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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Sep 14;67(Pt 10):m1362. doi: 10.1107/S1600536811035860

Bis(hydrogen l-glutamato)palladium(II)

Antje Seifert a, Christoph Wagner a, Kurt Merzweiler a,*
PMCID: PMC3201544  PMID: 22065700

Abstract

In the title compound, [Pd(C5H8NO4)2], the Pd(II) atom is coordinated by two O atoms and two N atoms of two N,O-chelating hydrogen l-glutatmate ligands in a square–planar geometry with the N and O atoms in a mutually trans arrangement. The complex units are embedded in a network of N—H⋯O and O—H⋯O hydrogen-bonding inter­actions that stabilize the three-dimensional crystal structure. The strongest hydrogen bonds are formed between the γ-COOH untis of adjacent glutamate ligands, leading to dimers of the type R 2 2(8) with O⋯O separations of 2.640 (6) Å.

Related literature

For the synthesis of the title compound, see: Spacu & Scherzer (1962). For the structures of related palladium complexes with amino acid ligands, see: Vagg (1979); Jarzab et al. (1973); Sabat et al. (1979); Pletnev et al. (1992); Hao et al. (2007); Gao et al. (2008).graphic file with name e-67-m1362-scheme1.jpg

Experimental

Crystal data

  • [Pd(C5H8NO4)2]

  • M r = 398.66

  • Triclinic, Inline graphic

  • a = 4.8858 (3) Å

  • b = 5.1605 (4) Å

  • c = 13.3651 (9) Å

  • α = 93.725 (6)°

  • β = 99.734 (6)°

  • γ = 104.245 (6)°

  • V = 319.90 (4) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 1.49 mm−1

  • T = 200 K

  • 0.17 × 0.06 × 0.04 mm

Data collection

  • Stoe IPDS 2T diffractometer

  • Absorption correction: integration (X-RED; Stoe & Cie, 2009) T min = 0.806, T max = 0.973

  • 4724 measured reflections

  • 2406 independent reflections

  • 2389 reflections with I > 2σ(I)

  • R int = 0.044

Refinement

  • R[F 2 > 2σ(F 2)] = 0.029

  • wR(F 2) = 0.066

  • S = 1.04

  • 2406 reflections

  • 208 parameters

  • 9 restraints

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

  • Δρmax = 0.37 e Å−3

  • Δρmin = −0.74 e Å−3

  • Absolute structure: Flack (1983), 1146 Friedel pairs

  • Flack parameter: −0.02 (4)

Data collection: X-AREA (Stoe & Cie, 2009); cell refinement: X-AREA; data reduction: X-RED (Stoe & Cie, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2009); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) I, publication_text. DOI: 10.1107/S1600536811035860/wm2526sup1.cif

e-67-m1362-sup1.cif (18.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811035860/wm2526Isup2.hkl

e-67-m1362-Isup2.hkl (118.2KB, hkl)

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

Table 1. Selected bond lengths (Å).

Pd—N1 2.072 (9)
Pd—N2 2.005 (11)
Pd—O1 1.976 (8)
Pd—O5 2.024 (7)

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

D—H⋯A D—H H⋯A DA D—H⋯A
N2—H9⋯O6i 0.85 (2) 2.15 (4) 2.979 (15) 162 (8)
N2—H10⋯O5ii 0.85 (2) 2.43 (8) 3.121 (13) 138 (10)
O7—H16⋯O4iii 0.85 (2) 1.80 (2) 2.639 (6) 169 (7)
O3—H8⋯O8iv 0.86 (2) 1.79 (3) 2.640 (6) 167 (7)
N1—H1⋯O2v 0.85 (2) 2.15 (3) 2.996 (15) 170 (9)
N1—H2⋯O1vi 0.85 (2) 2.30 (8) 2.998 (13) 139 (10)
N1—H2⋯O5vii 0.85 (2) 2.42 (7) 3.117 (13) 140 (10)

