Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 May 31;68(Pt 6):o1931–o1932. doi: 10.1107/S1600536812023318

3,4,7,8-Tetra­methyl-1,10-phenanthrolin-1-ium nitrate monohydrate

Ke-Jie Zhang a,*, Yan-Fang Zhang b
PMCID: PMC3379486  PMID: 22719684

Abstract

In the crystal of the title compound, C16H17N2 +·NO3 ·H2O, the tetra­methyl-1,10-phenanthrolinium cations, nitrate anions and lattice water mol­ecules are all located on a mirror plane with the methyl H atoms of the cation equally disordered over two sites about the mirror plane. The cation, anion and water mol­ecule are linked by O—H⋯O and N—H⋯O hydrogen bonds into a sheet parallel to the bc plane. π–π stacking between phenanthroline ring systems is observed in the crystal structure, the centroid–centroid distance being 3.4745 (6) Å.

Related literature  

For proton-transfer structures of phenanthroline and its derivatives, see: Bei et al. (2004); Buttery et al. (2006); Gillard et al. (1998); Harvey et al. (2008); Hensen et al. (1998, 2000); Kolev et al. (2009); Lin et al. (2009); Maresca et al. (1989); Milani et al. (1997); Montagu-Bourin et al. (1981); Shang et al. (2006); Thevenet & Rodier (1978); Thevenet et al. (1977, 1978, 1980); Wang et al. (1999); Yu et al. (2006).graphic file with name e-68-o1931-scheme1.jpg

Experimental  

Crystal data  

  • C16H17N2 +·NO3 ·H2O

  • M r = 317.34

  • Orthorhombic, Inline graphic

  • a = 6.7401 (8) Å

  • b = 24.090 (3) Å

  • c = 19.254 (2) Å

  • V = 3126.1 (6) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.10 mm−1

  • T = 296 K

  • 0.37 × 0.30 × 0.21 mm

Data collection  

  • Bruker SMART 1000 CCD area-detector diffractometer

  • 11308 measured reflections

  • 1585 independent reflections

  • 1149 reflections with I > 2σ(I)

  • R int = 0.029

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.052

  • wR(F 2) = 0.153

  • S = 1.03

  • 1585 reflections

  • 143 parameters

  • H-atom parameters constrained

  • Δρmax = 0.22 e Å−3

  • Δρmin = −0.27 e Å−3

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812023318/xu5537sup1.cif

e-68-o1931-sup1.cif (24.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812023318/xu5537Isup2.hkl

e-68-o1931-Isup2.hkl (78.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812023318/xu5537Isup3.cml

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
N2—H2⋯O4i 0.86 1.86 2.692 (3) 164
O4—H1W⋯O1ii 0.84 1.97 2.808 (4) 174
O4—H2W⋯O1iii 0.83 2.07 2.886 (4) 170

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

Acknowledgments

Financial support from the National Natural Science Foundation of Henan Educational Committee, China (2011 C550002) is gratefully acknowledged.

supplementary crystallographic information

Comment

1,10-Phenanthroline and its derivatives have been recognized as good proton acceptors, and usually are considered a suitable agent in the synthesis of proton-transfer systems. Some proton-transfer complexes based on 1,10-phenanthroline (Buttery et al. 2006; Gillard et al. 1998; Hensen et al. 1998, 2000; Kolev et al. 2009; Maresca et al. 1989; Milani et al. 1997; Montagu-Bourin, Levillain, Ceolin, Thevenet & Souleau 1981; Shang et al. 2006; Thevenet & Rodier 1978; Thevenet et al. 1977, 1980; Thevenet, Rodier & Khodadad 1978; Wang et al. 1999), 2,9-dimethyl-1,10-phenanthroline (Harvey et al. 2008; Yu et al. 2006), and 6-nitro-1,10-phenanthroline (Bei et al. 2004), 5,6-dihydroxy-phenanthroline (Lin et al. 2009) have been synthesized. In the recent work, the title compound (I), C16H17N2]NO3.H2O, was obtained unintentionally as a major product in the reaction of Tb(NO3)3.6H2O with the 3,4,7,8-tetramethyl-1,10-phenanthroline in water. To the best our knowledge, this is the first example of proton-transfer system containing 3,4,7,8-tetramethyl-1,10- 1,10-phenanthroline.

