Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Sep 6;64(Pt 10):o1881. doi: 10.1107/S160053680802775X

1,2,3,4-Tetra­methyl­cyclo­pent-2-ene-1,4-diol

Steffen Blaurock a, Axel Fischer a, Jochen Gottfriedsen a, Marlies Spoida a, Frank T Edelmann a,*
PMCID: PMC2959352  PMID: 21201094

Abstract

The title compound, C9H16O2, crystallizes with two mol­ecules in the asymmetric unit. The structure displays inter­molecular O—H⋯O hydrogen bonding.

Related literature

For related literature, see: Etter (1991); Brock & Duncan (1994); Fendrick et al. (1988).graphic file with name e-64-o1881-scheme1.jpg

Experimental

Crystal data

  • C9H16O2

  • M r = 156.22

  • Monoclinic, Inline graphic

  • a = 13.006 (3) Å

  • b = 10.5279 (16) Å

  • c = 13.892 (2) Å

  • β = 107.257 (10)°

  • V = 1816.6 (6) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 133 (2) K

  • 0.45 × 0.28 × 0.07 mm

Data collection

  • Bruker SMART CCD diffractometer

  • Absorption correction: none

  • 20936 measured reflections

  • 5532 independent reflections

  • 3876 reflections with I > 2σ(I)

  • R int = 0.048

Refinement

  • R[F 2 > 2σ(F 2)] = 0.048

  • wR(F 2) = 0.142

  • S = 1.03

  • 5532 reflections

  • 223 parameters

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

  • Δρmax = 0.41 e Å−3

  • Δρmin = −0.23 e Å−3

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: XP5 in SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053680802775X/bt2745sup1.cif

e-64-o1881-sup1.cif (21.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680802775X/bt2745Isup2.hkl

e-64-o1881-Isup2.hkl (270.9KB, 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
O1—H01⋯O2i 0.95 (2) 1.80 (2) 2.7438 (13) 174.7 (17)
O1′—H01′⋯O1 0.921 (18) 1.824 (18) 2.7345 (13) 169.3 (16)
O2—H02⋯O2′ii 0.841 (19) 1.89 (2) 2.7263 (13) 173.0 (18)
O2′—H02′⋯O1′ii 0.86 (2) 1.89 (2) 2.7333 (13) 166.1 (18)

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

Acknowledgments

Financial support by the Otto-von-Guericke-Universität Magdeburg is gratefully acknowledged.

supplementary crystallographic information

Comment

In the solid state, alcohols generally form hydrogen-bonded networks resulting in a variety of ring, chain, or helix structures (Brock & Duncan, 1994). The hitherto unknown title compound, 1,2,3,4-tetramethylcyclopen-2-ene-1,4-diol, was obtained in minor quantities (less than 5% isolated yield) in the form of colorless crystals during a preparation of 1,2,3,4-tetramethylcyclopentadiene according to the literature (Fendrick et al., 1988). The structure of the title compound is shown in Figure 1. Dimensions are available in the archived CIF. Especially notable is the hydrogen-bond network in the crystal structure. As depicted in Figure 2, four molecules of 1,2,3,4-tetramethylcyclopen-2-ene-1,4-diol are connected via hydrogen-bonds to give cyclic tetramers. Further hydrogen-bonding between adjacent tetrameric units results in an extended hydrogen-bond network.

Experimental

Crystals of the title compound were obtained as a minor by-product during the synthesis of 1,2,3,4-tetramethylcyclopentadiene according to the literature preparatio (Fendrick et al., 1988).

Refinement

H atoms bonded to C were refined with fixed individual displacement parameters [U(H) = 1.2 Ueq(C) or U(H) = 1.5 Ueq(Cmethyl)] using a riding model with C-H(methylen) = 0.99 Å or C-H(methyl) = 0.98Å, respectively. The H atoms bonded to O were refined isotropically.

Figures

Fig. 1.

Fig. 1.

The molecule of the title compound in the crystal. Displacement ellipsoids represent 50% probability levels. H-Atom radii are arbitrary.

Fig. 2.

Fig. 2.

The hydrogen-bond network.

