0.246* 0.476 (12)
H2EF 0.5892 0.7484 0.0729 0.246* 0.476 (12)
C3E" 0.436 (3) 0.6469 (19) 0.0256 (13) 0.122 (5) 0.476 (12)
H3EB 0.5246 0.6116 0.0105 0.146* 0.476 (12)
O1E" 0.356 (3) 0.602 (2) 0.0292 (11) 0.181 (7) 0.476 (12)
O4' 0.7492 (13) 0.8086 (11) 0.2641 (7) 0.100 (4)* 0.383 (3)
O5' 0.650 (2) 0.759 (2) 0.3001 (13) 0.078 (8)* 0.180 (10)
O5" 0.6248 (15) 0.8221 (12) 0.2377 (9) 0.050 (5)* 0.202 (10)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ni1 0.0430 (3) 0.0411 (3) 0.0384 (3) −0.0093 (2) −0.0099 (2) −0.0055 (2)
N1A 0.052 (2) 0.0410 (18) 0.0427 (18) −0.0085 (15) −0.0085 (15) −0.0111 (14)
N2A 0.0477 (19) 0.0378 (18) 0.0443 (18) −0.0061 (15) −0.0075 (15) −0.0042 (14)
C1A 0.065 (3) 0.050 (3) 0.056 (3) −0.010 (2) −0.007 (2) −0.019 (2)
C2A 0.099 (4) 0.045 (3) 0.074 (3) −0.021 (3) −0.010 (3) −0.023 (2)
C3A 0.092 (4) 0.061 (3) 0.064 (3) −0.042 (3) −0.013 (3) −0.012 (2)
C4A 0.066 (3) 0.062 (3) 0.048 (2) −0.029 (2) −0.016 (2) −0.006 (2)
C5A 0.063 (3) 0.092 (4) 0.071 (3) −0.044 (3) −0.011 (3) −0.006 (3)
C6A 0.046 (3) 0.101 (5) 0.083 (4) −0.027 (3) −0.005 (3) −0.005 (3)
C7A 0.045 (2) 0.069 (3) 0.059 (3) −0.007 (2) −0.005 (2) −0.002 (2)
C8A 0.051 (3) 0.077 (4) 0.077 (3) 0.010 (3) 0.002 (2) −0.006 (3)
C9A 0.068 (3) 0.053 (3) 0.077 (3) 0.014 (3) −0.003 (3) −0.009 (2)
C10A 0.064 (3) 0.050 (3) 0.054 (3) −0.007 (2) −0.009 (2) −0.003 (2)
C11A 0.044 (2) 0.053 (2) 0.040 (2) −0.0096 (19) −0.0093 (17) −0.0028 (18)
C12A 0.045 (2) 0.051 (2) 0.039 (2) −0.0152 (19) −0.0107 (17) −0.0042 (17)
N1B 0.0424 (18) 0.0446 (18) 0.0401 (17) −0.0111 (15) −0.0093 (14) 0.0034 (14)
N2B 0.0461 (19) 0.0437 (18) 0.0460 (18) −0.0046 (15) −0.0145 (15) −0.0087 (15)
C1B 0.045 (2) 0.066 (3) 0.047 (2) −0.005 (2) −0.0110 (19) 0.001 (2)
C2B 0.040 (2) 0.058 (3) 0.070 (3) −0.003 (2) −0.010 (2) 0.002 (2)
C3B 0.040 (2) 0.063 (3) 0.062 (3) −0.007 (2) 0.002 (2) −0.013 (2)
C4B 0.047 (2) 0.053 (2) 0.048 (2) −0.018 (2) 0.0004 (18) −0.0088 (19)
C5B 0.061 (3) 0.080 (3) 0.049 (3) −0.024 (3) 0.003 (2) −0.018 (2)
C6B 0.073 (3) 0.071 (3) 0.038 (2) −0.023 (3) −0.004 (2) −0.012 (2)
C7B 0.061 (3) 0.057 (3) 0.040 (2) −0.018 (2) −0.013 (2) −0.0051 (19)
C8B 0.079 (3) 0.080 (3) 0.044 (2) −0.013 (3) −0.026 (2) −0.007 (2)
C9B 0.070 (3) 0.085 (4) 0.061 (3) −0.001 (3) −0.034 (3) −0.006 (3)
C10B 0.053 (3) 0.067 (3) 0.059 (3) −0.001 (2) −0.022 (2) −0.010 (2)
C11B 0.048 (2) 0.043 (2) 0.039 (2) −0.0168 (18) −0.0115 (17) −0.0066 (16)
C12B 0.042 (2) 0.042 (2) 0.041 (2) −0.0174 (17) −0.0052 (16) −0.0070 (16)
N1C 0.0462 (19) 0.053 (2) 0.0458 (19) −0.0155 (16) −0.0105 (15) −0.0049 (16)
N2C 0.0463 (19) 0.051 (2) 0.0401 (17) −0.0078 (16) −0.0085 (15) −0.0060 (15)
