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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Mar 26;67(Pt 4):o984. doi: 10.1107/S1600536811010865

Ammonium 2-amino­pyrazine-3-carboxyl­ate

Martin Lutz a,*, Arjen J Jakobi a
PMCID: PMC3099982  PMID: 21754242

Abstract

The title compound NH4 +·C5H4N3O2 crystallizes with two formula units in the asymmetric unit. In each anion, the carboxyl­ate is deprotonated and the planar amino group [angle sums of 359 (3) and 355 (3)° at N] remains protonated. In the crystal, the cations and anions are bridged by N—H⋯O and N—H⋯N hydrogen bonds, forming a three-dimensional network.

Related literature

For the crystal structure of the free acid, see: Dobson & Gerkin (1996); Ptasiewicz-Bak & Leciejewicz (1997). For the metal complex with nickel, see: Ptasiewicz-Bak & Leciejewicz (1999). For the coordination chemistry of 2-pyrazine­carb­oxy­lic acid, see: Ptasiewicz-Bak et al. (1995); Ellsworth & zur Loye (2008). In the present study a half-normal probability plot (Abrahams & Keve, 1971), a quaternion fit (Mackay, 1984) and rigid-body analysis (Schomaker & Trueblood, 1998) have been used.graphic file with name e-67-0o984-scheme1.jpg

Experimental

Crystal data

  • NH4 +·C5H4N3O2

  • M r = 156.15

  • Orthorhombic, Inline graphic

  • a = 12.5066 (6) Å

  • b = 3.8833 (2) Å

  • c = 27.9659 (14) Å

  • V = 1358.22 (12) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.12 mm−1

  • T = 150 K

  • 0.40 × 0.19 × 0.09 mm

Data collection

  • Bruker Kappa APEXII diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2008a ) T min = 0.70, T max = 0.75

  • 16898 measured reflections

  • 1580 independent reflections

  • 1540 reflections with I > 2σ(I)

  • R int = 0.018

Refinement

  • R[F 2 > 2σ(F 2)] = 0.026

  • wR(F 2) = 0.072

  • S = 1.05

  • 1580 reflections

  • 247 parameters

  • 1 restraint

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

  • Δρmax = 0.33 e Å−3

  • Δρmin = −0.16 e Å−3

Data collection: APEX2 (Bruker, 2010); cell refinement: SAINT (Bruker, 2010); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008b ); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008b ); molecular graphics: PLATON (Spek, 2009) and Mercury (Macrae et al., 2006); software used to prepare material for publication: manual editing of SHELXL cif file.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811010865/zl2357sup1.cif

e-67-0o984-sup1.cif (18.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010865/zl2357Isup2.hkl

e-67-0o984-Isup2.hkl (77.9KB, 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
N31—H31A⋯N22i 0.92 (3) 2.20 (3) 3.103 (2) 169 (2)
N31—H31B⋯O21 0.90 (3) 2.07 (3) 2.726 (2) 129 (2)
N32—H32A⋯N21ii 0.88 (3) 2.23 (3) 3.100 (2) 168 (2)
N32—H32B⋯O22 0.86 (3) 2.06 (3) 2.686 (2) 129 (2)
N3—H3B⋯O21 0.93 (3) 1.97 (3) 2.849 (2) 157 (2)
N3—H3C⋯O11iii 0.96 (3) 2.58 (3) 3.287 (2) 131 (2)
N3—H3C⋯N11iii 0.96 (3) 2.00 (3) 2.909 (2) 159 (2)
N3—H3D⋯O11iv 0.89 (3) 2.13 (3) 2.944 (2) 152 (2)
N4—H4A⋯O12 0.86 (3) 2.13 (3) 2.897 (2) 148 (3)
N4—H4A⋯N12 0.86 (3) 2.23 (3) 2.912 (2) 135 (3)
N4—H4B⋯O11 0.95 (4) 1.86 (4) 2.793 (2) 166 (3)
N4—H4C⋯O11v 0.84 (3) 2.01 (4) 2.839 (2) 170 (3)
N4—H4D⋯O22vi 0.87 (3) 1.87 (3) 2.742 (2) 176 (3)