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

supplementary crystallographic information

Comment

The title compound, [Pd(C5H8NO4)2] (I), consists of a palladium(II) atom which is coordinated by two N and two O atoms of two chelating hydrogen glutamate ligands. The metal atom adopts a distorted square–planar coordination with the two N atoms and the two O atoms in mutual trans arrangements. The maximum deviation from the least squares plane through the atoms Pd, N1, N2, O1 and O5 is 0.026 Å for N2. The distances Pd—O (1.976 (8), 2.024 (7) Å) and Pd—N (2.005 (11), 2.072 (9) Å) are in agreement with the values observed for other Pd(II) amino acid derivatives, like cis-bis(L-tyrosinato)-palladium(II) hemihydrate (Jarzab et al., 1973), bis(L-tyrosinato)-palladium(II) (Sabat et al., 1979), bis(L-valinato)-palladium(II) monohydrate (Pletnev et al., 1992); Hao et al., 2007), cis-bis(L-aspartato-N,O)-palladium(II) (Gao et al., 2008) or bis(L-serinato)-palladium(II) (Vagg, 1979). For both the hydrogen glutatmate ligands, the five membered PdNC2O chelate rings adopt envelope conformations with a nearly coplanar arrangement of the Pd, O, C and N atoms at the flap positions.

The main conformational difference between both chelate rings arises from the orientation of the carboxyethyl groups. In the case of C2 the carboxyethyl group is in an axial position and for C7 an equatorially arrangend carboxyethyl group is observed (Fig. 1).

The packing of the complex units is supported by different types of hydrogen bonding interactions. The strongest hydrogen bridges are formed between the γ-carboxyl groups of neighbouring molecules. Consequently, R22(8) motifs are observed and the complex units are arranged in chains. Additionally, there are N—H···O hydrogen bridges of the type C11(4) and C11(5) which are formed between amino groups and oxygen atoms of adjacent α-carboxylate groups (Fig. 2)

Experimental

The title compound was prepared from K2PdCl4 and sodium hydrogen glutamate according to a procedure described by Spacu & Scherzer (1962). For the growth of single crystals, the reaction mixture was stored at 278 K for several weeks.

Refinement

C-bound H atoms of the hydrogen glutamate units were positioned geometrically and refinded using a riding model with Uiso(H) = 1.2 Ueq(C) [d(C—H) = 0.99 (for C–H) and 1.00 Å (for CH2)]. H atoms attached to N and O were located from difference fourier maps and refined with N—H distances fixed at 0.85 (2) Å (Uiso(H) = 1.2 Ueq(N)) and O—H distances fixed at 0.85 (2) and 0.86 (2) Å (Uiso(H) = 1.2 Ueq(O)).

Figures

Fig. 1.

Fig. 1.

Molecular structure of (I). Displacement ellipsoids are drawn at the 50% probabiltiy level.

Fig. 2.

Fig. 2.

Arrangement of the hydrogen bonds around the complex unit. [Symmetry operators: (i) x + 1, y + 1, z; (ii) x, y + 1, z; (iii) x - 1, y + 1, z + 1; (iv) x + 1, y - 1, z - 1; (v) x - 1, y - 1, z; (vi) x, y - 1, z; (vii) x + 1, y, z; (viii) x - 1, y, z.]

Crystal data

[Pd(C5H8NO4)2] Z = 1
Mr = 398.66 F(000) = 201
Triclinic, P1 Dx = 2.070 Mg m3
Hall symbol: P 1 Mo Kα radiation, λ = 0.71073 Å
a = 4.8858 (3) Å Cell parameters from 7673 reflections
b = 5.1605 (4) Å θ = 3.1–29.3°
c = 13.3651 (9) Å µ = 1.49 mm1
α = 93.725 (6)° T = 200 K
β = 99.734 (6)° Prism, yellow
γ = 104.245 (6)° 0.17 × 0.06 × 0.04 mm
V = 319.90 (4) Å3

Data collection

Stoe IPDS 2T diffractometer 2406 independent reflections
Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus 2389 reflections with I > 2σ(I)
plane graphite Rint = 0.044
Detector resolution: 6.67 pixels mm-1 θmax = 26.0°, θmin = 3.1°
ω–scans h = −6→6
Absorption correction: integration (X-RED; Stoe & Cie, 2009) k = −6→6
Tmin = 0.806, Tmax = 0.973 l = −16→16
4724 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.029 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.066 w = 1/[σ2(Fo2) + (0.0356P)2 + 0.1842P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max < 0.001
2406 reflections Δρmax = 0.37 e Å3
208 parameters Δρmin = −0.74 e Å3
9 restraints Absolute structure: Flack (1983), 1146 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: −0.02 (4)

