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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Sep 25;66(Pt 10):m1300. doi: 10.1107/S1600536810028989

Poly[[hexa­aqua­tris­[μ2-2,5-dihy­droxy-1,4-benzoquinona­to(2−)]diholmium(III)] octa­deca­hydrate]

Koji Nakabayashi a, Shin-ichi Ohkoshi a,*
PMCID: PMC2983139  PMID: 21587439

Abstract

In the polymeric title compound, {[Ho2(C6H2O4)3(H2O)6]·18H2O}n, the HoIII ion is nine-coordinated by six O atoms derived from three bidentate 2,5-dihy­droxy-1,4-benzoquinonate (DHBQ2−) ligands and three O atoms from three water mol­ecules. The HoIII ions are connected via three ligands, resulting in the formation of a two-dimensional honeycomb layer parallel to the ab plane. The layer is racemic in which Δ- and Λ-coordination geometries around HoIII ions are alternately arranged. The asymmetric unit comprises a third of a HoIII ion, located on a threefold axis, one-half of a DHBQ2− ion, located on a centre of inversion, one coordinated water mol­ecule and three uncoordinated water mol­ecules.

Related literature

For general background, see: Kitagawa & Kawata (2002); Nakabayashi & Ohkoshi (2009); Ohkoshi et al. (2001). For details of the synthesis, see: Weider et al. (1985). For related structures, see: Robl & Sheldrick (1988); Weiss et al. (1986).graphic file with name e-66-m1300-scheme1.jpg

Experimental

Crystal data

  • [Ho2(C6H2O4)3(H2O)6]·18H2O

  • M r = 1176.46

  • Trigonal, Inline graphic

  • a = 14.1407 (3) Å

  • c = 18.0629 (5) Å

  • V = 3127.93 (12) Å3

  • Z = 3

  • Mo Kα radiation

  • μ = 3.88 mm−1

  • T = 90 K

  • 0.10 × 0.10 × 0.04 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.704, T max = 0.856

  • 11262 measured reflections

  • 1594 independent reflections

  • 1525 reflections with I > 2σ(I)

  • R int = 0.025

Refinement

  • R[F 2 > 2σ(F 2)] = 0.023

  • wR(F 2) = 0.063

  • S = 1.23

  • 1594 reflections

  • 86 parameters

  • H-atom parameters constrained

  • Δρmax = 0.65 e Å−3

  • Δρmin = −0.30 e Å−3

Data collection: PROCESS-AUTO (Rigaku, 1998); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and pyMOL (DeLano, 2007); software used to prepare material for publication: CrystalStructure.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810028989/tk2691sup1.cif

e-66-m1300-sup1.cif (20.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810028989/tk2691Isup2.hkl

e-66-m1300-Isup2.hkl (78.9KB, hkl)

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

Table 1. Selected bond lengths (Å).

Ho1—O1 2.371 (2)
Ho1—O2 2.463 (2)
Ho1—O3 2.385 (3)

Acknowledgments

We are thankful for a Grant-in-Aid for Young Scientists (S) from JSPS, the Global COE Program, "Chemistry Innovation through Cooperation of Science and Engineering" from MEXT Japan, the Photon Frontier Network Program from MEXT, the Izumi Science and Technology Foundation and Asahi Glass Foundation. We also thank the Cryogenic Research Center and the Center for Nano Lithography & Analysis, The University of Tokyo, supported by MEXT Japan. This work has been approved by the Photon Factory Program Advisory Committee (Proposal 2009 G678).

supplementary crystallographic information

Comment

Lanthanide complexes have attracted attention as magnetic and luminescent materials due to the properties of the 4f orbitals in lanthanide ions. Although the magnetism of mononuclear lanthanide complexes are well understood, studies on polynuclear lanthanide complexes are much less advanced (Ohkoshi et al., 2001). The dimensionality of complexes and coordination geometry around lanthanide ions are key factors to control their magnetic properties. From this viewpoint, constructing polynuclear lanthanide complexes with various topologies are interesting. In our previous work, we reported the 3-D monometallic lanthanide metal assembly, Na5[{Ho(THB4-)2}.7H2O]n (THB = 1,2,4,5-tetrahydroxybenzene) (Nakabayashi et al., 2009). In this work, we synthesized a 2-D honeycomb network composed of holmium ions (HoIII) and 2,5-dihydroxy-1,4-benzoquinonate, [{Ho2 (DHBQ2-)3 (H2O)6}.18H2O]n (Kitagawa et al., 2002; Robl et al., 1988).