The numbering scheme of (I) is given in Fig. 1, and the selected bond lengths and bond angles are provided in the cif file. The crystal contains one protonated 3,4,7,8-tetramethyl-1,10- 1,10-phenanthroline cation, one nitrate anion and one water molecule. In the crystal structure, the cations, anions and water molecules are linked into two dimensional layers parallel to the bc plane by N—H···O and O—H···O hydrogen bonds (Table 1). Among them, N—H···O hydrogen bonds play a very important role in the formation of proton-transfer compounds. Additionally, the monoprotonated 3,4,7,8-tetramethyl-1,10- 1,10-phenanthroline cations are parallel to each other in the crystal packing, showing π-π interactions (Fig. 2); the centroid–centroid distance is 3.4745 (6) Å.

Experimental

A aqueous solution (12 ml) of Tb(NO3)3.6H2O (1 mmol) and 3,4,7,8-tetramethyl-1,10-phenanthroline (1 mmol) was stirred. The mixture was then transferred to a 25-ml Teflon reactor and kept at 433 K for 3 d under autogenous pressure, and then cooled to room temperature at a rate of 10 K h-1. Colorless crystals of the title compound were obtained.

Refinement

The carbon-bound H atoms were placed in calculated positions and were included in the refinement in the riding model approximation, with C—H = 0.93 Å, Uiso(H) = 1.2Ueq(C aromatic) and C—H = 0.96 Å, Uiso(H) = 1.5Ueq(C methyl), respectively. The H atoms bound to O were located in a difference Fourier map, and refined as riding in their as-found relative positions with Uiso(H) = 1.5Ueq(O). The methyl H atoms are equally disordered over two sites about the mirror plane.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, with atom labels and 30% probability displacement ellipsoids for non-H atoms.

Fig. 2.

Fig. 2.

π-π interactions between the neighboring aromatic rings of the title compound. Aromatic hydrogen atoms and methyl groups have been omitted for clarity.

Crystal data

C16H17N2+·NO3·H2O F(000) = 1344
Mr = 317.34 Dx = 1.349 Mg m3
Orthorhombic, Cmca Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2bc 2 Cell parameters from 2972 reflections
a = 6.7401 (8) Å θ = 2.7–25.0°
b = 24.090 (3) Å µ = 0.10 mm1
c = 19.254 (2) Å T = 296 K
V = 3126.1 (6) Å3 Block, colorless
Z = 8 0.37 × 0.30 × 0.21 mm

Data collection

Bruker SMART 1000 CCD area-detector diffractometer 1149 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.029
Graphite monochromator θmax = 25.5°, θmin = 2.7°
φ and ω scans h = −8→7
11308 measured reflections k = −28→28
1585 independent reflections l = −23→23

