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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 18;67(Pt 1):o149. doi: 10.1107/S1600536810052153

2,4,6-Trimethyl­pyridinium dihydrogen phosphate

Jing Dai a,*, Jie Xu a
PMCID: PMC3050353  PMID: 21522656

Abstract

The asymmetric unit of the title compound, C8H12N+·H2PO4 −, contains two H2PO4 − anions and two 2,4,6-trimethyl­pyridinium cations. In the crystal, the anions are linked by O—H⋯O hydrogen bonds, forming supra­molecular chains running along the a axis; the cations are connected to the anion chains by N—H⋯O hydrogen bonds. Weak inter­molecular C—H⋯O hydrogen bonding is also present in the crystal structure.

Related literature

For the properties and structures of pyridine salts, see: Fu et al. (2007 ▶, 2008 ▶, 2009 ▶); Fu & Xiong (2008 ▶).graphic file with name e-67-0o149-scheme1.jpg

Experimental

Crystal data

  • C8H12N+·H2PO4 −

  • M r = 219.17

  • Monoclinic, Inline graphic

  • a = 7.9501 (16) Å

  • b = 15.324 (3) Å

  • c = 9.0252 (18) Å

  • β = 97.97 (3)°

  • V = 1088.9 (4) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.24 mm−1

  • T = 298 K

  • 0.30 × 0.05 × 0.05 mm

Data collection

  • Rigaku Mercury2 diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.910, T max = 1.000

  • 11306 measured reflections

  • 4970 independent reflections

  • 3973 reflections with I > 2σ(I)

  • R int = 0.033

Refinement

  • R[F 2 > 2σ(F 2)] = 0.044

  • wR(F 2) = 0.101

  • S = 1.02

  • 4970 reflections

  • 275 parameters

  • 5 restraints

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

  • Δρmax = 0.15 e Å−3

  • Δρmin = −0.25 e Å−3

  • Absolute structure: Flack (1983 ▶), 2380 Friedel pairs

  • Flack parameter: 0.01 (8)

Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; 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: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810052153/xu5121sup1.cif

e-67-0o149-sup1.cif (20.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052153/xu5121Isup2.hkl

e-67-0o149-Isup2.hkl (243.4KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
O1—H1⋯O8 0.85 (2) 1.77 (2) 2.610 (2) 169 (3)
O3—H3⋯O7i 0.85 (3) 1.72 (3) 2.569 (2) 173 (3)
O5—H5⋯O4ii 0.84 (2) 1.79 (2) 2.627 (3) 173 (3)
O6—H6⋯O2 0.85 (2) 1.69 (2) 2.538 (2) 176 (3)
N1—H1A⋯O4iii 0.86 1.77 2.633 (3) 177
N2—H2A⋯O8iv 0.86 1.78 2.632 (3) 170
C2—H2B⋯O6v 0.93 2.59 3.443 (4) 152
C4—H4A⋯O7i 0.93 2.59 3.481 (4) 161

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

Acknowledgments

This work was supported by a start-up grant from Southeast University, China.

supplementary crystallographic information

Comment

Salts of pyridine attracted more attention as phase transition dielectric materials for its application in memory storage (Fu et al. 2007; Fu & Xiong 2008; Fu et al. 2008; Fu et al. 2009). With the purpose of obtaining phase transition crystals of 2,4,6-trimethylpyridine salts, its interaction with various acids has been studied and we have elaborated a series of new materials with this organic molecule. In this study, we describe the crystal structure of the title compound, di-2,4,6-trimethylpyridinium dihydrogen phosphate.

The dielectric constant of title compound as a function of temperature indicates that the permittivity is basically temperature-independent, suggesting that this compound should be not a real ferroelectrics or there may be no distinct phase transition occurred within the measured temperature range. Similarly, below the melting point (425 K) of the compound, the dielectric constant as a function of temperature also goes smoothly, and there is no dielectric anomaly observed (dielectric constant equaling to 6.9 to 8.7).

