Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Sep 14;67(Pt 10):m1356. doi: 10.1107/S1600536811035422

Bis(triphenyl­phosphanyl­idene)iminium dichloridotriphenyl­stannate(IV)

Lucio De Lorentiis a, Claudia Graiff a,*, Giovanni Predieri a
PMCID: PMC3201402  PMID: 22065826

Abstract

The structure of the title compound, [Ph3P=N=PPh3]+[Ph3SnCl2] or (C36H30NP2)[Sn(C6H5)3Cl2], obtained as a by product of the reaction between Ph3SnCl and [Ph3P=N=PPh3]+·HSeO3 , consists of discrete essentially isolated ions. Both the cation and the anion lie on twofold axes which pass through the central N atom in the cation and through the SnIV atom in the anion. In the crystal, the ions inter­act only through a weak inter­action between the Cl atom of the anion and an H atom of a phenyl ring of the cation.

Related literature

For general background to selenite compounds, see: Delferro et al. (2010, 2011). For related structures, see: Harrison et al. (1978); Nayek et al. (2010); Ng (1995, 1999). For details of the Cambridge Crystal Structure Database, see: Allen (2002).graphic file with name e-67-m1356-scheme1.jpg

Experimental

Crystal data

  • (C36H30NP2)[Sn(C6H5)3Cl2]

  • M r = 959.44

  • Orthorhombic, Inline graphic

  • a = 17.9119 (6) Å

  • b = 9.7744 (3) Å

  • c = 13.3835 (4) Å

  • V = 2343.16 (13) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.76 mm−1

  • T = 296 K

  • 0.42 × 0.22 × 0.18 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2007) T min = 0.629, T max = 0.746

  • 36432 measured reflections

  • 7179 independent reflections

  • 6352 reflections with I > 2σ(I)

  • R int = 0.026

Refinement

  • R[F 2 > 2σ(F 2)] = 0.025

  • wR(F 2) = 0.065

  • S = 1.04

  • 7179 reflections

  • 273 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.20 e Å−3

  • Δρmin = −0.25 e Å−3

  • Absolute structure: Flack (1983), 3430 Friedel pairs

  • Flack parameter: −0.022 (13)

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811035422/su2296sup1.cif

e-67-m1356-sup1.cif (20.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811035422/su2296Isup2.hkl

e-67-m1356-Isup2.hkl (351.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811035422/su2296Isup3.mol

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
C9—H9⋯Cl1i 0.93 2.79 3.718 (2) 173

Symmetry code: (i) Inline graphic.

Acknowledgments

Financial support from the PRIN 2008-Mol­ecular Clusters in Nanoscience and the University of Parma, Italy, is gratefully acknowledged.

supplementary crystallographic information

Comment

The title compound was isolated from a dichloromethane solution as a by product of the reaction between of Ph3SnCl with [Ph3P=N=PPh3]+ HSeO3- in dichloromethane solvent. The hydrogen selenite salt, prepared in the framework of our research activity on selenite compounds (Delferro et al., 2010, Delferro et al., 2011), contained a significant amount of [Ph3P=N=PPh3]+ Cl-, which is responsible of the formation of the title compound.

The structure of the title compound consists of discrete [Ph3P=N=PPh3]+ and [Ph3SnCl2]- ions (Fig. 1). The [Ph3P=N=PPh3]+, (or PPN+ for simplicity), cation is rather typical, lieing on a two fold axis that passes through the central N atom, N1. The P1—N1 bond distance of 1.5763 (9) Å and the P1—N1—P1i [symmetry code (i) = -x + 2, -y + 1, z] bond angle of 141.9 (2)° are in good agreement with the average values of 1.577 (6) Å and 143 (9)° found in 1409 PPN+ cations reported in the Cambridge Crystal Structure Database (CSD, V5.32, last update May 2011; Allen, 2002), see Fig. 3. In particular, examining the 1409 PPN+ cations it is evident that less than 40 examples present a linear geometry at the nitrogen atom. On excluding these cases the mean value of the P—N—P bond angle is reduced to 142 (7)°, even more in agreement with the angle in the title compound. The P atom is tetrahedral, with the C—P—C and C—P—N angles averaging 109 (3)°.