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 0.649 (3) 0.240 (2) 0.7428 (9) 0.020 (3)
C2 0.478 (2) −0.043 (2) 0.7031 (8) 0.015 (2)
H3 0.6076 −0.1464 0.6791 0.017*
C3 0.2260 (11) −0.0501 (11) 0.6139 (4) 0.0219 (11)
H4 0.1138 −0.2395 0.5939 0.026*
H5 0.0971 0.0487 0.6394 0.026*
C4 0.3130 (13) 0.0694 (11) 0.5184 (4) 0.0234 (11)
H6 0.1410 0.1014 0.4755 0.028*
H7 0.4546 0.2460 0.5398 0.028*
C5 0.4388 (11) −0.1010 (11) 0.4554 (4) 0.0224 (11)
C6 −0.125 (2) 0.009 (2) 1.0111 (8) 0.018 (2)
C7 0.098 (2) 0.272 (2) 1.0603 (9) 0.019 (2)
H11 0.2662 0.2244 1.1017 0.023*
C8 −0.0210 (12) 0.4448 (10) 1.1299 (4) 0.0213 (11)
H12 −0.2096 0.4604 1.0938 0.026*
H13 0.1110 0.6279 1.1447 0.026*
C9 −0.0580 (13) 0.3289 (13) 1.2308 (4) 0.0249 (12)
H14 −0.1794 0.1414 1.2162 0.030*
H15 0.1325 0.3254 1.2694 0.030*
C10 −0.1944 (12) 0.4914 (11) 1.2950 (4) 0.0210 (11)
N1 0.345 (2) −0.179 (2) 0.7842 (7) 0.018 (2)
H2 0.464 (16) −0.25 (2) 0.820 (7) 0.022*
H1 0.196 (12) −0.311 (12) 0.767 (7) 0.022*
N2 0.194 (2) 0.405 (2) 0.9716 (8) 0.020 (2)
H10 0.054 (15) 0.46 (2) 0.944 (8) 0.024*
H9 0.346 (13) 0.526 (13) 0.999 (7) 0.024*
O1 0.5808 (17) 0.3460 (16) 0.8246 (6) 0.023 (2)
O2 0.8325 (17) 0.3614 (16) 0.6976 (6) 0.0259 (16)
O3 0.3977 (9) −0.0697 (8) 0.3575 (3) 0.0278 (8)
H8 0.503 (13) −0.150 (12) 0.328 (5) 0.033*
O4 0.5723 (10) −0.2598 (10) 0.4909 (3) 0.0289 (9)
O5 −0.0695 (16) −0.1097 (14) 0.9320 (6) 0.0206 (18)
O6 −0.3437 (17) −0.0908 (16) 1.0453 (6) 0.0237 (15)
O7 −0.1369 (9) 0.4718 (8) 1.3941 (3) 0.0267 (8)
H16 −0.220 (15) 0.553 (12) 1.432 (5) 0.032*
O8 −0.3538 (9) 0.6250 (9) 1.2573 (3) 0.0319 (9)
Pd 0.26234 (18) 0.11739 (15) 0.87796 (9) 0.01627 (10)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.021 (6) 0.011 (5) 0.029 (6) 0.004 (4) 0.005 (5) −0.001 (4)
C2 0.007 (4) 0.025 (4) 0.014 (4) 0.007 (3) 0.004 (3) 0.003 (3)
C3 0.017 (2) 0.026 (3) 0.023 (3) 0.007 (2) 0.003 (2) 0.000 (2)
C4 0.027 (3) 0.024 (3) 0.021 (3) 0.011 (2) 0.005 (2) 0.002 (2)
C5 0.017 (3) 0.025 (3) 0.022 (3) −0.001 (2) 0.004 (2) 0.001 (2)
C6 0.014 (5) 0.024 (6) 0.015 (5) 0.009 (5) −0.001 (4) 0.001 (4)
C7 0.012 (4) 0.016 (4) 0.027 (4) 0.000 (3) 0.002 (3) −0.003 (3)
C8 0.028 (3) 0.017 (2) 0.020 (3) 0.004 (2) 0.010 (2) −0.001 (2)
C9 0.027 (3) 0.027 (3) 0.023 (3) 0.009 (3) 0.008 (3) 0.001 (2)
C10 0.021 (3) 0.026 (3) 0.019 (3) 0.007 (2) 0.008 (2) 0.003 (2)
N1 0.020 (5) 0.016 (5) 0.018 (4) 0.004 (4) 0.006 (4) −0.009 (3)
N2 0.015 (5) 0.022 (5) 0.027 (5) 0.005 (4) 0.006 (4) 0.013 (4)
O1 0.028 (4) 0.023 (5) 0.019 (4) 0.010 (4) 0.003 (3) −0.006 (4)
O2 0.024 (3) 0.023 (3) 0.029 (3) −0.001 (2) 0.011 (2) −0.001 (2)
O3 0.037 (2) 0.033 (2) 0.0169 (18) 0.0129 (18) 0.0092 (16) 0.0034 (16)
O4 0.035 (3) 0.038 (3) 0.021 (2) 0.022 (2) 0.0092 (19) 0.003 (2)
O5 0.018 (4) 0.013 (4) 0.031 (4) 0.000 (3) 0.010 (3) 0.002 (3)
O6 0.021 (3) 0.024 (3) 0.026 (3) 0.003 (2) 0.007 (2) 0.004 (2)
O7 0.031 (2) 0.035 (2) 0.0165 (18) 0.0136 (18) 0.0065 (16) −0.0001 (16)
O8 0.035 (2) 0.048 (3) 0.020 (2) 0.023 (2) 0.0071 (17) 0.0018 (18)
Pd 0.01683 (17) 0.01537 (15) 0.01715 (16) 0.00487 (11) 0.00451 (11) −0.00026 (10)