The asymmetric unit is composed of two H2PO4- anion and two C8H12N+ cation (Fig.1). Both the pyridine N atoms are protonated, thus indicating two positive charges in the pyridine N atoms. And the H2PO4- anions were showing two negative charges to make the charge balance. The geometric parameters of the title compound are in the normal range.

In the crystal structure, all the H atoms of pyridinium cations and the H2PO4- anions are involved in N—H···O and O—H···O hydrogen bonds. These hydrogen bonds link the ionic units into a one-dimentional chains parallel to the a-axis. Furthermore, the π···π (centroid-to-centroid distance = 3.8403 (8) Å and 4.1676 (8) Å) interactions link the chains into a two-dimentional network parallel to the (0 0 1) plane. (Table 1 and Fig.2).

Experimental

The commercial 2,4,6-trimethylpyridine (3 mmol) was dissolved in water/H3PO4 (50:1 v/v) solution. The solvent was slowly evaporated in air affording colourless needle-shaped crystals of the title compound suitable for X-ray analysis.

Refinement

H atoms of H2PO 4- anions were located in a difference Fourier map and freely refined, with the O—H distance constrained to 0.85 Å. Other H atoms were fixed geometrically and treated as riding with C–H = 0.93 Å (aromatic), 0.96 Å (methyl) and N–H = 0.86 Å, with Uiso(H) = 1.2Ueq(C,N) and Uiso(H) = 1.5Ueq(C) for methyl.

Figures

Fig. 1.

Fig. 1.

A view of the title compound with the atomic numbering scheme. Displacement ellipsoids were drawn at the 30% probability level.

Fig. 2.

Fig. 2.

The crystal packing of the title compound, showing the two-dimensional network. H atoms not involved in hydrogen bonding (dashed line) have been omitted for clarity.

Crystal data

C8H12N+·H2PO4− F(000) = 464
Mr = 219.17 Dx = 1.337 Mg m−3
Monoclinic, P21 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2yb Cell parameters from 4970 reflections
a = 7.9501 (16) Å θ = 3.2–27.5°
b = 15.324 (3) Å µ = 0.24 mm−1
c = 9.0252 (18) Å T = 298 K
β = 97.97 (3)° Needle, colorless
V = 1088.9 (4) Å3 0.30 × 0.05 × 0.05 mm
Z = 4

Data collection

Rigaku Mercury2 diffractometer 4970 independent reflections
Radiation source: fine-focus sealed tube 3973 reflections with I > 2σ(I)
graphite Rint = 0.033
Detector resolution: 13.6612 pixels mm-1 θmax = 27.5°, θmin = 3.2°
CCD profile fitting scans h = −10→10
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) k = −19→19
Tmin = 0.910, Tmax = 1.000 l = −11→11
11306 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)] = 0.044 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.101 w = 1/[σ2(Fo2) + (0.0489P)2 + 0.0746P] where P = (Fo2 + 2Fc2)/3
S = 1.02 (Δ/σ)max = 0.001
4970 reflections Δρmax = 0.15 e Å−3
275 parameters Δρmin = −0.25 e Å−3
5 restraints Absolute structure: Flack (1983), 2380 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.01 (8)