C1C 0.070 (3) 0.052 (3) 0.062 (3) −0.022 (2) −0.018 (2) −0.001 (2)
C2C 0.074 (3) 0.052 (3) 0.089 (4) −0.023 (3) −0.020 (3) 0.001 (3)
C3C 0.059 (3) 0.060 (3) 0.104 (4) −0.019 (2) −0.018 (3) −0.029 (3)
C4C 0.041 (2) 0.061 (3) 0.074 (3) −0.010 (2) −0.010 (2) −0.026 (2)
C5C 0.059 (3) 0.082 (4) 0.083 (4) −0.014 (3) −0.015 (3) −0.044 (3)
C6C 0.059 (3) 0.102 (4) 0.064 (3) −0.003 (3) −0.021 (2) −0.043 (3)
C7C 0.044 (2) 0.087 (3) 0.047 (2) 0.000 (2) −0.0112 (19) −0.026 (2)
C8C 0.067 (3) 0.106 (4) 0.042 (3) 0.001 (3) −0.019 (2) −0.013 (3)
C9C 0.078 (3) 0.083 (4) 0.045 (3) −0.006 (3) −0.017 (2) 0.010 (3)
C10C 0.062 (3) 0.061 (3) 0.045 (2) −0.010 (2) −0.012 (2) 0.002 (2)
C11C 0.0330 (19) 0.061 (3) 0.042 (2) −0.0020 (18) −0.0055 (16) −0.0170 (19)
C12C 0.035 (2) 0.052 (2) 0.052 (2) −0.0083 (18) −0.0062 (17) −0.0164 (19)
O1W 0.096 (3) 0.109 (4) 0.127 (4) −0.023 (3) −0.002 (3) 0.029 (3)
S1 0.0785 (8) 0.0605 (7) 0.0471 (6) −0.0279 (6) −0.0163 (6) −0.0020 (5)
S2 0.0782 (8) 0.0452 (6) 0.0671 (7) −0.0088 (6) −0.0203 (6) −0.0065 (5)
O1 0.113 (3) 0.085 (3) 0.096 (3) −0.028 (2) −0.059 (2) −0.002 (2)
O2 0.127 (3) 0.075 (2) 0.067 (2) −0.039 (2) −0.019 (2) 0.0123 (17)
O3 0.166 (4) 0.079 (2) 0.066 (2) −0.047 (2) −0.032 (2) −0.0130 (17)
O4 0.085 (2) 0.082 (3) 0.084 (3) −0.034 (3) −0.021 (2) −0.028 (2)
O5 0.080 (2) 0.066 (3) 0.104 (4) −0.016 (2) −0.025 (2) −0.027 (2)
O6 0.182 (5) 0.066 (2) 0.090 (3) −0.041 (3) −0.021 (3) 0.0140 (19)
O7 0.132 (3) 0.063 (2) 0.088 (3) −0.008 (2) −0.037 (2) −0.0262 (18)
O8 0.108 (3) 0.062 (2) 0.141 (3) −0.004 (2) −0.074 (3) −0.021 (2)
N1D 0.094 (4) 0.109 (4) 0.084 (3) −0.041 (3) −0.013 (3) −0.008 (3)
O1D' 0.115 (7) 0.096 (6) 0.120 (7) −0.034 (5) −0.049 (6) 0.006 (5)
C1D 0.110 (5) 0.100 (5) 0.120 (6) −0.044 (4) −0.030 (4) −0.006 (4)
O1D" 0.152 (12) 0.213 (16) 0.108 (9) −0.004 (9) −0.034 (8) 0.019 (9)
C2D 0.146 (7) 0.135 (7) 0.107 (5) −0.041 (5) −0.042 (5) 0.013 (5)
C3D 0.122 (7) 0.223 (10) 0.121 (6) 0.005 (7) −0.018 (5) −0.076 (7)
N1E 0.117 (5) 0.102 (4) 0.100 (4) −0.005 (4) −0.003 (4) −0.006 (3)
C1E' 0.156 (13) 0.162 (17) 0.126 (14) 0.037 (13) 0.000 (13) −0.003 (12)
C2E' 0.183 (18) 0.131 (12) 0.206 (18) −0.065 (12) 0.003 (16) −0.035 (11)
C3E' 0.139 (9) 0.107 (11) 0.135 (12) −0.038 (9) −0.006 (10) −0.015 (10)
O1E' 0.226 (16) 0.144 (12) 0.152 (11) −0.085 (12) −0.001 (12) −0.029 (9)
C1E" 0.132 (12) 0.175 (18) 0.173 (17) 0.027 (14) 0.015 (15) −0.017 (17)
C2E" 0.146 (12) 0.138 (15) 0.204 (19) −0.051 (12) −0.010 (15) −0.011 (14)
C3E" 0.146 (14) 0.121 (10) 0.103 (11) −0.045 (9) −0.025 (11) 0.001 (10)
O1E" 0.220 (19) 0.204 (15) 0.152 (12) −0.120 (14) −0.040 (14) 0.000 (12)