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

supplementary crystallographic information

Comment

2-Pyrazinecarboxylic acid is a complexation reagent in transition metal chemistry (Ptasiewicz-Bak et al., 1995) with a large variety of coordination modes (Ellsworth & zur Loye, 2008). The corresponding 3-aminopyrazine-2-carboxylic has been used in a similar way for the complexation of nickel (Ptasiewicz-Bak & Leciejewicz, 1999). The crystal structure of the free acid has been determined by Dobson & Gerkin (1996) and Ptasiewicz-Bak & Leciejewicz (1997).

The asymmetric unit of the crystal structure of the title compound (I) consists of two formula units (Z' = 2). The anions are essentially planar with a maximal deviation from the least-squares plane of 0.059 (2) and 0.093 (1) Å for the two molecules, respectively (Fig. 1). The molecular planes form angles of 5.54 (3) and 0.58 (3)° with the c axis. Also the amino moieties are planar with angle sums of 359 (3) and 355 (3)° at N31 and N32.

The two independent molecules are very similar, as can be seen in a quaternion fit (Fig. 2). This allows the generation of a half-normal probability plot (Fig. 3). The largest differences between the two molecules are in the C–O distances (Δ = 3.5σ). A possible explanation is the different hydrogen bonding situation of the four O atoms. If the anions in (I) are compared with the neutral molecule of the free acid (Dobson & Gerkin, 1996) the geometries are again very similar. As expected, the only difference is in the carboxylate, which is deprotonated in (I) and protonated in the free acid. The distances C51–O11 and C52–O12 in (I) are 1.266 (2) and 1.256 (2)Å compared to the C–OH distance of 1.328 (2)Å in the free acid. This is accompanied by a change of the corresponding C–C–O angles, which are 116.01 (14) and 116.79 (14)° in (I) compared to 118.20 (10)° in the free acid.

The two independent molecules in (I) can be modelled by rigid body model using the program THMA11 (Schomaker & Trueblood, 1998). The fit of this TLS model is good, as indicated by R-values (R={[Σ(wΔU)2]/[Σ(wUobs)2]}1/2) of 0.080 and 0.085 for the two molecules. The two molecules can thus be appropriately described as rigid bodies. The T tensor has eigenvalues of 0.01925, 0.01329, and 0.01076 Å2 for the first independent molecule in (I), and 0.02060, 0.01368, and 0.01227 Å2 for the second molecule. The L tensor has eigenvalues of 13.62, 6.42, and 4.28 deg.2 for the first molecule, and 12.96, 7.20, and 4.22 deg.2 for the second molecule.

The amino moieties of the anions act as donors of two hydrogen bonds, respecively. One is intramolecular to the carboxylate [graph set S11(6)], and one is intermolecular to a pyrazine N atom [graph set D11(2)]. Overall, this results in one-dimensional hydrogen-bonded chains along the b axis. These chains are interconnected by the ammonium cations to form a three-dimensional network. Hydrogen atoms H3C and H4A of the ammonium cations are involved in bifurcated hydrogen bonds (Table 1, Fig. 4).

Experimental

212 mg of 2-aminopyrazine-3-carboxylic acid were suspended in 20 ml water. A concentrated solution of ammonium hydroxide was added dropwise until the suspension became clear. Slow evaporation at room temperature gave crystals of (I) suitable for the diffraction experiment.

Refinement

During the intensity integration, a small second crystal fragment has been ignored (less than 5% occupancy). Friedel pairs have been averaged prior to the refinement.