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
P1 0.90061 (8) 0.60246 (4) 0.30479 (7) 0.04278 (17)
P2 0.39135 (8) 0.53464 (4) 0.24480 (8) 0.04306 (17)
O1 0.8423 (2) 0.51862 (14) 0.3826 (2) 0.0600 (5)
N1 0.9315 (3) 0.21030 (14) 0.3374 (2) 0.0439 (5)
H1A 0.9367 0.1865 0.4242 0.053*
O5 0.3427 (2) 0.54241 (16) 0.4065 (2) 0.0618 (5)
O2 0.7595 (2) 0.66752 (12) 0.2811 (2) 0.0532 (5)
N2 0.5339 (3) 0.80459 (14) 0.7547 (2) 0.0445 (5)
H2A 0.4972 0.8574 0.7515 0.053*
O6 0.4507 (2) 0.62723 (13) 0.2008 (3) 0.0632 (6)
O3 0.9432 (2) 0.57407 (16) 0.1485 (2) 0.0602 (6)
O7 0.2392 (2) 0.50926 (13) 0.1375 (2) 0.0558 (5)
O4 1.0612 (2) 0.63287 (13) 0.4013 (2) 0.0561 (5)
O8 0.5398 (2) 0.47211 (12) 0.2575 (2) 0.0561 (5)
C8 1.0619 (4) 0.3360 (2) 0.4720 (3) 0.0654 (8)
H8A 1.1303 0.2957 0.5356 0.098*
H8B 0.9697 0.3560 0.5215 0.098*
H8C 1.1301 0.3849 0.4506 0.098*
C13 0.5302 (3) 0.76072 (19) 0.6246 (3) 0.0481 (6)
C5 0.9927 (3) 0.29160 (17) 0.3293 (3) 0.0490 (6)
C1 0.8620 (3) 0.16344 (18) 0.2166 (3) 0.0459 (6)
C12 0.5901 (4) 0.6770 (2) 0.6307 (3) 0.0565 (7)
H12A 0.5901 0.6457 0.5424 0.068*
C9 0.5917 (3) 0.77016 (17) 0.8891 (3) 0.0456 (6)
C10 0.6513 (3) 0.68578 (18) 0.8946 (3) 0.0512 (7)
H10A 0.6924 0.6609 0.9865 0.061*
C2 0.8552 (4) 0.2015 (2) 0.0782 (3) 0.0553 (7)
H2B 0.8070 0.1712 −0.0064 0.066*
C6 0.8017 (4) 0.0734 (2) 0.2423 (3) 0.0633 (8)
H6A 0.8924 0.0404 0.2973 0.095*
H6B 0.7662 0.0456 0.1478 0.095*
H6C 0.7078 0.0760 0.2985 0.095*
C11 0.6509 (3) 0.63792 (17) 0.7658 (3) 0.0526 (7)
C14 0.5867 (5) 0.8266 (2) 1.0239 (3) 0.0691 (9)
H14A 0.6357 0.8824 1.0076 0.104*
H14B 0.6501 0.7993 1.1097 0.104*
H14C 0.4710 0.8342 1.0407 0.104*
C3 0.9196 (4) 0.2845 (2) 0.0636 (3) 0.0580 (7)
C4 0.9881 (4) 0.3288 (2) 0.1899 (3) 0.0585 (7)
H4A 1.0319 0.3846 0.1812 0.070*
C15 0.7111 (5) 0.5453 (2) 0.7726 (4) 0.0814 (10)
H15A 0.7847 0.5357 0.8648 0.122*
H15B 0.7721 0.5339 0.6900 0.122*
H15C 0.6152 0.5068 0.7673 0.122*
C16 0.4597 (4) 0.8072 (2) 0.4839 (3) 0.0729 (9)
H16A 0.4441 0.8678 0.5054 0.109*
H16B 0.3524 0.7819 0.4443 0.109*
H16C 0.5372 0.8018 0.4119 0.109*
C7 0.9177 (5) 0.3237 (3) −0.0919 (4) 0.0923 (12)
H7A 0.9096 0.3861 −0.0860 0.138*
H7B 0.8218 0.3015 −0.1575 0.138*
H7C 1.0204 0.3082 −0.1302 0.138*
H5 0.254 (2) 0.5713 (15) 0.413 (3) 0.048 (8)*