Geometric parameters (Å, º)

Ni1—N2B 2.088 (3) C4C—C12C 1.402 (6)
Ni1—N2C 2.089 (3) C4C—C5C 1.425 (7)
Ni1—N1B 2.090 (3) C5C—C6C 1.344 (7)
Ni1—N2A 2.091 (3) C5C—H5C 0.9300
Ni1—N1C 2.098 (3) C6C—C7C 1.428 (7)
Ni1—N1A 2.100 (3) C6C—H6C 0.9300
N1A—C1A 1.321 (5) C7C—C8C 1.403 (7)
N1A—C12A 1.349 (5) C7C—C11C 1.416 (5)
N2A—C10A 1.347 (5) C8C—C9C 1.356 (7)
N2A—C11A 1.355 (5) C8C—H8C 0.9300
C1A—C2A 1.391 (6) C9C—C10C 1.390 (6)
C1A—H1A 0.9300 C9C—H9C 0.9300
C2A—C3A 1.361 (7) C10C—H10C 0.9300
C2A—H2A 0.9300 C11C—C12C 1.433 (6)
C3A—C4A 1.399 (7) O1W—H1WA 0.854 (13)
C3A—H3A 0.9300 O1W—H1WB 0.850 (13)
C4A—C12A 1.400 (6) S1—O1 1.395 (3)
C4A—C5A 1.428 (7) S1—O2 1.408 (3)
C5A—C6A 1.330 (8) S1—O3 1.422 (3)
C5A—H5A 0.9300 S1—O4 1.608 (3)
C6A—C7A 1.439 (7) S2—O8 1.401 (3)
C6A—H6A 0.9300 S2—O6 1.403 (3)
C7A—C8A 1.384 (7) S2—O7 1.420 (3)
C7A—C11A 1.412 (6) S2—O5 1.622 (3)
C8A—C9A 1.362 (7) O4—O5 1.399 (4)
C8A—H8A 0.9300 N1D—C2D 1.366 (9)
C9A—C10A 1.400 (7) N1D—C1D 1.377 (9)
C9A—H9A 0.9300 N1D—C3D 1.422 (9)
C10A—H10A 0.9300 O1D'—C1D 1.267 (10)
C11A—C12A 1.433 (6) C1D—H1DD 0.9300
N1B—C1B 1.332 (5) C1D—H1DA 0.9600
N1B—C12B 1.357 (5) C1D—H1DB 0.9600
N2B—C10B 1.326 (5) C1D—H1DC 0.9600
N2B—C11B 1.354 (5) O1D"—C2D 1.246 (15)
C1B—C2B 1.383 (6) C2D—H2DB 0.9600
C1B—H1B 0.9300 C2D—H2DC 0.9600
C2B—C3B 1.362 (6) C2D—H2DD 0.9600
C2B—H2B 0.9300 C2D—H2DA 0.9300
C3B—C4B 1.403 (6) C3D—H3D1 0.9600
C3B—H3B 0.9300 C3D—H3D2 0.9600
C4B—C12B 1.395 (5) C3D—H3D3 0.9600
C4B—C5B 1.431 (6) N1E—C1E" 1.28 (2)
C5B—C6B 1.360 (7) N1E—C1E' 1.30 (2)
C5B—H5B 0.9300 N1E—C3E" 1.38 (2)
C6B—C7B 1.427 (6) N1E—C2E' 1.46 (2)
C6B—H6B 0.9300 N1E—C3E' 1.47 (2)
C7B—C11B 1.395 (5) N1E—C2E" 1.58 (2)
C7B—C8B 1.400 (6) C1E'—H1EA 0.9600
C8B—C9B 1.354 (7) C1E'—H1EB 0.9600
C8B—H8B 0.9300 C1E'—H1EC 0.9600