Hydrogen atoms were located in difference Fourier maps. N—H hydrogen atoms were refined freely with isotropic displacement parameters. C—H hydrogen atoms were refined using a riding model with C—H = 0.95 Å and with Uiso(H) = 1.2 times Ueq(C).

Figures

Fig. 1.

Fig. 1.

: Displacement ellipsoid plot of (I). View along the b axis. Non-hydrogen atoms are drawn at the 50% probability level; H atoms are drawn as spheres with arbitrary radii.

Fig. 2.

Fig. 2.

: Quaternion fit (Mackay, 1984) of the two independent anions in (I). One of the molecules is inverted. The r.m.s. deviation of the fit is 0.041 Å.

Fig. 3.

Fig. 3.

: Half-normal probability plot (Abrahams & Keve, 1971) of the bond lengths of the two independent molecules of (I). On the vertical axis are the experimental Δ/σ data, on the horizontal axis the theoretical expectation values. Linear regression results in a slope of 2.2 and an intercept of 0.08.

Fig. 4.

Fig. 4.

: Hydrogen bonding interactions in the crystal structure of (I). View along the b axis.

Crystal data

NH4+·C5H4N3O2 F(000) = 656
Mr = 156.15 Dx = 1.527 Mg m3
Orthorhombic, Pca21 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2c -2ac Cell parameters from 9416 reflections
a = 12.5066 (6) Å θ = 2.9–27.5°
b = 3.8833 (2) Å µ = 0.12 mm1
c = 27.9659 (14) Å T = 150 K
V = 1358.22 (12) Å3 Plate, colourless
Z = 8 0.40 × 0.19 × 0.09 mm

Data collection

Bruker Kappa APEXII diffractometer 1580 independent reflections
Radiation source: fine-focus sealed tube 1540 reflections with I > 2σ(I)
graphite Rint = 0.018
φ and ω scans θmax = 27.5°, θmin = 2.9°
Absorption correction: multi-scan (SADABS; Sheldrick, 2008a) h = −16→15
Tmin = 0.70, Tmax = 0.75 k = −4→5
16898 measured reflections l = −36→36