The asymmetric unit comprises a third of a HoIII ion, being located on a three-fold axis, one-half of a DHBQ2- ion, being disposed about a centre of inversion, one coordinated water molecule, and three zeolitic water molecules.

The C—O distances of 1.276 (4) Å (C1—O1) and 1.274 (3) Å (C2—O2) in this compound agree with those of the DHBQ2- ligands which were previously reported, e.g. 1.276 (6) Å (Weiss et al. 1986). In the coordination geometry, a HoIII ion is coordinated to six O atoms from three bidentate DHBQ2- ligands and three O atoms from three water molecules (Fig. 1 and Table 1). The HoIII ion is connected via three ligands, which results in a two-dimensional honeycomb layer with a diameter of 16.6 Å. The layer has a racemic structure in which Δ- and Λ-coordination geometries around HoIII ions are alternately arranged (Fig. 2). The zeolitic water molecules occupy regions between the layers.

The product of the molar magnetic susceptibility (χM) and temperature (T), χMT, values at room temperature was 13.6 cm3 K mol-1. This value nearly corresponds to the expected value of 13.9 cm3 K mol-1 due to HoIII ions (J = 8, L = 6, S = 2, and g = 5/4).

All known compounds of this type have two specific structures, honeycomb or racemic, and show paramagnetism. Mixing lanthanide ions, the chiral lanthanide assemblies with Δ- or Λ-coordination geometries are targeted for synthesis, which should show a magneto-chiral dichroism. A study to clarify this hypotheses, work is currently under way.

Experimental

Under air, aqueous solutions of 0.1 M Ho(NO3)3 and 0.4 M 1,2,4,5-tetrahydroxybenzene (THB) (Weider et al., 1985) mixed. THB was gradually oxidized to 2,5-dihydroxy-1,4-benzoquinone (DHBQ) in the mixed solution, and slow complexation of Ho(NO3)3 and DHBQ) produced red crystals of the title polymer in 24% yield within a week. The obtained polycrystalline compound was dried under air. Elemental analysis indicated the formula was [Ho2(C6H2O4)3(H2O)6].17H2O, C18H52O35Ho2, calcd. Ho, 28.18%; C, 18.47%; H, 4.49%, found. Ho, 28.29%; C, 18.23%; H, 4.64%. There is a slight difference of zeolitic water molecules between the elemental analysis and the crystallographic formulation because zeolitic water molecules are easy to be lost from the crystals and their number depends on the drying processes.

Refinement

The H atoms were placed in their calculated positions,with C—H = 0.95 Å, and refined using a riding model, with Uiso(H) = 1.2 Ueq(C).

Figures

Fig. 1.

Fig. 1.

A part of the title polymeric compound, thermal ellipsoids are shown at the 50% probability level. Blue, gray, and red represent Ho, C and O atoms, respectively. The labeled atoms indicate all independent atoms.

Fig. 2.

Fig. 2.

A layer with a honeycomb structure. Blue spheres and gray sticks represent Ho atoms and other atoms (C and O), respectively.

Crystal data

[Ho2(C6H2O4)3(H2O)6]·18H2O Dx = 1.796 Mg m3
Mr = 1176.46 Mo Kα radiation, λ = 0.71075 Å
Trigonal, R3 Cell parameters from 9640 reflections
Hall symbol: -R 3 θ = 3.4–27.5°
a = 14.1407 (3) Å µ = 3.88 mm1
c = 18.0629 (5) Å T = 90 K
V = 3127.93 (12) Å3 Platelet, red
Z = 3 0.10 × 0.10 × 0.04 mm
F(000) = 1608.00

Data collection

Rigaku R-AXIS RAPID diffractometer 1525 reflections with F2 > 2σ(F2)
Detector resolution: 10.00 pixels mm-1 Rint = 0.025
ω scans θmax = 27.5°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) h = −18→18
Tmin = 0.704, Tmax = 0.856 k = −18→18
11262 measured reflections l = −23→23
1594 independent reflections