C9B—C10B 1.397 (6) C2E'—H2EA 0.9600
C9B—H9B 0.9300 C2E'—H2EB 0.9600
C10B—H10B 0.9300 C2E'—H2EC 0.9600
C11B—C12B 1.449 (5) C3E'—O1E' 1.13 (2)
N1C—C1C 1.322 (5) C3E'—H3EA 0.9300
N1C—C12C 1.354 (5) C1E"—H1ED 0.9600
N2C—C10C 1.326 (5) C1E"—H1EE 0.9600
N2C—C11C 1.349 (5) C1E"—H1EF 0.9600
C1C—C2C 1.398 (6) C2E"—H2ED 0.9600
C1C—H1C 0.9300 C2E"—H2EE 0.9600
C2C—C3C 1.350 (7) C2E"—H2EF 0.9600
C2C—H2C 0.9300 C3E"—O1E" 1.09 (2)
C3C—C4C 1.390 (7) C3E"—H3EB 0.9300
C3C—H3C 0.9300
N2B—Ni1—N2C 170.47 (12) C3C—C4C—C5C 123.6 (4)
N2B—Ni1—N1B 79.71 (12) C12C—C4C—C5C 119.3 (5)
N2C—Ni1—N1B 94.79 (12) C6C—C5C—C4C 120.8 (5)
N2B—Ni1—N2A 96.45 (13) C6C—C5C—H5C 119.6
N2C—Ni1—N2A 89.93 (13) C4C—C5C—H5C 119.6
N1B—Ni1—N2A 172.08 (12) C5C—C6C—C7C 122.0 (4)
N2B—Ni1—N1C 92.80 (13) C5C—C6C—H6C 119.0
N2C—Ni1—N1C 79.70 (13) C7C—C6C—H6C 119.0
N1B—Ni1—N1C 93.56 (13) C8C—C7C—C11C 116.6 (4)
N2A—Ni1—N1C 93.54 (13) C8C—C7C—C6C 125.0 (4)
N2B—Ni1—N1A 94.40 (12) C11C—C7C—C6C 118.5 (5)
N2C—Ni1—N1A 93.77 (13) C9C—C8C—C7C 120.3 (4)
N1B—Ni1—N1A 94.29 (13) C9C—C8C—H8C 119.9
N2A—Ni1—N1A 79.02 (13) C7C—C8C—H8C 119.9
N1C—Ni1—N1A 170.17 (13) C8C—C9C—C10C 119.4 (5)
C1A—N1A—C12A 117.9 (4) C8C—C9C—H9C 120.3
C1A—N1A—Ni1 128.8 (3) C10C—C9C—H9C 120.3
C12A—N1A—Ni1 113.3 (3) N2C—C10C—C9C 122.6 (5)
C10A—N2A—C11A 117.9 (4) N2C—C10C—H10C 118.7
C10A—N2A—Ni1 128.7 (3) C9C—C10C—H10C 118.7
C11A—N2A—Ni1 113.4 (3) N2C—C11C—C7C 122.5 (4)
N1A—C1A—C2A 122.4 (5) N2C—C11C—C12C 118.2 (3)
N1A—C1A—H1A 118.8 C7C—C11C—C12C 119.4 (4)
C2A—C1A—H1A 118.8 N1C—C12C—C4C 123.0 (4)
C3A—C2A—C1A 119.8 (5) N1C—C12C—C11C 116.9 (3)
C3A—C2A—H2A 120.1 C4C—C12C—C11C 120.1 (4)
C1A—C2A—H2A 120.1 H1WA—O1W—H1WB 105 (3)
C2A—C3A—C4A 119.6 (4) O1—S1—O2 115.5 (2)
C2A—C3A—H3A 120.2 O1—S1—O3 112.9 (3)
C4A—C3A—H3A 120.2 O2—S1—O3 115.6 (2)