The [Ph3SnCl2]- anion exhibits trigonal bipyramidal geometry at the tin atom, with the usual equatorial arrangement of organic groups and the chlorine atoms occupying axial positions. The anion is lying on a two-fold axis passing through the tin atom and atom C25 and C28 of one phenyl ring. The Cl1—Sn1 bond distance is 2.5858 (4) Å and the Cl—Sn—Clii [symmetry code: (ii) = -x + 2, -y + 2, z] bond angle is 177.83 (4)°, both in agreement with the values found in four examples (Ng, 1995,1999; Harrison et al., 1978; Nayek et al., 2010) reported in the CSD: The mean values are 2.590 (2) Å and 176.6 (7)°, respectively. The mean planes of the phenyl rings form dihedral angles of 59.70 (2)° and 38.78 (2)° with the SnC3 mean plane.

In the crystal there is a weak interaction between the chlorine atom of the dichlorotriphenylstannate anion and a hydrogen atom of a phenyl ring of the bis(triphenylphosphine)iminium cation (Table 1).

Experimental

A dichloromethane solution of equimolar amounts of triphenyl-tin chloride and bis(triphenylphosphine)iminium hydrogenselenite was stirred at room temperature for 1 h. The solution was then cooled slowly to 278 K. Crystals suitable for X-ray analysis were obtained from the solution in two days.

Refinement

The C-bound H-atoms were included in calculated positions and treated as riding atoms: C-H = 0.93 Å for CH(aromatic), with Uiso(H) = 1.2Ueq(parent C-atom).

Figures

Fig. 1.

Fig. 1.

ORTEP drawing of the [Ph3P=N=PPh3]+ cation, showing the atom labelling and the displacement ellipsoids drawn at the 30% probability level. Hydrogen atoms are omitted for clarity. Symmetry code for generating equivalent atoms: ' = -x + 2, -y + 1, z.

Fig. 2.

Fig. 2.

ORTEP drawing of the [Ph3SnCl2]- anion, showing the atom labelling and the displacement ellipsoids drawn at the 30% probability level. Hydrogen atoms are omitted for clarity. Symmetry code for generating equivalent atoms: ' = -x + 2, -y + 2, z.

Fig. 3.

Fig. 3.

Histogram showing the distribution of the P—N—P bond angle over the 1409 [Ph3P=N=PPh3]+ cations reported in the Cambridge Structural Database (Allen, 2002).

Crystal data

(C36H30NP2)[Sn(C6H5)3Cl2] F(000) = 980
Mr = 959.44 Dx = 1.360 Mg m3
Orthorhombic, Pnn2 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2 -2n Cell parameters from 999 reflections
a = 17.9119 (6) Å θ = 3–27°
b = 9.7744 (3) Å µ = 0.76 mm1
c = 13.3835 (4) Å T = 296 K
V = 2343.16 (13) Å3 Prism, colourless
Z = 2 0.42 × 0.22 × 0.18 mm

Data collection

Bruker APEXII CCD diffractometer 7179 independent reflections
Radiation source: fine-focus sealed tube 6352 reflections with I > 2σ(I)
graphite Rint = 0.026
ω scans θmax = 30.6°, θmin = 1.9°
Absorption correction: multi-scan (SADABS; Bruker, 2007) h = −25→25
Tmin = 0.629, Tmax = 0.746 k = −13→13
36432 measured reflections l = −19→19

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)] = 0.025 H-atom parameters constrained
wR(F2) = 0.065 w = 1/[σ2(Fo2) + (0.0339P)2 + 0.062P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.001
7179 reflections Δρmax = 0.20 e Å3
273 parameters Δρmin = −0.25 e Å3
1 restraint Absolute structure: Flack (1983), 3430 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: −0.022 (13)