Crystal data

C9H16O2 F(000) = 688
Mr = 156.22 Dx = 1.142 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P2ybc Cell parameters from 5784 reflections
a = 13.006 (3) Å θ = 2.5–30.0°
b = 10.5279 (16) Å µ = 0.08 mm1
c = 13.892 (2) Å T = 133 K
β = 107.257 (10)° Plate, colourless
V = 1816.6 (6) Å3 0.45 × 0.28 × 0.07 mm
Z = 8

Data collection

Bruker SMART CCD diffractometer 3876 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.048
graphite θmax = 30.5°, θmin = 1.6°
Detector resolution: 8.192 pixels mm-1 h = −18→18
ω–scans k = −14→15
20936 measured reflections l = −19→19
5532 independent reflections

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)] = 0.048 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.142 H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0812P)2] where P = (Fo2 + 2Fc2)/3
5532 reflections (Δ/σ)max = 0.002
223 parameters Δρmax = 0.41 e Å3
0 restraints Δρmin = −0.23 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
O1 0.16035 (7) 0.34338 (9) 0.59028 (7) 0.0255 (2)
O2 0.16763 (8) 0.21564 (10) 0.28457 (7) 0.0330 (3)
H02 0.2279 (16) 0.2415 (16) 0.3207 (14) 0.048 (5)*
H01 0.1585 (14) 0.3212 (17) 0.6560 (15) 0.055 (5)*
C1 0.08579 (10) 0.28972 (13) 0.41367 (9) 0.0260 (3)
H1A 0.0100 0.3172 0.3852 0.031*
H1B 0.1335 0.3623 0.4115 0.031*
C2 0.10655 (9) 0.24265 (12) 0.52290 (8) 0.0210 (2)
C3 0.17851 (9) 0.12814 (12) 0.52756 (9) 0.0217 (2)
C4 0.17849 (10) 0.09054 (12) 0.43564 (10) 0.0242 (3)
C5 0.11007 (10) 0.17648 (13) 0.35382 (9) 0.0260 (3)
C6 0.00335 (10) 0.20778 (14) 0.54767 (10) 0.0290 (3)
H6C 0.0216 0.1724 0.6159 0.035*
H6B −0.0368 0.1446 0.4992 0.035*
H6A −0.0410 0.2840 0.5438 0.035*
C7 0.23648 (11) 0.06809 (14) 0.62666 (10) 0.0312 (3)
H7C 0.2703 −0.0112 0.6148 0.037*
H7B 0.1851 0.0499 0.6641 0.037*
H7A 0.2920 0.1263 0.6659 0.037*
C8 0.23380 (13) −0.02192 (15) 0.40823 (12) 0.0397 (4)
H8C 0.2779 −0.0635 0.4698 0.048*
H8B 0.2800 0.0058 0.3678 0.048*
H8A 0.1799 −0.0819 0.3691 0.048*
C9 0.00891 (12) 0.11076 (17) 0.28879 (11) 0.0403 (4)
H9C −0.0333 0.1707 0.2385 0.048*
H9B −0.0343 0.0814 0.3315 0.048*
H9A 0.0293 0.0379 0.2545 0.048*
O1' 0.34071 (7) 0.44079 (8) 0.55499 (7) 0.0229 (2)
H01' 0.2803 (14) 0.4165 (17) 0.5720 (13) 0.042 (5)*
O2' 0.63799 (7) 0.68485 (9) 0.61022 (7) 0.0229 (2)
H02' 0.6360 (15) 0.6373 (17) 0.5589 (15) 0.053 (5)*
C1' 0.48169 (9) 0.58556 (11) 0.64713 (8) 0.0188 (2)
H1'1 0.5235 0.5089 0.6413 0.023*
H1'2 0.4843 0.5963 0.7186 0.023*