C12A—C4A—C3A 116.5 (4) O1—S1—O4 110.5 (3)
C12A—C4A—C5A 119.4 (4) O2—S1—O4 108.3 (3)
C3A—C4A—C5A 124.1 (4) O3—S1—O4 91.0 (2)
C6A—C5A—C4A 121.5 (4) O8—S2—O6 117.0 (3)
C6A—C5A—H5A 119.2 O8—S2—O7 115.2 (2)
C4A—C5A—H5A 119.2 O6—S2—O7 115.1 (3)
C5A—C6A—C7A 121.6 (5) O8—S2—O5 106.7 (3)
C5A—C6A—H6A 119.2 O6—S2—O5 106.5 (3)
C7A—C6A—H6A 119.2 O7—S2—O5 92.5 (2)
C8A—C7A—C11A 117.4 (4) O5—O4—S1 112.6 (3)
C8A—C7A—C6A 124.6 (5) O4—O5—S2 111.3 (3)
C11A—C7A—C6A 117.9 (5) C2D—N1D—C1D 121.1 (7)
C9A—C8A—C7A 121.0 (5) C2D—N1D—C3D 120.7 (8)
C9A—C8A—H8A 119.5 C1D—N1D—C3D 118.2 (7)
C7A—C8A—H8A 119.5 O1D'—C1D—N1D 127.0 (9)
C8A—C9A—C10A 118.5 (5) O1D'—C1D—H1DD 116.5
C8A—C9A—H9A 120.7 N1D—C1D—H1DD 116.5
C10A—C9A—H9A 120.7 O1D'—C1D—H1DA 123.2
N2A—C10A—C9A 122.7 (4) N1D—C1D—H1DA 109.5
N2A—C10A—H10A 118.6 N1D—C1D—H1DB 109.5
C9A—C10A—H10A 118.6 H1DD—C1D—H1DB 100.5
N2A—C11A—C7A 122.5 (4) H1DA—C1D—H1DB 109.5
N2A—C11A—C12A 117.1 (4) N1D—C1D—H1DC 109.5
C7A—C11A—C12A 120.4 (4) H1DD—C1D—H1DC 110.9
N1A—C12A—C4A 123.7 (4) H1DA—C1D—H1DC 109.5
N1A—C12A—C11A 117.2 (3) H1DB—C1D—H1DC 109.5
C4A—C12A—C11A 119.1 (4) O1D"—C2D—N1D 134.5 (12)
C1B—N1B—C12B 116.9 (4) O1D"—C2D—H2DB 115.3
C1B—N1B—Ni1 129.8 (3) N1D—C2D—H2DB 109.5
C12B—N1B—Ni1 113.2 (2) N1D—C2D—H2DC 109.5
C10B—N2B—C11B 117.8 (4) H2DB—C2D—H2DC 109.5
C10B—N2B—Ni1 129.0 (3) N1D—C2D—H2DD 109.5
C11B—N2B—Ni1 113.2 (2) H2DB—C2D—H2DD 109.5
N1B—C1B—C2B 123.7 (4) H2DC—C2D—H2DD 109.5
N1B—C1B—H1B 118.2 O1D"—C2D—H2DA 112.8
C2B—C1B—H1B 118.2 N1D—C2D—H2DA 112.8
C3B—C2B—C1B 119.3 (4) H2DC—C2D—H2DA 115.8
C3B—C2B—H2B 120.3 H2DD—C2D—H2DA 99.3
C1B—C2B—H2B 120.3 N1D—C3D—H3D1 109.5
C2B—C3B—C4B 119.3 (4) N1D—C3D—H3D2 109.5
C2B—C3B—H3B 120.3 H3D1—C3D—H3D2 109.5
C4B—C3B—H3B 120.3 N1D—C3D—H3D3 109.5
C12B—C4B—C3B 117.4 (4) H3D1—C3D—H3D3 109.5
C12B—C4B—C5B 119.2 (4) H3D2—C3D—H3D3 109.5