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 0.88435 (9) 0.69033 (16) 0.54090 (12) 0.0432 (3)
C2 0.81206 (10) 0.72511 (17) 0.51192 (17) 0.0576 (5)
H2 0.7811 0.6596 0.4832 0.069*
C3 0.78656 (12) 0.8566 (2) 0.5259 (2) 0.0726 (6)
H3 0.7384 0.8800 0.5065 0.087*
C4 0.83185 (16) 0.9526 (2) 0.5683 (2) 0.0786 (7)
H4 0.8146 1.0416 0.5764 0.094*
C5 0.90228 (15) 0.9193 (2) 0.5988 (2) 0.0812 (7)
H5 0.9323 0.9852 0.6287 0.097*
C6 0.92925 (11) 0.7871 (2) 0.58522 (17) 0.0611 (5)
H6 0.9772 0.7643 0.6059 0.073*
C7 0.85781 (9) 0.40724 (16) 0.59273 (12) 0.0436 (3)
C8 0.88264 (11) 0.3604 (2) 0.68448 (15) 0.0542 (4)
H8 0.9306 0.3818 0.7060 0.065*
C9 0.83627 (14) 0.2816 (2) 0.74452 (16) 0.0677 (5)
H9 0.8530 0.2500 0.8061 0.081*
C10 0.76534 (13) 0.2506 (2) 0.71193 (19) 0.0711 (6)
H10 0.7339 0.1989 0.7524 0.085*
C11 0.74047 (11) 0.2948 (2) 0.62107 (19) 0.0660 (6)
H11 0.6928 0.2713 0.5995 0.079*
C12 0.78589 (9) 0.37442 (19) 0.56092 (16) 0.0537 (4)
H12 0.7685 0.4059 0.4996 0.064*
C13 0.90382 (10) 0.48460 (16) 0.39035 (14) 0.0428 (3)
C14 0.91498 (10) 0.5907 (2) 0.32243 (14) 0.0507 (4)
H14 0.9251 0.6784 0.3456 0.061*
C15 0.91117 (12) 0.5664 (3) 0.22073 (16) 0.0654 (5)
H15 0.9192 0.6376 0.1758 0.078*
C16 0.89552 (13) 0.4373 (3) 0.18605 (18) 0.0725 (6)
H16 0.8922 0.4215 0.1177 0.087*
C17 0.88481 (14) 0.3321 (3) 0.2517 (2) 0.0783 (7)
H17 0.8744 0.2450 0.2273 0.094*
C18 0.88920 (11) 0.3529 (2) 0.35474 (17) 0.0601 (5)
H18 0.8825 0.2804 0.3989 0.072*
C19 0.93324 (11) 0.8460 (2) 0.92452 (14) 0.0555 (4)
C20 0.94493 (15) 0.7072 (2) 0.9444 (2) 0.0787 (6)
H20 0.9844 0.6807 0.9852 0.094*
C21 0.89793 (18) 0.6079 (3) 0.9033 (3) 0.0981 (8)
H21 0.9064 0.5160 0.9172 0.118*
C22 0.84039 (17) 0.6437 (3) 0.8437 (2) 0.0908 (8)
H22 0.8097 0.5766 0.8166 0.109*
C23 0.82711 (15) 0.7791 (3) 0.82299 (19) 0.0835 (7)
H23 0.7874 0.8035 0.7819 0.100*
C24 0.87280 (12) 0.8799 (2) 0.86322 (17) 0.0681 (5)
H24 0.8630 0.9714 0.8492 0.082*
C25 1.0000 1.0000 1.1555 (2) 0.0497 (6)
C26 1.06462 (16) 1.0253 (2) 1.20891 (19) 0.0680 (6)
H26 1.1092 1.0408 1.1752 0.082*
C27 1.0633 (2) 1.0278 (3) 1.3133 (2) 0.0940 (11)
H27 1.1066 1.0488 1.3484 0.113*
C28 1.0000 1.0000 1.3635 (3) 0.104 (2)
H28 1.0000 1.0000 1.4329 0.125*
N1 1.0000 0.5000 0.55925 (18) 0.0477 (5)
P1 0.91740 (2) 0.51807 (4) 0.52080 (3) 0.03734 (9)
Sn1 1.0000 1.0000 0.996036 (19) 0.04870 (5)