H1 0.745 (2) 0.4985 (19) 0.350 (3) 0.060 (9)*
H6 0.5523 (18) 0.643 (2) 0.229 (3) 0.072 (11)*
H3 1.037 (3) 0.549 (2) 0.142 (4) 0.089 (13)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
P1 0.0381 (3) 0.0457 (4) 0.0429 (4) −0.0005 (3) 0.0001 (3) 0.0003 (3)
P2 0.0388 (3) 0.0379 (3) 0.0519 (4) −0.0018 (3) 0.0045 (3) −0.0010 (3)
O1 0.0492 (11) 0.0587 (14) 0.0693 (13) 0.0007 (11) −0.0019 (10) 0.0212 (10)
N1 0.0441 (11) 0.0414 (12) 0.0453 (12) 0.0021 (10) 0.0025 (9) 0.0010 (9)
O5 0.0510 (11) 0.0827 (15) 0.0503 (11) 0.0086 (12) 0.0020 (9) −0.0016 (11)
O2 0.0446 (11) 0.0436 (10) 0.0695 (13) 0.0002 (9) 0.0014 (9) 0.0022 (9)
N2 0.0467 (12) 0.0372 (11) 0.0492 (13) 0.0005 (10) 0.0053 (10) 0.0018 (9)
O6 0.0416 (11) 0.0469 (12) 0.0982 (16) −0.0006 (9) −0.0008 (11) 0.0205 (10)
O3 0.0453 (11) 0.0892 (16) 0.0445 (11) 0.0043 (11) −0.0002 (8) −0.0064 (10)
O7 0.0446 (10) 0.0650 (13) 0.0565 (11) −0.0038 (9) 0.0023 (8) −0.0165 (9)
O4 0.0421 (10) 0.0681 (13) 0.0556 (11) 0.0002 (9) −0.0022 (8) −0.0160 (9)
O8 0.0424 (10) 0.0383 (10) 0.0862 (14) 0.0005 (9) 0.0034 (9) −0.0012 (9)
C8 0.074 (2) 0.0488 (16) 0.0685 (19) −0.0032 (16) −0.0079 (16) −0.0075 (15)
C13 0.0465 (15) 0.0522 (16) 0.0439 (15) −0.0034 (13) 0.0000 (11) −0.0035 (12)
C5 0.0447 (14) 0.0375 (14) 0.0641 (18) 0.0052 (12) 0.0048 (12) 0.0029 (12)
C1 0.0396 (13) 0.0469 (15) 0.0506 (15) −0.0012 (12) 0.0039 (11) −0.0048 (12)
C12 0.0620 (17) 0.0548 (17) 0.0520 (16) −0.0010 (15) 0.0051 (13) −0.0139 (14)
C9 0.0485 (15) 0.0424 (14) 0.0462 (15) −0.0074 (12) 0.0072 (11) 0.0034 (11)
C10 0.0540 (16) 0.0512 (16) 0.0476 (15) −0.0020 (13) 0.0044 (12) 0.0129 (13)
C2 0.0521 (15) 0.0615 (19) 0.0521 (17) 0.0062 (15) 0.0065 (12) −0.0039 (14)
C6 0.0656 (19) 0.0533 (18) 0.072 (2) −0.0094 (15) 0.0119 (15) −0.0097 (14)
C11 0.0472 (15) 0.0407 (15) 0.0696 (19) 0.0005 (12) 0.0074 (13) −0.0007 (13)
C14 0.102 (3) 0.0580 (18) 0.0482 (17) −0.0005 (19) 0.0136 (16) −0.0051 (14)
C3 0.0587 (17) 0.0607 (19) 0.0554 (17) 0.0128 (15) 0.0103 (13) 0.0066 (14)
C4 0.0590 (17) 0.0442 (15) 0.072 (2) 0.0042 (14) 0.0098 (15) 0.0080 (15)
C15 0.087 (2) 0.0502 (19) 0.105 (3) 0.0163 (18) 0.009 (2) 0.0011 (18)
C16 0.088 (2) 0.073 (2) 0.0536 (18) 0.0057 (19) −0.0051 (17) 0.0082 (16)
C7 0.107 (3) 0.098 (3) 0.073 (2) 0.012 (3) 0.015 (2) 0.034 (2)