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)] = 0.026 Hydrogen site location: difference Fourier map
wR(F2) = 0.072 H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0562P)2 + 0.1369P] where P = (Fo2 + 2Fc2)/3
1580 reflections (Δ/σ)max = 0.001
247 parameters Δρmax = 0.33 e Å3
1 restraint Δρmin = −0.16 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
O11 0.42965 (10) 0.7629 (3) 0.54691 (4) 0.0224 (3)
O21 0.30439 (11) 0.9858 (4) 0.59468 (5) 0.0238 (3)
N11 0.55372 (12) 0.5954 (4) 0.62042 (5) 0.0188 (3)
N21 0.50221 (12) 0.7550 (4) 0.71454 (5) 0.0200 (3)
N31 0.34689 (13) 1.0186 (4) 0.69017 (5) 0.0224 (3)
H31A 0.338 (2) 1.088 (7) 0.7212 (11) 0.031 (6)*
H31B 0.304 (2) 1.100 (7) 0.6670 (10) 0.032 (7)*
C11 0.61962 (15) 0.5125 (5) 0.65636 (6) 0.0211 (3)
H11 0.6854 0.3996 0.6498 0.025*
C21 0.59216 (14) 0.5908 (5) 0.70302 (6) 0.0209 (3)
H21 0.6395 0.5246 0.7279 0.025*
C31 0.43627 (13) 0.8473 (4) 0.67848 (6) 0.0164 (3)
C41 0.46320 (13) 0.7604 (4) 0.63013 (6) 0.0156 (3)
C51 0.39253 (13) 0.8432 (4) 0.58752 (6) 0.0174 (3)
O12 0.14633 (10) 0.3689 (4) 0.46142 (4) 0.0245 (3)
O22 0.02147 (11) 0.5588 (4) 0.41050 (5) 0.0281 (3)
N12 0.26120 (11) 0.1003 (4) 0.39032 (5) 0.0188 (3)
N22 0.21177 (12) 0.2151 (4) 0.29449 (5) 0.0207 (3)
N32 0.05731 (12) 0.4997 (4) 0.31616 (6) 0.0232 (3)
H32A 0.0512 (19) 0.574 (6) 0.2864 (10) 0.026 (6)*
H32B 0.020 (2) 0.611 (7) 0.3371 (10) 0.035 (7)*
C12 0.32517 (14) −0.0150 (5) 0.35539 (7) 0.0211 (3)
H12 0.3883 −0.1386 0.3632 0.025*
C22 0.29979 (14) 0.0451 (5) 0.30788 (7) 0.0216 (4)
H22 0.3469 −0.0379 0.2838 0.026*
C32 0.14642 (13) 0.3310 (4) 0.32951 (6) 0.0175 (3)
C42 0.17362 (13) 0.2711 (4) 0.37884 (5) 0.0163 (3)
C52 0.10825 (13) 0.4099 (4) 0.42027 (6) 0.0189 (3)
N3 0.12272 (12) 0.8079 (4) 0.53838 (5) 0.0201 (3)
H3A 0.133 (2) 0.702 (7) 0.5094 (11) 0.032 (6)*
H3B 0.189 (2) 0.888 (7) 0.5486 (10) 0.032 (6)*
H3C 0.086 (2) 0.660 (7) 0.5602 (11) 0.037 (6)*