Refinement

Refinement on F2 H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.023 w = 1/[σ2(Fo2) + (0.0248P)2 + 19.995P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.063 (Δ/σ)max = 0.002
S = 1.23 Δρmax = 0.65 e Å3
1594 reflections Δρmin = −0.30 e Å3
86 parameters

Special details

Geometry. loop_ _Bond lengths and angles Ho1 - Distance Angles O1_$1 2.3715 (0.0023) O1 2.3715 (0.0024) 78.04 (0.09) O1_$2 2.3715 (0.0023) 78.05 (0.09) 78.05 (0.09) O3_$2 2.3851 (0.0025) 138.54 (0.09) 85.02 (0.10) 134.88 (0.09) O3_$1 2.3851 (0.0025) 134.88 (0.09) 138.54 (0.09) 85.02 (0.10) 80.68 (0.11) O3 2.3852 (0.0025) 85.02 (0.10) 134.88 (0.09) 138.54 (0.09) 80.68 (0.11) 80.68 (0.11) O2_$1 2.4626 (0.0024) 65.01 (0.08) 134.82 (0.08) 69.90 (0.08) 140.07 (0.09) 69.92 (0.09) 68.65 (0.09) O2 2.4626 (0.0023) 69.90 (0.08) 65.01 (0.08) 134.82 (0.08) 68.65 (0.09) 140.07 (0.09) 69.92 (0.08) 119.91 (0.01) O2_$2 2.4626 (0.0023) 134.82 (0.08) 69.90 (0.08) 65.01 (0.08) 69.92 (0.08) 68.65 (0.09) 140.07 (0.09) 119.91 (0.01) Ho1 - O1_$1 O1 O1_$2 O3_$2 O3_$1 O3 O2_$1 O1 - Distance Angles C1 1.2764 (0.0041) Ho1 2.3715 (0.0023) 123.38 (0.21) O1 - C1 O2 - Distance Angles C2 1.2739 (0.0041) Ho1 2.4626 (0.0023) 119.92 (0.21) O2 - C2 O3 - Distance Angles Ho1 2.3852 (0.0025) O3 - C1 - Distance Angles O1 1.2764 (0.0041) C3 1.3846 (0.0049) 125.21 (0.32) C2 1.5290 (0.0046) 114.26 (0.29) 120.50 (0.30) C1 - O1 C3 C3 - Distance Angles C1 1.3846 (0.0049) C2_$3 1.3982 (0.0048) 119.67 (0.32) H3 0.9500 120.16 120.16 C3 - C1 C2_$3 C2 - Distance Angles O2 1.2739 (0.0041) C3_$3 1.3982 (0.0048) 124.89 (0.31) C1 1.5290 (0.0046) 115.30 (0.29) 119.80 (0.30) C2 - O2 C3_$3
Refinement. Refinement was performed using all reflections. The weighted R-factor (wR) and goodness of fit (S) are based on F2. R-factor (gt) are based on F. The threshold expression of F2 > 2.0 σ(F2) is used only for calculating R-factor (gt).