Cl1 0.88562 (3) 1.16132 (5) 0.99969 (5) 0.07087 (13)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0413 (8) 0.0429 (7) 0.0452 (8) −0.0004 (6) 0.0109 (6) −0.0061 (6)
C2 0.0472 (8) 0.0522 (8) 0.0735 (14) 0.0078 (6) 0.0013 (9) −0.0093 (10)
C3 0.0606 (11) 0.0593 (11) 0.0979 (19) 0.0178 (9) 0.0169 (11) −0.0040 (11)
C4 0.0870 (17) 0.0482 (10) 0.1007 (18) 0.0135 (11) 0.0296 (14) −0.0106 (11)
C5 0.0852 (16) 0.0531 (12) 0.105 (2) −0.0121 (11) 0.0140 (14) −0.0259 (12)
C6 0.0527 (10) 0.0546 (10) 0.0760 (13) −0.0077 (8) 0.0047 (9) −0.0150 (9)
C7 0.0381 (7) 0.0415 (7) 0.0513 (9) −0.0010 (6) 0.0064 (7) −0.0023 (7)
C8 0.0569 (11) 0.0566 (10) 0.0490 (10) −0.0034 (8) 0.0032 (8) −0.0030 (8)
C9 0.0928 (16) 0.0613 (11) 0.0491 (10) −0.0055 (10) 0.0154 (10) 0.0016 (9)
C10 0.0732 (14) 0.0598 (12) 0.0802 (15) −0.0155 (10) 0.0313 (12) −0.0049 (10)
C11 0.0459 (10) 0.0605 (11) 0.0914 (16) −0.0101 (8) 0.0166 (10) −0.0056 (11)
C12 0.0390 (8) 0.0516 (10) 0.0703 (12) −0.0042 (7) 0.0018 (8) 0.0020 (8)
C13 0.0355 (7) 0.0512 (9) 0.0418 (9) 0.0077 (6) −0.0030 (6) −0.0088 (6)
C14 0.0497 (9) 0.0579 (9) 0.0445 (9) 0.0199 (7) −0.0037 (7) 0.0002 (7)
C15 0.0618 (11) 0.0859 (15) 0.0484 (10) 0.0300 (11) −0.0056 (9) 0.0042 (10)
C16 0.0651 (13) 0.1060 (18) 0.0464 (11) 0.0206 (13) −0.0085 (9) −0.0204 (13)
C17 0.0743 (14) 0.0871 (17) 0.0736 (16) −0.0019 (12) 0.0025 (12) −0.0441 (14)
C18 0.0597 (11) 0.0558 (11) 0.0648 (13) −0.0010 (8) 0.0035 (9) −0.0120 (9)
C19 0.0593 (11) 0.0659 (11) 0.0414 (9) 0.0071 (8) 0.0049 (8) −0.0087 (8)
C20 0.0872 (16) 0.0715 (13) 0.0774 (15) 0.0129 (12) −0.0088 (12) −0.0081 (11)
C21 0.113 (2) 0.0713 (16) 0.110 (2) −0.0072 (15) −0.0013 (18) −0.0146 (16)
C22 0.0943 (19) 0.0950 (19) 0.0831 (18) −0.0156 (15) 0.0095 (15) −0.0308 (14)
C23 0.0711 (15) 0.114 (2) 0.0650 (14) 0.0008 (14) −0.0075 (11) −0.0255 (14)
C24 0.0700 (13) 0.0775 (13) 0.0567 (11) 0.0032 (10) −0.0080 (9) −0.0113 (10)
C25 0.0626 (16) 0.0476 (13) 0.0389 (13) −0.0052 (10) 0.000 0.000
C26 0.0810 (15) 0.0662 (11) 0.0568 (13) −0.0148 (10) −0.0186 (11) 0.0072 (9)
C27 0.152 (3) 0.0699 (14) 0.0604 (16) −0.0191 (16) −0.0434 (19) 0.0006 (12)
C28 0.210 (7) 0.064 (2) 0.0396 (17) −0.012 (2) 0.000 0.000
N1 0.0341 (9) 0.0663 (13) 0.0427 (11) 0.0008 (8) 0.000 0.000
P1 0.03077 (16) 0.04225 (16) 0.0390 (2) 0.00106 (13) 0.00104 (13) −0.00220 (15)
Sn1 0.04949 (8) 0.06206 (9) 0.03456 (7) 0.00872 (6) 0.000 0.000
Cl1 0.0614 (2) 0.0894 (3) 0.0618 (3) 0.0292 (2) −0.0110 (3) −0.0201 (3)