Geometric parameters (Å, °)

P1—O2 1.494 (2) C12—C11 1.384 (4)
P1—O4 1.5155 (19) C12—H12A 0.9300
P1—O3 1.558 (2) C9—C10 1.376 (4)
P1—O1 1.565 (2) C9—C14 1.498 (4)
P2—O7 1.4924 (19) C10—C11 1.374 (4)
P2—O8 1.5120 (19) C10—H10A 0.9300
P2—O6 1.564 (2) C2—C3 1.385 (4)
P2—O5 1.565 (2) C2—H2B 0.9300
O1—H1 0.849 (10) C6—H6A 0.9600
N1—C5 1.343 (3) C6—H6B 0.9600
N1—C1 1.358 (3) C6—H6C 0.9600
N1—H1A 0.8600 C11—C15 1.497 (4)
O5—H5 0.843 (10) C14—H14A 0.9600
N2—C9 1.343 (3) C14—H14B 0.9600
N2—C13 1.351 (3) C14—H14C 0.9600
N2—H2A 0.8600 C3—C4 1.373 (4)
O6—H6 0.849 (10) C3—C7 1.525 (4)
O3—H3 0.85 (3) C4—H4A 0.9300
C8—C5 1.492 (4) C15—H15A 0.9600
C8—H8A 0.9600 C15—H15B 0.9600
C8—H8B 0.9600 C15—H15C 0.9600
C8—H8C 0.9600 C16—H16A 0.9600
C13—C12 1.367 (4) C16—H16B 0.9600
C13—C16 1.495 (4) C16—H16C 0.9600
C5—C4 1.377 (4) C7—H7A 0.9600
C1—C2 1.372 (4) C7—H7B 0.9600
C1—C6 1.490 (4) C7—H7C 0.9600
O2—P1—O4 115.66 (12) C11—C10—H10A 119.7
O2—P1—O3 108.04 (12) C9—C10—H10A 119.7
O4—P1—O3 109.57 (11) C1—C2—C3 120.6 (3)
O2—P1—O1 110.44 (11) C1—C2—H2B 119.7
O4—P1—O1 105.82 (11) C3—C2—H2B 119.7
O3—P1—O1 106.98 (13) C1—C6—H6A 109.5
O7—P2—O8 115.98 (11) C1—C6—H6B 109.5
O7—P2—O6 108.51 (11) H6A—C6—H6B 109.5
O8—P2—O6 109.55 (10) C1—C6—H6C 109.5
O7—P2—O5 109.99 (11) H6A—C6—H6C 109.5
O8—P2—O5 105.56 (12) H6B—C6—H6C 109.5
O6—P2—O5 106.86 (13) C10—C11—C12 118.3 (3)
P1—O1—H1 117 (2) C10—C11—C15 120.5 (3)
C5—N1—C1 123.9 (2) C12—C11—C15 121.1 (3)
C5—N1—H1A 118.1 C9—C14—H14A 109.5
C1—N1—H1A 118.1 C9—C14—H14B 109.5
P2—O5—H5 115.0 (17) H14A—C14—H14B 109.5
C9—N2—C13 123.6 (2) C9—C14—H14C 109.5
C9—N2—H2A 118.2 H14A—C14—H14C 109.5
C13—N2—H2A 118.2 H14B—C14—H14C 109.5
P2—O6—H6 119 (2) C4—C3—C2 119.0 (3)
P1—O3—H3 120 (2) C4—C3—C7 121.4 (3)
C5—C8—H8A 109.5 C2—C3—C7 119.6 (3)
C5—C8—H8B 109.5 C3—C4—C5 120.7 (3)
H8A—C8—H8B 109.5 C3—C4—H4A 119.6
C5—C8—H8C 109.5 C5—C4—H4A 119.6
H8A—C8—H8C 109.5 C11—C15—H15A 109.5
H8B—C8—H8C 109.5 C11—C15—H15B 109.5
N2—C13—C12 117.8 (2) H15A—C15—H15B 109.5
N2—C13—C16 117.5 (3) C11—C15—H15C 109.5
C12—C13—C16 124.7 (3) H15A—C15—H15C 109.5
N1—C5—C4 118.0 (3) H15B—C15—H15C 109.5
N1—C5—C8 117.9 (3) C13—C16—H16A 109.5
C4—C5—C8 124.0 (3) C13—C16—H16B 109.5