Geometric parameters (Å, °)

C1—O2 1.231 (14) C7—H11 1.0000
C1—O1 1.318 (14) C8—C9 1.530 (7)
C1—C2 1.508 (17) C8—H12 0.9900
C2—N1 1.483 (16) C8—H13 0.9900
C2—C3 1.553 (11) C9—C10 1.503 (8)
C2—H3 1.0000 C9—H14 0.9900
C3—C4 1.532 (7) C9—H15 0.9900
C3—H4 0.9900 C10—O8 1.230 (7)
C3—H5 0.9900 C10—O7 1.323 (7)
C4—C5 1.485 (7) Pd—N1 2.072 (9)
C4—H6 0.9900 N1—H2 0.85 (2)
C4—H7 0.9900 N1—H1 0.85 (2)
C5—O4 1.238 (7) Pd—N2 2.005 (11)
C5—O3 1.316 (7) N2—H10 0.85 (2)
C6—O6 1.243 (14) N2—H9 0.85 (2)
C6—O5 1.289 (14) Pd—O1 1.976 (8)
C6—C7 1.538 (16) O3—H8 0.86 (2)
C7—N2 1.493 (16) O5—Pd 2.024 (7)
C7—C8 1.529 (12) O7—H16 0.85 (2)
O2—C1—O1 124.1 (11) C9—C8—H12 109.1
O2—C1—C2 120.1 (10) C7—C8—H13 109.1
O1—C1—C2 115.7 (11) C9—C8—H13 109.1
N1—C2—C1 110.6 (9) H12—C8—H13 107.8
N1—C2—C3 106.2 (8) C10—C9—C8 111.8 (5)
C1—C2—C3 111.7 (9) C10—C9—H14 109.3
N1—C2—H3 109.4 C8—C9—H14 109.3
C1—C2—H3 109.4 C10—C9—H15 109.3
C3—C2—H3 109.4 C8—C9—H15 109.3
C4—C3—C2 115.7 (5) H14—C9—H15 107.9
C4—C3—H4 108.4 O8—C10—O7 123.0 (5)
C2—C3—H4 108.4 O8—C10—C9 122.2 (5)
C4—C3—H5 108.4 O7—C10—C9 114.8 (5)
C2—C3—H5 108.4 C2—N1—Pd 106.8 (8)
H4—C3—H5 107.4 C2—N1—H2 110 (6)
C5—C4—C3 114.6 (4) Pd—N1—H2 108 (8)
C5—C4—H6 108.6 C2—N1—H1 119 (7)
C3—C4—H6 108.6 Pd—N1—H1 110 (7)
C5—C4—H7 108.6 H2—N1—H1 102 (9)
C3—C4—H7 108.6 C7—N2—Pd 106.3 (7)
H6—C4—H7 107.6 C7—N2—H10 105 (7)
O4—C5—O3 122.1 (5) Pd—N2—H10 111 (9)
O4—C5—C4 123.5 (5) C7—N2—H9 103 (7)
O3—C5—C4 114.5 (5) Pd—N2—H9 114 (8)
O6—C6—O5 120.4 (11) H10—N2—H9 115 (10)
O6—C6—C7 123.5 (10) C1—O1—Pd 116.3 (8)
O5—C6—C7 116.1 (10) C5—O3—H8 109 (5)
N2—C7—C8 114.0 (9) C6—O5—Pd 113.1 (8)
N2—C7—C6 104.2 (10) C10—O7—H16 117 (5)
C8—C7—C6 112.8 (8) O1—Pd—N2 97.7 (4)
N2—C7—H11 108.6 O1—Pd—O5 178.6 (4)
C8—C7—H11 108.6 N2—Pd—O5 81.3 (4)
C6—C7—H11 108.6 O1—Pd—N1 81.7 (4)