H3D 0.079 (2) 0.986 (7) 0.5356 (9) 0.034 (7)*
N4 0.37274 (14) 0.2716 (5) 0.47857 (6) 0.0249 (3)
H4A 0.312 (3) 0.249 (7) 0.4640 (11) 0.043 (8)*
H4B 0.380 (2) 0.443 (10) 0.5025 (14) 0.057 (9)*
H4C 0.388 (2) 0.102 (8) 0.4961 (12) 0.043 (8)*
H4D 0.420 (2) 0.315 (7) 0.4564 (10) 0.032 (6)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O11 0.0230 (6) 0.0326 (7) 0.0115 (5) −0.0014 (5) −0.0003 (4) 0.0001 (5)
O21 0.0174 (6) 0.0355 (7) 0.0184 (6) 0.0022 (5) −0.0026 (4) −0.0009 (5)
N11 0.0193 (7) 0.0201 (7) 0.0169 (7) 0.0002 (5) 0.0015 (5) 0.0005 (5)
N21 0.0234 (7) 0.0226 (7) 0.0140 (6) −0.0029 (6) −0.0012 (6) 0.0007 (5)
N31 0.0204 (7) 0.0308 (8) 0.0160 (7) 0.0036 (6) −0.0001 (5) −0.0042 (6)
C11 0.0186 (8) 0.0222 (8) 0.0225 (8) 0.0031 (6) −0.0017 (6) 0.0005 (6)
C21 0.0224 (8) 0.0214 (8) 0.0189 (8) −0.0019 (6) −0.0049 (6) 0.0019 (7)
C31 0.0190 (8) 0.0168 (7) 0.0133 (7) −0.0055 (6) −0.0001 (5) 0.0000 (6)
C41 0.0158 (7) 0.0179 (7) 0.0131 (7) −0.0029 (6) 0.0006 (6) 0.0006 (5)
C51 0.0178 (8) 0.0201 (7) 0.0145 (7) −0.0060 (6) −0.0006 (5) 0.0014 (6)
O12 0.0280 (6) 0.0322 (7) 0.0133 (5) 0.0041 (5) 0.0000 (5) −0.0021 (5)
O22 0.0226 (6) 0.0423 (8) 0.0193 (6) 0.0091 (6) 0.0021 (5) −0.0012 (6)
N12 0.0183 (6) 0.0220 (7) 0.0162 (6) −0.0019 (5) −0.0004 (5) −0.0018 (5)
N22 0.0234 (7) 0.0237 (7) 0.0151 (6) −0.0040 (6) 0.0019 (5) −0.0016 (5)
N32 0.0227 (7) 0.0325 (8) 0.0144 (7) 0.0024 (6) −0.0005 (6) 0.0043 (6)
C12 0.0190 (8) 0.0224 (9) 0.0220 (8) 0.0008 (6) 0.0014 (6) −0.0026 (7)
C22 0.0228 (8) 0.0217 (8) 0.0203 (8) −0.0029 (6) 0.0055 (6) −0.0050 (6)
C32 0.0187 (8) 0.0192 (7) 0.0146 (7) −0.0054 (6) −0.0004 (6) −0.0004 (6)
C42 0.0176 (7) 0.0187 (8) 0.0126 (7) −0.0032 (6) 0.0006 (6) −0.0012 (6)
C52 0.0198 (8) 0.0211 (8) 0.0158 (7) −0.0014 (6) 0.0025 (6) −0.0017 (6)
N3 0.0196 (7) 0.0230 (7) 0.0178 (7) −0.0004 (6) −0.0007 (5) −0.0002 (6)
N4 0.0227 (7) 0.0348 (9) 0.0174 (7) −0.0044 (6) −0.0042 (6) 0.0037 (7)