C3B—C4B—C5B 123.3 (4) C1E"—N1E—C1E' 170.5 (19)
C6B—C5B—C4B 120.7 (4) C1E"—N1E—C3E" 135 (2)
C6B—C5B—H5B 119.6 C1E'—N1E—C2E' 128.9 (19)
C4B—C5B—H5B 119.6 C3E"—N1E—C2E' 166.9 (17)
C5B—C6B—C7B 121.3 (4) C1E'—N1E—C3E' 123.3 (18)
C5B—C6B—H6B 119.4 C3E"—N1E—C3E' 83.9 (15)
C7B—C6B—H6B 119.4 C2E'—N1E—C3E' 107.2 (14)
C11B—C7B—C8B 117.0 (4) C1E"—N1E—C2E" 116.1 (19)
C11B—C7B—C6B 119.3 (4) C1E'—N1E—C2E" 68.7 (15)
C8B—C7B—C6B 123.7 (4) C3E"—N1E—C2E" 108.3 (15)
C9B—C8B—C7B 119.8 (4) C3E'—N1E—C2E" 167.8 (14)
C9B—C8B—H8B 120.1 N1E—C1E'—H1EA 109.5
C7B—C8B—H8B 120.1 N1E—C1E'—H1EB 109.5
C8B—C9B—C10B 119.6 (5) H1EA—C1E'—H1EB 109.5
C8B—C9B—H9B 120.2 N1E—C1E'—H1EC 109.5
C10B—C9B—H9B 120.2 H1EA—C1E'—H1EC 109.5
N2B—C10B—C9B 122.4 (5) H1EB—C1E'—H1EC 109.5
N2B—C10B—H10B 118.8 N1E—C2E'—H2EA 109.5
C9B—C10B—H10B 118.8 N1E—C2E'—H2EB 109.5
N2B—C11B—C7B 123.4 (4) H2EA—C2E'—H2EB 109.5
N2B—C11B—C12B 117.0 (3) N1E—C2E'—H2EC 109.5
C7B—C11B—C12B 119.6 (4) H2EA—C2E'—H2EC 109.5
N1B—C12B—C4B 123.3 (4) H2EB—C2E'—H2EC 109.5
N1B—C12B—C11B 116.9 (3) O1E'—C3E'—N1E 123 (2)
C4B—C12B—C11B 119.9 (3) O1E'—C3E'—H3EA 118.7
C1C—N1C—C12C 117.7 (4) N1E—C3E'—H3EA 118.7
C1C—N1C—Ni1 129.6 (3) N1E—C1E"—H1ED 109.5
C12C—N1C—Ni1 112.6 (3) N1E—C1E"—H1EE 109.5
C10C—N2C—C11C 118.7 (3) H1ED—C1E"—H1EE 109.5
C10C—N2C—Ni1 128.9 (3) N1E—C1E"—H1EF 109.5
C11C—N2C—Ni1 112.4 (3) H1ED—C1E"—H1EF 109.5
N1C—C1C—C2C 122.6 (4) H1EE—C1E"—H1EF 109.5
N1C—C1C—H1C 118.7 N1E—C2E"—H2ED 109.5
C2C—C1C—H1C 118.7 N1E—C2E"—H2EE 109.5
C3C—C2C—C1C 119.6 (5) H2ED—C2E"—H2EE 109.5
C3C—C2C—H2C 120.2 N1E—C2E"—H2EF 109.5
C1C—C2C—H2C 120.2 H2ED—C2E"—H2EF 109.5
C2C—C3C—C4C 120.0 (4) H2EE—C2E"—H2EF 109.5
C2C—C3C—H3C 120.0 O1E"—C3E"—N1E 120 (3)
C4C—C3C—H3C 120.0 O1E"—C3E"—H3EB 120.0
C3C—C4C—C12C 117.1 (4) N1E—C3E"—H3EB 120.0