N1—C1—C2 117.8 (3) H16A—C16—H16B 109.5
N1—C1—C6 118.0 (2) C13—C16—H16C 109.5
C2—C1—C6 124.2 (3) H16A—C16—H16C 109.5
C13—C12—C11 121.3 (3) H16B—C16—H16C 109.5
C13—C12—H12A 119.4 C3—C7—H7A 109.5
C11—C12—H12A 119.4 C3—C7—H7B 109.5
N2—C9—C10 118.4 (2) H7A—C7—H7B 109.5
N2—C9—C14 117.5 (2) C3—C7—H7C 109.5
C10—C9—C14 124.1 (2) H7A—C7—H7C 109.5
C11—C10—C9 120.7 (3) H7B—C7—H7C 109.5
C9—N2—C13—C12 −0.6 (4) N1—C1—C2—C3 0.8 (4)
C9—N2—C13—C16 179.1 (3) C6—C1—C2—C3 −177.7 (3)
C1—N1—C5—C4 −1.5 (4) C9—C10—C11—C12 0.5 (4)
C1—N1—C5—C8 178.6 (3) C9—C10—C11—C15 −178.2 (3)
C5—N1—C1—C2 0.5 (4) C13—C12—C11—C10 −0.7 (4)
C5—N1—C1—C6 179.1 (2) C13—C12—C11—C15 178.0 (3)
N2—C13—C12—C11 0.7 (4) C1—C2—C3—C4 −0.9 (4)
C16—C13—C12—C11 −178.9 (3) C1—C2—C3—C7 177.3 (3)
C13—N2—C9—C10 0.4 (4) C2—C3—C4—C5 −0.1 (4)
C13—N2—C9—C14 −179.6 (3) C7—C3—C4—C5 −178.4 (3)
N2—C9—C10—C11 −0.3 (4) N1—C5—C4—C3 1.3 (4)
C14—C9—C10—C11 179.6 (3) C8—C5—C4—C3 −178.8 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H1···O8 0.85 (2) 1.77 (2) 2.610 (2) 169 (3)
O3—H3···O7i 0.85 (3) 1.72 (3) 2.569 (2) 173 (3)
O5—H5···O4ii 0.84 (2) 1.79 (2) 2.627 (3) 173 (3)
O6—H6···O2 0.85 (2) 1.69 (2) 2.538 (2) 176 (3)
N1—H1A···O4iii 0.86 1.77 2.633 (3) 177
N2—H2A···O8iv 0.86 1.78 2.632 (3) 170
C2—H2B···O6v 0.93 2.59 3.443 (4) 152
C4—H4A···O7i 0.93 2.59 3.481 (4) 161

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5121).

References

  1. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  2. Fu, D.-W., Ge, J.-Z., Dai, J., Ye, H.-Y. & Qu, Z.-R. (2009). Inorg. Chem. Commun. 12, 994–997.
  3. Fu, D.-W., Song, Y.-M., Wang, G.-X., Ye, Q., Xiong, R.-G., Akutagawa, T., Nakamura, T., Chan, P. W. H. & Huang, S. P. D. (2007). J. Am. Chem. Soc. 129, 5346–5347. [DOI] [PubMed]
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  6. Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
  7. 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/S1600536810052153/xu5121sup1.cif

e-67-0o149-sup1.cif (20.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810052153/xu5121Isup2.hkl

e-67-0o149-Isup2.hkl (243.4KB, 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

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