Geometric parameters (Å, °)

O11—C51 1.266 (2) N22—C22 1.337 (2)
O21—C51 1.250 (2) N22—C32 1.353 (2)
N11—C41 1.329 (2) N32—C32 1.346 (2)
N11—C11 1.339 (2) N32—H32A 0.88 (3)
N21—C21 1.333 (2) N32—H32B 0.86 (3)
N21—C31 1.351 (2) C12—C22 1.386 (3)
N31—C31 1.341 (2) C12—H12 0.9500
N31—H31A 0.92 (3) C22—H22 0.9500
N31—H31B 0.90 (3) C32—C42 1.440 (2)
C11—C21 1.383 (2) C42—C52 1.517 (2)
C11—H11 0.9500 N3—H3A 0.92 (3)
C21—H21 0.9500 N3—H3B 0.93 (3)
C31—C41 1.434 (2) N3—H3C 0.96 (3)
C41—C51 1.518 (2) N3—H3D 0.89 (3)
O12—C52 1.256 (2) N4—H4A 0.86 (3)
O22—C52 1.260 (2) N4—H4B 0.95 (4)
N12—C42 1.320 (2) N4—H4C 0.84 (3)
N12—C12 1.340 (2) N4—H4D 0.87 (3)
C41—N11—C11 119.14 (15) N12—C12—H12 119.8
C21—N21—C31 117.49 (15) C22—C12—H12 119.8
C31—N31—H31A 118.4 (17) N22—C22—C12 122.70 (16)
C31—N31—H31B 119.6 (17) N22—C22—H22 118.7
H31A—N31—H31B 121 (2) C12—C22—H22 118.7
N11—C11—C21 120.16 (16) N32—C32—N22 117.48 (15)
N11—C11—H11 119.9 N32—C32—C42 122.70 (16)
C21—C11—H11 119.9 N22—C32—C42 119.81 (15)
N21—C21—C11 122.88 (16) N12—C42—C32 120.68 (15)
N21—C21—H21 118.6 N12—C42—C52 116.10 (14)
C11—C21—H21 118.6 C32—C42—C52 123.17 (15)
N31—C31—N21 117.27 (15) O12—C52—O22 125.71 (15)
N31—C31—C41 122.85 (15) O12—C52—C42 116.79 (14)
N21—C31—C41 119.88 (15) O22—C52—C42 117.50 (15)
N11—C41—C31 120.42 (15) H3A—N3—H3B 107 (2)
N11—C41—C51 115.96 (14) H3A—N3—H3C 111 (2)
C31—C41—C51 123.62 (14) H3B—N3—H3C 116 (2)
O21—C51—O11 125.19 (15) H3A—N3—H3D 111 (2)
O21—C51—C41 118.80 (14) H3B—N3—H3D 108 (2)
O11—C51—C41 116.01 (14) H3C—N3—H3D 103 (2)
C42—N12—C12 119.08 (15) H4A—N4—H4B 119 (3)
C22—N22—C32 117.32 (15) H4A—N4—H4C 113 (3)
C32—N32—H32A 119.4 (16) H4B—N4—H4C 97 (3)
C32—N32—H32B 119.9 (18) H4A—N4—H4D 106 (3)
H32A—N32—H32B 116 (2) H4B—N4—H4D 107 (3)
N12—C12—C22 120.40 (16) H4C—N4—H4D 114 (3)
C41—N11—C11—C21 1.6 (3) C42—N12—C12—C22 0.1 (2)
C31—N21—C21—C11 −0.2 (3) C32—N22—C22—C12 0.2 (3)
N11—C11—C21—N21 −1.4 (3) N12—C12—C22—N22 −0.5 (3)
C21—N21—C31—N31 −178.70 (15) C22—N22—C32—N32 −179.47 (15)
C21—N21—C31—C41 1.5 (2) C22—N22—C32—C42 0.5 (2)
C11—N11—C41—C31 −0.2 (2) C12—N12—C42—C32 0.5 (2)
C11—N11—C41—C51 −179.62 (15) C12—N12—C42—C52 −176.88 (15)
N31—C31—C41—N11 178.87 (16) N32—C32—C42—N12 179.09 (15)
N21—C31—C41—N11 −1.3 (2) N22—C32—C42—N12 −0.8 (2)
N31—C31—C41—C51 −1.8 (2) N32—C32—C42—C52 −3.7 (2)
N21—C31—C41—C51 178.00 (15) N22—C32—C42—C52 176.38 (14)
N11—C41—C51—O21 177.16 (15) N12—C42—C52—O12 4.3 (2)
C31—C41—C51—O21 −2.2 (2) C32—C42—C52—O12 −173.05 (16)
N11—C41—C51—O11 −3.6 (2) N12—C42—C52—O22 −176.49 (15)
C31—C41—C51—O11 177.04 (15) C32—C42—C52—O22 6.2 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N31—H31A···N22i 0.92 (3) 2.20 (3) 3.103 (2) 169 (2)
N31—H31B···O21 0.90 (3) 2.07 (3) 2.726 (2) 129 (2)
N32—H32A···N21ii 0.88 (3) 2.23 (3) 3.100 (2) 168 (2)
N32—H32B···O22 0.86 (3) 2.06 (3) 2.686 (2) 129 (2)
N3—H3B···O21 0.93 (3) 1.97 (3) 2.849 (2) 157 (2)
N3—H3C···O11iii 0.96 (3) 2.58 (3) 3.287 (2) 131 (2)
N3—H3C···N11iii 0.96 (3) 2.00 (3) 2.909 (2) 159 (2)
N3—H3D···O11iv 0.89 (3) 2.13 (3) 2.944 (2) 152 (2)
N4—H4A···O12 0.86 (3) 2.13 (3) 2.897 (2) 148 (3)
N4—H4A···N12 0.86 (3) 2.23 (3) 2.912 (2) 135 (3)
N4—H4B···O11 0.95 (4) 1.86 (4) 2.793 (2) 166 (3)
N4—H4C···O11v 0.84 (3) 2.01 (4) 2.839 (2) 170 (3)
N4—H4D···O22vi 0.87 (3) 1.87 (3) 2.742 (2) 176 (3)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZL2357).

References

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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/S1600536811010865/zl2357sup1.cif

e-67-0o984-sup1.cif (18.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811010865/zl2357Isup2.hkl

e-67-0o984-Isup2.hkl (77.9KB, hkl)

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


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