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O1W—H1WA···O6i 0.85 (5) 2.02 (6) 2.839 (7) 160 (10)
O1W—H1WB···O1Di 0.85 (7) 1.90 (7) 2.668 (10) 149 (7)
C3B—H3B···O1Wii 0.93 2.54 3.305 (8) 139
C1B—H1B···O3ii 0.93 2.55 3.192 (6) 126
C3A—H3A···O8 0.93 2.59 3.271 (6) 130
C3C—H3C···O1iii 0.93 2.43 3.337 (6) 164
C5A—H5A···O3 0.93 2.58 3.505 (7) 170
C5C—H5C···O2iii 0.93 2.53 3.365 (7) 150
C6B—H6B···O1i 0.93 2.53 3.434 (5) 163
C6C—H6C···O2iv 0.93 2.56 3.409 (6) 151
C8C—H8C···O3iv 0.93 2.30 3.197 (6) 162
C10A—H10A···O8v 0.93 2.48 3.220 (6) 137
C10C—H10C···O1E 0.93 2.59 3.228 (19) 126

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BR2216).

References

  1. Allen, F. H. (2002). Acta Cryst. B58, 380–388. [DOI] [PubMed]
  2. Baffert, C., Orio, M., Pantazis, D. A., Duboc, C., Blackman, A. G., Blondin, G., Neese, F., Deronzier, A. & Collomb, M.-N. (2009). Inorg. Chem. 48, 10281–10288. [DOI] [PubMed]
  3. Blackman, A. G., Huffman, J. C., Lobkovsky, E. B. & Christov, G. (1991). Chem. Commun. pp. 989–990.
  4. Brown, I. D. & Altermatt, D. (1985). Acta Cryst. B41, 244–247.
  5. Harrison, W. D. & Hathaway, B. J. (1980). Acta Cryst. B36, 1069–1074.
  6. Harvey, M. A., Baggio, S. & Baggio, R. (2006). Acta Cryst. B62, 1038–1042. [DOI] [PubMed]
  7. Harvey, M. A., Baggio, S., Garland, M. T. & Baggio, R. (2005). J. Coord. Chem. 58, 243–253.
  8. Harvey, M. A., Baggio, S., Ibañez, A. & Baggio, R. (2004). Acta Cryst. C60, m375–m381. [DOI] [PubMed]
  9. Harvey, M. A., Diaz de Vivar, M. E., Baggio, R. & Baggio, S. (2011). J. Chem. Crystallogr. 41, 1717–1721.
  10. Manson, J. L., Stone, K. H., Southerland, H. I., Lancaster, T., Steele, A. J., Blundell, S. J., Pratt, F. L., Baker, P. J., McDonald, R. D., Sengupta, P., Singleton, J., Goddard, P. A., Lee, C., Whangbo, M.-H., Warter, M. M., Mielke, C. H. & Stephens, P. W. (2009). J. Am. Chem. Soc. 131, 4590–4591. [DOI] [PubMed]
  11. Oxford Diffraction (2009). CrysAlis PRO Oxford Diffraction Ltd, Yarnton, England.
  12. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  13. Singh, A., Sharma, R. P., Ferretti, V., Rossetti, S. & Venugopalan, P. (2009). J. Mol. Struct. 927, 111–120.
  14. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
  15. Youngme, S., Phatchimkun, J., Wannarit, N., Chaichit, N., Meejoo, S., van Albada, G. A. & Reedijk, J. (2008). Polyhedron, 27, 304–318.
  16. Youngme, S., Wannarit, N., Pakawatchai, C., Chaichit, N., Somsook, E., Turpeinen, U. & Mutikainen, I. (2007). Polyhedron, 26, 1459–1468.

Associated Data

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

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812050775/br2216sup1.cif

e-69-00m63-sup1.cif (48KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812050775/br2216Isup2.hkl

e-69-00m63-Isup2.hkl (492.4KB, hkl)

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


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