C2' 0.36462 (9) 0.57287 (11) 0.58020 (9) 0.0183 (2)
C3' 0.36529 (9) 0.64743 (11) 0.48658 (9) 0.0195 (2)
C4' 0.45363 (9) 0.71901 (11) 0.50268 (8) 0.0190 (2)
C5' 0.52810 (9) 0.70382 (11) 0.60928 (8) 0.0182 (2)
C6' 0.28221 (10) 0.62512 (13) 0.62934 (10) 0.0258 (3)
H6'C 0.2096 0.6166 0.5823 0.031*
H6'B 0.2974 0.7149 0.6461 0.031*
H6'A 0.2869 0.5772 0.6910 0.031*
C7' 0.27255 (10) 0.63672 (14) 0.39236 (10) 0.0279 (3)
H7'C 0.2824 0.6968 0.3420 0.033*
H7'B 0.2054 0.6563 0.4076 0.033*
H7'A 0.2691 0.5501 0.3658 0.033*
C8' 0.48398 (11) 0.80742 (12) 0.43083 (10) 0.0269 (3)
H8'C 0.4254 0.8108 0.3674 0.032*
H8'B 0.5497 0.7766 0.4178 0.032*
H8'A 0.4966 0.8926 0.4604 0.032*
C9' 0.52987 (11) 0.82140 (12) 0.67418 (10) 0.0251 (3)
H9'C 0.5805 0.8079 0.7414 0.030*
H9'B 0.4576 0.8364 0.6801 0.030*
H9'A 0.5526 0.8953 0.6427 0.030*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1 0.0289 (5) 0.0282 (5) 0.0219 (4) −0.0072 (4) 0.0112 (4) −0.0031 (4)
O2 0.0267 (5) 0.0570 (7) 0.0158 (4) −0.0163 (5) 0.0073 (4) −0.0031 (4)
C1 0.0231 (6) 0.0341 (7) 0.0202 (6) 0.0010 (5) 0.0056 (5) 0.0049 (5)
C2 0.0199 (6) 0.0263 (6) 0.0171 (5) −0.0033 (5) 0.0058 (4) 0.0005 (4)
C3 0.0188 (6) 0.0260 (6) 0.0205 (6) −0.0037 (5) 0.0061 (5) 0.0017 (5)
C4 0.0226 (6) 0.0274 (6) 0.0243 (6) −0.0055 (5) 0.0095 (5) −0.0036 (5)
C5 0.0208 (6) 0.0402 (7) 0.0173 (6) −0.0091 (5) 0.0061 (5) −0.0010 (5)
C6 0.0216 (6) 0.0397 (8) 0.0278 (7) −0.0046 (5) 0.0106 (5) −0.0011 (5)
C7 0.0316 (7) 0.0343 (7) 0.0265 (7) 0.0029 (6) 0.0067 (6) 0.0063 (6)
C8 0.0442 (9) 0.0363 (8) 0.0449 (9) 0.0000 (7) 0.0229 (7) −0.0084 (7)
C9 0.0297 (7) 0.0629 (11) 0.0264 (7) −0.0213 (7) 0.0055 (6) −0.0049 (7)
O1' 0.0221 (4) 0.0214 (4) 0.0278 (5) −0.0045 (3) 0.0114 (4) −0.0053 (3)
O2' 0.0167 (4) 0.0300 (5) 0.0219 (4) −0.0034 (3) 0.0057 (3) −0.0059 (4)
C1' 0.0199 (5) 0.0204 (5) 0.0160 (5) −0.0008 (4) 0.0053 (4) 0.0006 (4)
C2' 0.0185 (5) 0.0182 (5) 0.0193 (5) −0.0014 (4) 0.0074 (4) −0.0025 (4)
C3' 0.0204 (5) 0.0211 (6) 0.0166 (5) 0.0036 (4) 0.0049 (4) −0.0002 (4)
C4' 0.0227 (6) 0.0192 (5) 0.0161 (5) 0.0025 (4) 0.0071 (4) 0.0009 (4)
C5' 0.0171 (5) 0.0206 (6) 0.0175 (5) −0.0010 (4) 0.0062 (4) −0.0009 (4)
C6' 0.0249 (6) 0.0274 (6) 0.0288 (6) −0.0009 (5) 0.0138 (5) −0.0038 (5)
C7' 0.0250 (6) 0.0323 (7) 0.0215 (6) 0.0025 (5) −0.0006 (5) 0.0001 (5)
C8' 0.0320 (7) 0.0270 (6) 0.0241 (6) 0.0014 (5) 0.0119 (5) 0.0067 (5)
C9' 0.0301 (6) 0.0237 (6) 0.0230 (6) −0.0028 (5) 0.0101 (5) −0.0054 (5)