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

x y z Uiso*/Ueq
Ho1 0.0000 0.0000 0.754297 (13) 0.01802 (8)
O1 −0.1198 (2) −0.12391 (19) 0.66415 (13) 0.0270 (5)
O2 −0.00678 (19) −0.17736 (19) 0.75023 (13) 0.0252 (4)
O3 0.1248 (2) −0.0026 (2) 0.84201 (15) 0.0366 (6)
O4 0.1390 (2) −0.1541 (2) 0.93023 (18) 0.0481 (7)
O5 0.2672 (2) 0.1817 (2) 0.92192 (19) 0.0508 (7)
O6 −0.1882 (2) −0.0598 (2) 0.54192 (17) 0.0474 (7)
C1 −0.1492 (2) −0.2252 (2) 0.66312 (19) 0.0246 (6)
C3 −0.2332 (2) −0.3039 (2) 0.6206 (2) 0.0283 (7)
C2 −0.0802 (2) −0.2555 (2) 0.71218 (18) 0.0237 (6)
H3 −0.2770 −0.2850 0.5912 0.034*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ho1 0.01630 (11) 0.01630 (11) 0.02146 (14) 0.00815 (5) 0.0000 0.0000
O1 0.0310 (13) 0.0178 (11) 0.0320 (12) 0.0121 (10) −0.0067 (9) −0.0020 (9)
O2 0.0240 (11) 0.0194 (11) 0.0316 (12) 0.0103 (9) −0.0047 (9) −0.0032 (9)
O3 0.0363 (14) 0.0309 (14) 0.0405 (14) 0.0154 (12) −0.0164 (11) −0.0020 (11)
O4 0.0455 (18) 0.0513 (18) 0.0552 (18) 0.0299 (15) −0.0062 (14) 0.0051 (15)
O5 0.0490 (18) 0.0453 (18) 0.0558 (19) 0.0218 (15) −0.0121 (15) −0.0078 (14)
O6 0.0528 (19) 0.0470 (18) 0.0418 (16) 0.0244 (15) −0.0105 (13) 0.0015 (13)
C1 0.0241 (16) 0.0227 (15) 0.0271 (15) 0.0116 (13) 0.0016 (12) 0.0014 (12)
C3 0.0274 (17) 0.0235 (17) 0.0334 (17) 0.0122 (14) −0.0049 (13) 0.0001 (13)
C2 0.0228 (15) 0.0236 (16) 0.0241 (15) 0.0111 (13) 0.0019 (12) 0.0005 (12)

Geometric parameters (Å, °)