Geometric parameters (Å, °)

C1—C6 1.376 (2) C16—C17 1.367 (4)
C1—C2 1.394 (2) C16—H16 0.9300
C1—P1 1.8049 (16) C17—C18 1.396 (4)
C2—C3 1.377 (2) C17—H17 0.9300
C2—H2 0.9300 C18—H18 0.9300
C3—C4 1.364 (4) C19—C24 1.398 (3)
C3—H3 0.9300 C19—C20 1.398 (3)
C4—C5 1.365 (4) C19—Sn1 2.1476 (19)
C4—H4 0.9300 C20—C21 1.397 (4)
C5—C6 1.391 (3) C20—H20 0.9300
C5—H5 0.9300 C21—C22 1.349 (4)
C6—H6 0.9300 C21—H21 0.9300
C7—C8 1.384 (3) C22—C23 1.373 (4)
C7—C12 1.394 (2) C22—H22 0.9300
C7—P1 1.7998 (16) C23—C24 1.389 (3)
C8—C9 1.389 (3) C23—H23 0.9300
C8—H8 0.9300 C24—H24 0.9300
C9—C10 1.377 (3) C25—C26i 1.383 (3)
C9—H9 0.9300 C25—C26 1.383 (3)
C10—C11 1.365 (4) C25—Sn1 2.134 (3)
C10—H10 0.9300 C26—C27 1.397 (4)
C11—C12 1.384 (3) C26—H26 0.9300
C11—H11 0.9300 C27—C28 1.346 (5)
C12—H12 0.9300 C27—H27 0.9300
C13—C18 1.398 (3) C28—C27i 1.345 (5)
C13—C14 1.393 (3) C28—H28 0.9300
C13—P1 1.7929 (19) N1—P1ii 1.5763 (9)
C14—C15 1.383 (3) N1—P1 1.5763 (9)
C14—H14 0.9300 Sn1—C19i 2.1476 (19)
C15—C16 1.374 (4) Sn1—Cl1 2.5858 (4)
C15—H15 0.9300 Sn1—Cl1i 2.5858 (4)
C6—C1—C2 119.70 (16) C17—C18—C13 118.8 (2)
C6—C1—P1 120.91 (14) C17—C18—H18 120.6
C2—C1—P1 119.39 (12) C13—C18—H18 120.6
C1—C2—C3 119.87 (18) C24—C19—C20 117.2 (2)
C1—C2—H2 120.1 C24—C19—Sn1 121.74 (16)
C3—C2—H2 120.1 C20—C19—Sn1 120.81 (16)
C4—C3—C2 120.1 (2) C21—C20—C19 120.6 (3)
C4—C3—H3 120.0 C21—C20—H20 119.7
C2—C3—H3 120.0 C19—C20—H20 119.7
C5—C4—C3 120.7 (2) C22—C21—C20 120.8 (3)
C5—C4—H4 119.7 C22—C21—H21 119.6
C3—C4—H4 119.7 C20—C21—H21 119.6
C4—C5—C6 120.2 (2) C23—C22—C21 120.1 (3)
C4—C5—H5 119.9 C23—C22—H22 119.9
C6—C5—H5 119.9 C21—C22—H22 119.9
C1—C6—C5 119.4 (2) C22—C23—C24 120.2 (3)
C1—C6—H6 120.3 C22—C23—H23 119.9
C5—C6—H6 120.3 C24—C23—H23 119.9
C8—C7—C12 119.46 (16) C19—C24—C23 121.0 (2)
C8—C7—P1 118.89 (13) C19—C24—H24 119.5
C12—C7—P1 121.54 (14) C23—C24—H24 119.5
C7—C8—C9 120.3 (2) C26i—C25—C26 117.7 (3)
C7—C8—H8 119.8 C26i—C25—Sn1 121.14 (16)
C9—C8—H8 119.8 C26—C25—Sn1 121.14 (16)
C8—C9—C10 119.4 (2) C25—C26—C27 120.4 (3)
C8—C9—H9 120.3 C25—C26—H26 119.8
C10—C9—H9 120.3 C27—C26—H26 119.8
C11—C10—C9 120.91 (19) C28—C27—C26 120.6 (3)
C11—C10—H10 119.5 C28—C27—H27 119.7
C9—C10—H10 119.5 C26—C27—H27 119.7
C10—C11—C12 120.3 (2) C27i—C28—C27 120.1 (4)
C10—C11—H11 119.9 C27i—C28—H28 119.9
C12—C11—H11 119.9 C27—C28—H28 119.9
C11—C12—C7 119.66 (19) P1ii—N1—P1 141.90 (17)
C11—C12—H12 120.2 N1—P1—C13 115.13 (10)
C7—C12—H12 120.2 N1—P1—C7 108.34 (8)
C18—C13—C14 119.33 (18) C13—P1—C7 109.30 (8)
C18—C13—P1 121.71 (15) N1—P1—C1 111.33 (6)
C14—C13—P1 118.69 (13) C13—P1—C1 105.72 (8)
C15—C14—C13 120.5 (2) C7—P1—C1 106.69 (7)
C15—C14—H14 119.8 C25—Sn1—C19i 116.46 (5)
C13—C14—H14 119.8 C25—Sn1—C19 116.46 (5)
C16—C15—C14 120.0 (2) C19i—Sn1—C19 127.07 (10)
C16—C15—H15 120.0 C25—Sn1—Cl1 88.916 (18)
C14—C15—H15 120.0 C19i—Sn1—Cl1 91.27 (5)
C17—C16—C15 120.2 (2) C19—Sn1—Cl1 89.70 (5)
C17—C16—H16 119.9 C25—Sn1—Cl1i 88.917 (18)
C15—C16—H16 119.9 C19i—Sn1—Cl1i 89.70 (5)
C16—C17—C18 121.2 (2) C19—Sn1—Cl1i 91.27 (5)
C16—C17—H17 119.4 Cl1—Sn1—Cl1i 177.83 (4)
C18—C17—H17 119.4