C7—C8—C9 112.6 (6) N2—Pd—N1 178.3 (6)
C7—C8—H12 109.1 O5—Pd—N1 99.3 (4)
O2—C1—C2—N1 161.2 (10) C8—C9—C10—O7 −155.6 (5)
O1—C1—C2—N1 −20.8 (13) C1—C2—N1—Pd 30.8 (10)
O2—C1—C2—C3 −80.7 (12) C3—C2—N1—Pd −90.6 (8)
O1—C1—C2—C3 97.3 (11) C8—C7—N2—Pd −168.6 (6)
N1—C2—C3—C4 −177.5 (6) C6—C7—N2—Pd −45.3 (9)
C1—C2—C3—C4 61.8 (10) O2—C1—O1—Pd 176.4 (9)
C2—C3—C4—C5 74.0 (8) C2—C1—O1—Pd −1.5 (12)
C3—C4—C5—O4 −28.6 (8) O6—C6—O5—Pd 171.2 (8)
C3—C4—C5—O3 151.5 (5) C7—C6—O5—Pd −10.6 (11)
O6—C6—C7—N2 −144.1 (10) C1—O1—Pd—N2 −166.0 (8)
O5—C6—C7—N2 37.8 (12) C1—O1—Pd—N1 15.7 (8)
O6—C6—C7—C8 −20.0 (15) C7—N2—Pd—O1 −147.4 (7)
O5—C6—C7—C8 161.8 (8) C7—N2—Pd—O5 33.7 (7)
N2—C7—C8—C9 −168.1 (8) C6—O5—Pd—N2 −13.5 (7)
C6—C7—C8—C9 73.4 (10) C6—O5—Pd—N1 164.8 (7)
C7—C8—C9—C10 −176.1 (6) C2—N1—Pd—O1 −25.3 (7)
C8—C9—C10—O8 26.5 (8) C2—N1—Pd—O5 153.7 (7)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N2—H9···O6i 0.85 (2) 2.15 (4) 2.979 (15) 162 (8)
N2—H10···O5ii 0.85 (2) 2.43 (8) 3.121 (13) 138 (10)
O7—H16···O4iii 0.85 (2) 1.80 (2) 2.639 (6) 169 (7)
O3—H8···O8iv 0.86 (2) 1.79 (3) 2.640 (6) 167 (7)
N1—H1···O2v 0.85 (2) 2.15 (3) 2.996 (15) 170 (9)
N1—H2···O1vi 0.85 (2) 2.30 (8) 2.998 (13) 139 (10)
N1—H2···O5vii 0.85 (2) 2.42 (7) 3.117 (13) 140 (10)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2526).

References

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  12. Vagg, R. S. (1979). Acta Cryst. B35, 341–344.

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, publication_text. DOI: 10.1107/S1600536811035860/wm2526sup1.cif

e-67-m1362-sup1.cif (18.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811035860/wm2526Isup2.hkl

e-67-m1362-Isup2.hkl (118.2KB, hkl)

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


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