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)] = 0.052 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.153 H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0707P)2 + 2.7655P] where P = (Fo2 + 2Fc2)/3
1585 reflections (Δ/σ)max < 0.001
143 parameters Δρmax = 0.22 e Å3
0 restraints Δρmin = −0.27 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 Occ. (<1)
C1 1.0000 0.19047 (14) 0.08694 (15) 0.0642 (9)
H1 1.0000 0.1825 0.0397 0.077*
C2 1.0000 0.24624 (14) 0.10669 (16) 0.0618 (8)
C3 1.0000 0.25954 (12) 0.17669 (16) 0.0550 (8)
C4 1.0000 0.21518 (11) 0.22551 (14) 0.0474 (7)
C5 1.0000 0.22191 (12) 0.29933 (15) 0.0517 (7)
H5 1.0000 0.2576 0.3177 0.062*
C6 1.0000 0.17823 (11) 0.34314 (14) 0.0520 (7)
H6 1.0000 0.1847 0.3908 0.062*
C7 1.0000 0.12218 (11) 0.31849 (13) 0.0485 (7)
C8 1.0000 0.07458 (12) 0.36186 (14) 0.0561 (8)
C9 1.0000 0.02213 (12) 0.33180 (16) 0.0635 (9)
C10 1.0000 0.01823 (12) 0.26008 (17) 0.0660 (9)
H10 1.0000 −0.0168 0.2396 0.079*
C11 1.0000 0.11486 (10) 0.24627 (14) 0.0483 (7)
C12 1.0000 0.16081 (12) 0.19900 (13) 0.0485 (7)
C13 1.0000 0.29005 (16) 0.05051 (19) 0.0890 (12)
H13A 1.0207 0.2728 0.0062 0.134* 0.50
H13B 1.1046 0.3162 0.0592 0.134* 0.50
H13C 0.8747 0.3090 0.0505 0.134* 0.50
C14 1.0000 0.31938 (13) 0.1996 (2) 0.0764 (10)
H14A 0.8712 0.3352 0.1918 0.115* 0.50
H14B 1.0972 0.3397 0.1734 0.115* 0.50
H14C 1.0316 0.3214 0.2481 0.115* 0.50
C15 1.0000 0.08170 (15) 0.43955 (15) 0.0770 (11)
H15A 0.9482 0.0488 0.4610 0.116* 0.50
H15B 0.9186 0.1129 0.4518 0.116* 0.50
H15C 1.1332 0.0880 0.4554 0.116* 0.50
C16 1.0000 −0.03134 (13) 0.3737 (2) 0.0912 (13)
H16A 1.0869 −0.0274 0.4129 0.137* 0.50
H16B 1.0453 −0.0614 0.3450 0.137* 0.50
H16C 0.8679 −0.0390 0.3896 0.137* 0.50
N1 1.0000 0.14820 (10) 0.13060 (11) 0.0570 (7)
N2 1.0000 0.06277 (9) 0.21952 (11) 0.0574 (7)
H2 1.0000 0.0585 0.1752 0.069*
N3 0.5000 0.38702 (12) 0.09781 (14) 0.0702 (8)
O1 0.5000 0.41620 (12) 0.04627 (14) 0.1338 (15)
O2 0.5000 0.40810 (14) 0.15514 (15) 0.1348 (15)
O3 0.5000 0.33707 (11) 0.09262 (15) 0.1115 (11)
O4 0.0000 0.02821 (10) 0.08654 (12) 0.1174 (13)
H2W 0.0000 0.0477 0.0512 0.176*
H1W 0.0000 −0.0058 0.0779 0.176*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.080 (2) 0.077 (2) 0.0361 (15) 0.000 0.000 0.0103 (14)
C2 0.066 (2) 0.067 (2) 0.0532 (18) 0.000 0.000 0.0177 (15)
C3 0.0574 (18) 0.0486 (16) 0.0589 (18) 0.000 0.000 0.0098 (13)
C4 0.0515 (16) 0.0464 (15) 0.0444 (15) 0.000 0.000 0.0003 (11)
C5 0.0607 (18) 0.0442 (15) 0.0501 (16) 0.000 0.000 −0.0088 (12)
C6 0.0679 (19) 0.0516 (16) 0.0365 (14) 0.000 0.000 −0.0074 (12)
C7 0.0616 (18) 0.0480 (15) 0.0360 (13) 0.000 0.000 −0.0022 (11)
C8 0.078 (2) 0.0541 (17) 0.0366 (14) 0.000 0.000 0.0036 (12)
C9 0.093 (2) 0.0498 (17) 0.0477 (17) 0.000 0.000 0.0039 (13)
C10 0.101 (3) 0.0448 (16) 0.0521 (18) 0.000 0.000 −0.0060 (13)
C11 0.0632 (18) 0.0475 (15) 0.0343 (13) 0.000 0.000 −0.0024 (11)
C12 0.0574 (17) 0.0528 (16) 0.0354 (13) 0.000 0.000 0.0007 (11)
C13 0.110 (3) 0.091 (3) 0.067 (2) 0.000 0.000 0.036 (2)
C14 0.091 (3) 0.055 (2) 0.083 (2) 0.000 0.000 0.0130 (17)
C15 0.125 (3) 0.070 (2) 0.0363 (15) 0.000 0.000 0.0060 (14)
C16 0.149 (4) 0.053 (2) 0.072 (2) 0.000 0.000 0.0145 (17)
N1 0.0772 (17) 0.0600 (14) 0.0338 (11) 0.000 0.000 0.0002 (10)
N2 0.0918 (19) 0.0467 (13) 0.0336 (11) 0.000 0.000 −0.0057 (10)
N3 0.095 (2) 0.0645 (18) 0.0508 (16) 0.000 0.000 −0.0033 (13)
O1 0.259 (5) 0.0823 (19) 0.0605 (16) 0.000 0.000 0.0153 (15)
O2 0.233 (4) 0.104 (2) 0.0669 (18) 0.000 0.000 −0.0228 (17)
O3 0.178 (3) 0.0621 (17) 0.095 (2) 0.000 0.000 0.0016 (15)
O4 0.238 (4) 0.0661 (15) 0.0483 (14) 0.000 0.000 −0.0128 (11)

Geometric parameters (Å, º)