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

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C9—H9···Cl1iii 0.93 2.79 3.718 (2) 173

Symmetry codes: (iii) x, y−1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2296).

References

  1. Allen, F. H. (2002). Acta Cryst. B58, 380–388. [DOI] [PubMed]
  2. Bruker (2007). APEX2, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Delferro, M., Graiff, C., Elviri, L. & Predieri, G. (2010). Dalton Trans. 39, 4479–4481. [DOI] [PubMed]
  4. Delferro, M., Graiff, C., Marchiò, L., Elviri, L., Mazzani, M., Riccò, M. & Predieri, G. (2011). Eur. J. Inorg. Chem. doi:10.1002/ejic.201100385.
  5. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  6. Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
  7. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  8. Harrison, P. G., Molloy, K., Phillips, R. C., Smith, P. J. & Crowe, A. J. (1978). J. Organomet. Chem. 160, 421–434.
  9. Nayek, H. P., Massa, W. & Dehnen, S. (2010). Inorg. Chem. 49, 144–149. [DOI] [PubMed]
  10. Ng, S. W. (1995). Acta Cryst. C51, 1124–1125.
  11. Ng, S. W. (1999). Acta Cryst. C55, IUC9900098.
  12. 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 datablock(s) I, global. DOI: 10.1107/S1600536811035422/su2296sup1.cif

e-67-m1356-sup1.cif (20.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811035422/su2296Isup2.hkl

e-67-m1356-Isup2.hkl (351.3KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811035422/su2296Isup3.mol

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