Geometric parameters (Å, °)

O1—C2 1.4498 (14) O1'—C2' 1.4451 (14)
O1—H01 0.95 (2) O1'—H01' 0.921 (18)
O2—C5 1.4434 (15) O2'—C5' 1.4394 (14)
O2—H02 0.841 (19) O2'—H02' 0.86 (2)
C1—C5 1.5388 (19) C1'—C2' 1.5365 (16)
C1—C2 1.5421 (17) C1'—C5' 1.5425 (16)
C1—H1A 0.9900 C1'—H1'1 0.9900
C1—H1B 0.9900 C1'—H1'2 0.9900
C2—C3 1.5157 (18) C2'—C3' 1.5214 (16)
C2—C6 1.5259 (17) C2'—C6' 1.5334 (17)
C3—C4 1.3369 (17) C3'—C4' 1.3362 (17)
C3—C7 1.4992 (17) C3'—C7' 1.4981 (17)
C4—C8 1.492 (2) C4'—C8' 1.5007 (17)
C4—C5 1.5174 (19) C4'—C5' 1.5184 (16)
C5—C9 1.5233 (18) C5'—C9' 1.5275 (16)
C6—H6C 0.9800 C6'—H6'C 0.9800
C6—H6B 0.9800 C6'—H6'B 0.9800
C6—H6A 0.9800 C6'—H6'A 0.9800
C7—H7C 0.9800 C7'—H7'C 0.9800
C7—H7B 0.9800 C7'—H7'B 0.9800
C7—H7A 0.9800 C7'—H7'A 0.9800
C8—H8C 0.9800 C8'—H8'C 0.9800
C8—H8B 0.9800 C8'—H8'B 0.9800
C8—H8A 0.9800 C8'—H8'A 0.9800
C9—H9C 0.9800 C9'—H9'C 0.9800
C9—H9B 0.9800 C9'—H9'B 0.9800
C9—H9A 0.9800 C9'—H9'A 0.9800
C2—O1—H01 107.2 (11) C2'—O1'—H01' 110.1 (11)
C5—O2—H02 105.7 (13) C5'—O2'—H02' 106.6 (13)
C5—C1—C2 106.18 (10) C2'—C1'—C5' 106.36 (9)
C5—C1—H1A 110.5 C2'—C1'—H1'1 110.5
C2—C1—H1A 110.5 C5'—C1'—H1'1 110.5
C5—C1—H1B 110.5 C2'—C1'—H1'2 110.5
C2—C1—H1B 110.5 C5'—C1'—H1'2 110.5
H1A—C1—H1B 108.7 H1'1—C1'—H1'2 108.6
O1—C2—C3 112.37 (10) O1'—C2'—C3' 110.16 (9)
O1—C2—C6 108.58 (10) O1'—C2'—C6' 108.94 (10)
C3—C2—C6 111.86 (10) C3'—C2'—C6' 112.18 (10)
O1—C2—C1 108.08 (10) O1'—C2'—C1' 109.49 (9)
C3—C2—C1 102.90 (10) C3'—C2'—C1' 102.50 (9)
C6—C2—C1 112.97 (10) C6'—C2'—C1' 113.42 (10)
C4—C3—C7 127.58 (12) C4'—C3'—C7' 128.18 (11)
C4—C3—C2 111.69 (11) C4'—C3'—C2' 111.76 (10)
C7—C3—C2 120.70 (11) C7'—C3'—C2' 120.05 (11)
C3—C4—C8 127.96 (13) C3'—C4'—C8' 128.40 (11)
C3—C4—C5 111.89 (11) C3'—C4'—C5' 111.83 (10)
C8—C4—C5 120.13 (12) C8'—C4'—C5' 119.76 (10)
O2—C5—C4 111.39 (11) O2'—C5'—C4' 111.58 (9)
O2—C5—C9 105.18 (10) O2'—C5'—C9' 105.43 (9)
C4—C5—C9 112.63 (12) C4'—C5'—C9' 112.58 (10)
O2—C5—C1 111.66 (11) O2'—C5'—C1' 111.89 (9)
C4—C5—C1 103.06 (10) C4'—C5'—C1' 102.51 (9)
C9—C5—C1 113.13 (12) C9'—C5'—C1' 113.06 (10)
C2—C6—H6C 109.5 C2'—C6'—H6'C 109.5
C2—C6—H6B 109.5 C2'—C6'—H6'B 109.5
H6C—C6—H6B 109.5 H6'C—C6'—H6'B 109.5
C2—C6—H6A 109.5 C2'—C6'—H6'A 109.5
H6C—C6—H6A 109.5 H6'C—C6'—H6'A 109.5
H6B—C6—H6A 109.5 H6'B—C6'—H6'A 109.5
C3—C7—H7C 109.5 C3'—C7'—H7'C 109.5
C3—C7—H7B 109.5 C3'—C7'—H7'B 109.5
H7C—C7—H7B 109.5 H7'C—C7'—H7'B 109.5
C3—C7—H7A 109.5 C3'—C7'—H7'A 109.5
H7C—C7—H7A 109.5 H7'C—C7'—H7'A 109.5
H7B—C7—H7A 109.5 H7'B—C7'—H7'A 109.5
C4—C8—H8C 109.5 C4'—C8'—H8'C 109.5