C1—N1 1.320 (4) C11—N2 1.356 (3)
C1—C2 1.396 (5) C11—C12 1.433 (4)
C1—H1 0.9300 C12—N1 1.351 (3)
C2—C3 1.385 (4) C13—H13A 0.9600
C2—C13 1.511 (4) C13—H13B 0.9600
C3—C4 1.423 (4) C13—H13C 0.9600
C3—C14 1.508 (4) C14—H14A 0.9600
C4—C12 1.406 (4) C14—H14B 0.9600
C4—C5 1.431 (4) C14—H14C 0.9600
C5—C6 1.349 (4) C15—H15A 0.9600
C5—H5 0.9300 C15—H15B 0.9600
C6—C7 1.431 (4) C15—H15C 0.9600
C6—H6 0.9300 C16—H16A 0.9600
C7—C11 1.402 (4) C16—H16B 0.9600
C7—C8 1.419 (4) C16—H16C 0.9600
C8—C9 1.390 (4) N2—H2 0.8600
C8—C15 1.506 (4) N3—O3 1.208 (4)
C9—C10 1.384 (5) N3—O2 1.215 (4)
C9—C16 1.520 (4) N3—O1 1.216 (4)
C10—N2 1.327 (4) O4—H2W 0.8276
C10—H10 0.9300 O4—H1W 0.8365
N1—C1—C2 124.7 (3) N1—C12—C11 116.4 (2)
N1—C1—H1 117.7 C4—C12—C11 119.3 (2)
C2—C1—H1 117.7 C2—C13—H13A 109.5
C3—C2—C1 119.2 (3) C2—C13—H13B 109.5
C3—C2—C13 122.3 (3) H13A—C13—H13B 109.5
C1—C2—C13 118.5 (3) C2—C13—H13C 109.5
C2—C3—C4 118.0 (3) H13A—C13—H13C 109.5
C2—C3—C14 120.4 (3) H13B—C13—H13C 109.5
C4—C3—C14 121.7 (3) C3—C14—H14A 109.5
C12—C4—C3 117.4 (2) C3—C14—H14B 109.5
C12—C4—C5 117.8 (2) H14A—C14—H14B 109.5
C3—C4—C5 124.8 (3) C3—C14—H14C 109.5
C6—C5—C4 122.2 (3) H14A—C14—H14C 109.5
C6—C5—H5 118.9 H14B—C14—H14C 109.5
C4—C5—H5 118.9 C8—C15—H15A 109.5
C5—C6—C7 121.9 (2) C8—C15—H15B 109.5
C5—C6—H6 119.0 H15A—C15—H15B 109.5
C7—C6—H6 119.0 C8—C15—H15C 109.5
C11—C7—C8 118.8 (2) H15A—C15—H15C 109.5
C11—C7—C6 116.6 (2) H15B—C15—H15C 109.5
C8—C7—C6 124.6 (2) C9—C16—H16A 109.5
C9—C8—C7 119.3 (2) C9—C16—H16B 109.5
C9—C8—C15 121.2 (3) H16A—C16—H16B 109.5
C7—C8—C15 119.5 (3) C9—C16—H16C 109.5
C10—C9—C8 118.5 (3) H16A—C16—H16C 109.5
C10—C9—C16 118.2 (3) H16B—C16—H16C 109.5
C8—C9—C16 123.3 (3) C1—N1—C12 116.5 (3)
N2—C10—C9 122.2 (3) C10—N2—C11 121.6 (2)
N2—C10—H10 118.9 C10—N2—H2 119.2
C9—C10—H10 118.9 C11—N2—H2 119.2
N2—C11—C7 119.5 (2) O3—N3—O2 119.4 (3)
N2—C11—C12 118.3 (2) O3—N3—O1 120.6 (3)
C7—C11—C12 122.2 (2) O2—N3—O1 120.0 (3)
N1—C12—C4 124.3 (2) H2W—O4—H1W 113.2
N1—C1—C2—C3 0.0 C15—C8—C9—C16 0.0
N1—C1—C2—C13 180.0 C8—C9—C10—N2 0.0
C1—C2—C3—C4 0.0 C16—C9—C10—N2 180.0
C13—C2—C3—C4 180.0 C8—C7—C11—N2 0.0
C1—C2—C3—C14 180.0 C6—C7—C11—N2 180.0
C13—C2—C3—C14 0.0 C8—C7—C11—C12 180.0
C2—C3—C4—C12 0.0 C6—C7—C11—C12 0.0
C14—C3—C4—C12 180.0 C3—C4—C12—N1 0.0
C2—C3—C4—C5 180.0 C5—C4—C12—N1 180.0
C14—C3—C4—C5 0.0 C3—C4—C12—C11 180.0
C12—C4—C5—C6 0.0 C5—C4—C12—C11 0.0
C3—C4—C5—C6 180.0 N2—C11—C12—N1 0.0
C4—C5—C6—C7 0.0 C7—C11—C12—N1 180.0
C5—C6—C7—C11 0.0 N2—C11—C12—C4 180.0
C5—C6—C7—C8 180.0 C7—C11—C12—C4 0.0
C11—C7—C8—C9 0.0 C2—C1—N1—C12 0.0
C6—C7—C8—C9 180.0 C4—C12—N1—C1 0.0
C11—C7—C8—C15 180.0 C11—C12—N1—C1 180.0
C6—C7—C8—C15 0.0 C9—C10—N2—C11 0.0
C7—C8—C9—C10 0.0 C7—C11—N2—C10 0.0
C15—C8—C9—C10 180.0 C12—C11—N2—C10 180.0
C7—C8—C9—C16 180.0