Ho1—O1 2.371 (2) Ho1—O3ii 2.385 (2)
Ho1—O1i 2.371 (2) O1—C1 1.276 (4)
Ho1—O1ii 2.371 (2) O2—C2 1.274 (3)
Ho1—O2 2.463 (2) C1—C3 1.385 (4)
Ho1—O2i 2.4625 (19) C1—C2 1.529 (6)
Ho1—O2ii 2.463 (3) C3—C2iii 1.398 (5)
Ho1—O3 2.385 (3) C3—H3 0.950
Ho1—O3i 2.385 (3)
Ho1···C1 3.253 (3) O6···C1 3.444 (5)
Ho1···C1i 3.253 (3) O6···C1ii 3.369 (4)
Ho1···C1ii 3.253 (4) O6···C3 3.485 (5)
Ho1···C2 3.289 (3) O6···C3xi 3.326 (5)
Ho1···C2i 3.289 (2) C1···Ho1 3.253 (3)
Ho1···C2ii 3.289 (4) C1···O1i 3.592 (3)
O1···O1i 2.986 (3) C1···O2 2.372 (4)
O1···O1ii 2.986 (3) C1···O3ii 3.481 (4)
O1···O2 2.599 (4) C1···O6 3.444 (5)
O1···O2ii 2.770 (4) C1···O6i 3.369 (4)
O1···O3ii 3.214 (3) C1···C1iii 2.847 (5)
O1···O4iv 3.464 (4) C1···C3iii 2.533 (6)
O1···O6 2.740 (4) C1···C2iii 2.406 (4)
O1···O6i 3.390 (4) C3···O1 2.363 (3)
O1···C1ii 3.592 (5) C3···O2iii 2.370 (4)
O1···C3 2.363 (3) C3···O6 3.485 (5)
O1···C2 2.360 (5) C3···O6xii 3.326 (4)
O1···C2ii 3.458 (5) C3···C1iii 2.533 (6)
O2···O1 2.599 (4) C3···C3iii 2.927 (6)
O2···O1i 2.770 (3) C3···C2 2.531 (5)
O2···O3 2.778 (3) C2···Ho1 3.289 (3)
O2···O3ii 2.734 (4) C2···O1 2.360 (5)
O2···O4v 2.868 (5) C2···O1i 3.458 (3)
O2···O5ii 3.325 (4) C2···O3ii 3.254 (5)
O2···C1 2.372 (4) C2···O4v 3.499 (5)
O2···C3iii 2.370 (4) C2···C1iii 2.406 (4)
O3···O1i 3.214 (3) C2···C3 2.531 (5)
O3···O2 2.778 (3) C2···C2iii 2.855 (4)
O3···O2i 2.734 (3) O1···H3 2.608
O3···O3i 3.088 (5) O2···H3iii 2.614
O3···O3ii 3.088 (4) O4···H3ix 3.259
O3···O4 2.757 (5) O4···H3vi 3.484
O3···O5 2.772 (3) O5···H3ix 3.135
O3···C1i 3.481 (4) O6···H3 2.918
O3···C2i 3.254 (3) O6···H3xi 3.032
O4···O1vi 3.464 (5) C1···H3 2.035
O4···O2v 2.868 (5) C1···H3iii 3.400
O4···O3 2.757 (5) C2···H3 3.396
O4···O5ii 2.753 (4) C2···H3iii 2.048
O4···O5vii 2.802 (4) H3···O1 2.608
O4···C2v 3.499 (5) H3···O2iii 2.614
O5···O2i 3.325 (4) H3···O4x 3.259
O5···O3 2.772 (3) H3···O4iv 3.484
O5···O4i 2.753 (6) H3···O5x 3.135
O5···O4viii 2.802 (4) H3···O6 2.918
O5···O6ix 2.728 (4) H3···O6xii 3.032
O6···O1 2.740 (4) H3···C1 2.035
O6···O1ii 3.390 (3) H3···C1iii 3.400
O6···O5x 2.728 (4) H3···C2 3.396
O6···O6xi 2.801 (4) H3···C2iii 2.048
O6···O6xii 2.801 (5)
O1—Ho1—O1i 78.04 (8) O2—Ho1—O3i 140.07 (9)
O1—Ho1—O1ii 78.04 (8) O2—Ho1—O3ii 68.65 (10)
O1—Ho1—O2 65.01 (9) O2i—Ho1—O2ii 119.91 (9)
O1—Ho1—O2i 134.81 (7) O2i—Ho1—O3 68.65 (8)
O1—Ho1—O2ii 69.90 (9) O2i—Ho1—O3i 69.92 (8)
O1—Ho1—O3 134.88 (10) O2i—Ho1—O3ii 140.07 (8)
O1—Ho1—O3i 138.54 (11) O2ii—Ho1—O3 140.07 (9)
O1—Ho1—O3ii 85.02 (8) O2ii—Ho1—O3i 68.65 (9)
O1i—Ho1—O1ii 78.04 (10) O2ii—Ho1—O3ii 69.92 (10)
O1i—Ho1—O2 69.90 (8) O3—Ho1—O3i 80.68 (11)
O1i—Ho1—O2i 65.01 (8) O3—Ho1—O3ii 80.68 (9)
O1i—Ho1—O2ii 134.81 (8) O3i—Ho1—O3ii 80.68 (9)
O1i—Ho1—O3 85.02 (10) Ho1—O1—C1 123.4 (2)