C4—C8—H8B 109.5 C4'—C8'—H8'B 109.5
H8C—C8—H8B 109.5 H8'C—C8'—H8'B 109.5
C4—C8—H8A 109.5 C4'—C8'—H8'A 109.5
H8C—C8—H8A 109.5 H8'C—C8'—H8'A 109.5
H8B—C8—H8A 109.5 H8'B—C8'—H8'A 109.5
C5—C9—H9C 109.5 C5'—C9'—H9'C 109.5
C5—C9—H9B 109.5 C5'—C9'—H9'B 109.5
H9C—C9—H9B 109.5 H9'C—C9'—H9'B 109.5
C5—C9—H9A 109.5 C5'—C9'—H9'A 109.5
H9C—C9—H9A 109.5 H9'C—C9'—H9'A 109.5
H9B—C9—H9A 109.5 H9'B—C9'—H9'A 109.5
C5—C1—C2—O1 139.28 (10) C5'—C1'—C2'—O1' 138.54 (9)
C5—C1—C2—C3 20.24 (12) C5'—C1'—C2'—C3' 21.61 (11)
C5—C1—C2—C6 −100.55 (12) C5'—C1'—C2'—C6' −99.55 (11)
O1—C2—C3—C4 −130.31 (11) O1'—C2'—C3'—C4' −130.65 (11)
C6—C2—C3—C4 107.25 (12) C6'—C2'—C3'—C4' 107.81 (12)
C1—C2—C3—C4 −14.31 (13) C1'—C2'—C3'—C4' −14.19 (13)
O1—C2—C3—C7 51.62 (15) O1'—C2'—C3'—C7' 50.55 (14)
C6—C2—C3—C7 −70.82 (14) C6'—C2'—C3'—C7' −70.99 (14)
C1—C2—C3—C7 167.63 (11) C1'—C2'—C3'—C7' 167.00 (10)
C7—C3—C4—C8 1.6 (2) C7'—C3'—C4'—C8' −0.3 (2)
C2—C3—C4—C8 −176.35 (12) C2'—C3'—C4'—C8' −178.94 (11)
C7—C3—C4—C5 −179.83 (12) C7'—C3'—C4'—C5' 179.35 (11)
C2—C3—C4—C5 2.27 (15) C2'—C3'—C4'—C5' 0.67 (14)
C3—C4—C5—O2 130.67 (12) C3'—C4'—C5'—O2' 133.00 (10)
C8—C4—C5—O2 −50.59 (16) C8'—C4'—C5'—O2' −47.36 (14)
C3—C4—C5—C9 −111.43 (13) C3'—C4'—C5'—C9' −108.69 (12)
C8—C4—C5—C9 67.31 (16) C8'—C4'—C5'—C9' 70.96 (14)
C3—C4—C5—C1 10.82 (14) C3'—C4'—C5'—C1' 13.10 (13)
C8—C4—C5—C1 −170.44 (12) C8'—C4'—C5'—C1' −167.25 (10)
C2—C1—C5—O2 −138.72 (10) C2'—C1'—C5'—O2' −140.96 (9)
C2—C1—C5—C4 −19.06 (12) C2'—C1'—C5'—C4' −21.28 (11)
C2—C1—C5—C9 102.85 (12) C2'—C1'—C5'—C9' 100.18 (11)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H01···O2i 0.95 (2) 1.80 (2) 2.7438 (13) 174.7 (17)
O1'—H01'···O1 0.921 (18) 1.824 (18) 2.7345 (13) 169.3 (16)
O2—H02···O2'ii 0.841 (19) 1.89 (2) 2.7263 (13) 173.0 (18)
O2'—H02'···O1'ii 0.86 (2) 1.89 (2) 2.7333 (13) 166.1 (18)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2745).

References

  1. Brock, C. P. & Duncan, L. L. (1994). Chem. Mater.6, 1307–1312.
  2. Bruker (1997). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Etter, M. C. (1991). J. Phys. Chem.95, 4601–4610.
  4. Fendrick, C. M., Schertz, L. D., Day, V. W. & Marks, T. J. (1988). Organometallics, 7, 1828–1838.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]

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/S160053680802775X/bt2745sup1.cif

e-64-o1881-sup1.cif (21.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S160053680802775X/bt2745Isup2.hkl

e-64-o1881-Isup2.hkl (270.9KB, hkl)

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