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N2—H2···O4i 0.86 1.86 2.692 (3) 164
O4—H1W···O1ii 0.84 1.97 2.808 (4) 174
O4—H2W···O1iii 0.83 2.07 2.886 (4) 170

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5537).

References

  1. Bei, F.-L., Yang, X.-J., Lu, L.-D. & Wang, X. (2004). J. Mol. Struct. 689, 237–243.
  2. Bruker (1997). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Buttery, J. H., Effendy, Junk, P. C., Mutrofin, S.,Skelton, B. W., Whitaker, C. R., White, A. H. (2006). Z. Anorg. Allg. Chem. 632, 1326–1339.
  4. Gillard, R. D., Hursthouse, M. B., Abdul Malik, K. M. & Paisey, S. (1998). J. Chem. Crystallogr. 28, 611–619.
  5. Harvey, M. A., Baggio, S., Garland, M. T. & Baggio, R. (2008). Acta Cryst. C64, o489–o492. [DOI] [PubMed]
  6. Hensen, K., Gebhardt, F. & Bolte, M. (1998). Acta Cryst. C54, 359–361.
  7. Hensen, K., Spangenberg, B. & Bolte, M. (2000). Acta Cryst. C56, 208–210. [DOI] [PubMed]
  8. Kolev, T., Koleva, B. B., Nikolova, R., Seidel, R. W., Mayer-Figge, H., Spiteller, M. & Sheldrick, W. S. (2009). Spectrochim. Acta Part A, 73, 929–935. [DOI] [PubMed]
  9. Lin, X.-Y., Tang, S.-J. & Wu, W.-S. (2009). Acta Cryst. E65, o2367. [DOI] [PMC free article] [PubMed]
  10. Maresca, L., Natile, G. & Fanizzi, F. P. (1989). J. Am. Chem. Soc. 111, 1492–1493.
  11. Milani, B., Anzilutti, A., Vicentini, L., Santi, A. S., o Zangrando, E., Geremia, S. & Mestroni, G. (1997). Organometallics, 16, 5064–5075.
  12. Montagu-Bourin, M., Levillain, P., Ceolin, R., Thevenet, G. & Souleau, C. (1981). J. Appl. Cryst. 14, 63.
  13. Shang, R.-L., Du, L. & Sun, B.-W. (2006). Acta Cryst. E62, o2920–o2921.
  14. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  15. Thevenet, G. & Rodier, N. (1978). Acta Cryst. B34, 880–882.
  16. Thevenet, G., Rodier, N. & Khodadad, P. (1978). Acta Cryst. B34, 2594–2599.
  17. Thevenet, G., Souleau, C., Montagu-Bourin, M. & Ceolin, R. (1980). J. Appl. Cryst. 13, 315.
  18. Thevenet, G., Toffoli, P., Rodier, N. & Céolin, R. (1977). Acta Cryst. B33, 2526–2529.
  19. Wang, Y.-Q., Wang, Z.-M., Liao, C.-S. & Yan, C.-H. (1999). Acta Cryst. C55, 1503–1506.
  20. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
  21. Yu, Y.-Q., Ding, C.-F., Zhang, M.-L., Li, X.-M. & Zhang, S.-S. (2006). Acta Cryst. E62, o2187–o2189.

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/S1600536812023318/xu5537sup1.cif

e-68-o1931-sup1.cif (24.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812023318/xu5537Isup2.hkl

e-68-o1931-Isup2.hkl (78.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812023318/xu5537Isup3.cml

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