O1i—Ho1—O3i 134.88 (7) Ho1—O2—C2 119.9 (2)
O1i—Ho1—O3ii 138.54 (10) O1—C1—C3 125.2 (4)
O1ii—Ho1—O2 134.81 (8) O1—C1—C2 114.3 (2)
O1ii—Ho1—O2i 69.90 (8) C3—C1—C2 120.5 (3)
O1ii—Ho1—O2ii 65.01 (8) C1—C3—C2iii 119.7 (4)
O1ii—Ho1—O3 138.54 (7) O2—C2—C1 115.3 (3)
O1ii—Ho1—O3i 85.02 (9) O2—C2—C3iii 124.9 (3)
O1ii—Ho1—O3ii 134.88 (11) C1—C2—C3iii 119.8 (2)
O2—Ho1—O2i 119.91 (9) C1—C3—H3 120.2
O2—Ho1—O2ii 119.91 (7) C2iii—C3—H3 120.2
O2—Ho1—O3 69.92 (9)
O1—Ho1—O1i—C1i 166.8 (3) O3—Ho1—O1ii—C1ii −125.1 (2)
O1i—Ho1—O1—C1 86.7 (2) O3i—Ho1—O1ii—C1ii −55.3 (2)
O1—Ho1—O1ii—C1ii 86.7 (2) O3ii—Ho1—O1ii—C1ii 16.3 (2)
O1ii—Ho1—O1—C1 166.8 (2) O2—Ho1—O2i—C2i 34.3 (2)
O1—Ho1—O2—C2 −10.8 (2) O2i—Ho1—O2—C2 −139.8 (2)
O2—Ho1—O1—C1 13.5 (2) O2—Ho1—O2ii—C2ii −139.8 (2)
O1—Ho1—O2i—C2i −49.0 (3) O2ii—Ho1—O2—C2 34.3 (2)
O2i—Ho1—O1—C1 121.7 (2) O3—Ho1—O2—C2 171.3 (2)
O1—Ho1—O2ii—C2ii −96.6 (2) O3i—Ho1—O2—C2 126.2 (2)
O2ii—Ho1—O1—C1 −125.7 (2) O3ii—Ho1—O2—C2 83.8 (2)
O3—Ho1—O1—C1 16.3 (3) O2i—Ho1—O2ii—C2ii 34.3 (2)
O3i—Ho1—O1—C1 −125.1 (2) O2ii—Ho1—O2i—C2i −139.8 (2)
O3ii—Ho1—O1—C1 −55.3 (2) O3—Ho1—O2i—C2i 83.8 (2)
O1i—Ho1—O1ii—C1ii 166.8 (2) O3i—Ho1—O2i—C2i 171.3 (2)
O1ii—Ho1—O1i—C1i 86.7 (3) O3ii—Ho1—O2i—C2i 126.2 (2)
O1i—Ho1—O2—C2 −96.6 (2) O3—Ho1—O2ii—C2ii 126.2 (2)
O2—Ho1—O1i—C1i −125.7 (3) O3i—Ho1—O2ii—C2ii 83.8 (2)
O1i—Ho1—O2i—C2i −10.8 (2) O3ii—Ho1—O2ii—C2ii 171.3 (2)
O2i—Ho1—O1i—C1i 13.5 (3) Ho1—O1—C1—C3 167.6 (2)
O1i—Ho1—O2ii—C2ii −49.0 (2) Ho1—O1—C1—C2 −14.4 (4)
O2ii—Ho1—O1i—C1i 121.7 (3) Ho1—O2—C2—C1 8.1 (3)
O3—Ho1—O1i—C1i −55.3 (3) Ho1—O2—C2—C3iii −171.9 (2)
O3i—Ho1—O1i—C1i 16.3 (3) O1—C1—C3—C2iii 176.2 (3)
O3ii—Ho1—O1i—C1i −125.1 (3) O1—C1—C2—O2 3.4 (4)
O1ii—Ho1—O2—C2 −49.0 (2) O1—C1—C2—C3iii −176.5 (3)
O2—Ho1—O1ii—C1ii 121.7 (2) C3—C1—C2—O2 −178.4 (3)
O1ii—Ho1—O2i—C2i −96.6 (2) C3—C1—C2—C3iii 1.7 (5)
O2i—Ho1—O1ii—C1ii −125.7 (2) C2—C1—C3—C2iii −1.7 (5)
O1ii—Ho1—O2ii—C2ii −10.8 (2) C1—C3—C2iii—O2iii −178.5 (3)
O2ii—Ho1—O1ii—C1ii 13.5 (2) C1—C3—C2iii—C1iii 1.6 (5)

Symmetry codes: (i) −y, xy, z; (ii) −x+y, −x, z; (iii) −x−1/3, −y−2/3, −z+4/3; (iv) xy−2/3, x−1/3, −z+5/3; (v) −x+1/3, −y−1/3, −z+5/3; (vi) y+1/3, −x+y−1/3, −z+5/3; (vii) y, −x+y, −z+2; (viii) xy, x, −z+2; (ix) x+2/3, y+1/3, z+1/3; (x) x−2/3, y−1/3, z−1/3; (xi) y, −x+y, −z+1; (xii) xy, x, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: TK2691).

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 global, I. DOI: 10.1107/S1600536810028989/tk2691sup1.cif

e-66-m1300-sup1.cif (20.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810028989/tk2691Isup2.hkl

e-66-m1300-Isup2.hkl (78.9KB, hkl)

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


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