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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2007 Dec 6;64(Pt 1):m99. doi: 10.1107/S1600536807064458

Tetra­kis(triphenyl­arsine)copper(I) hexa­fluoridophosphate

Thomas Kern a, Günther Knör a, Manfred Zabel b, Uwe Monkowius a,*
PMCID: PMC2914971  PMID: 21200664

Abstract

In the crystal structure of the title compound, [Cu(C18H15As)4]PF6, the Cu atom is coordinated by four As atoms of triphenyl­arsine ligands in a tetra­hedral geometry. The complex cation is located on a crystallographic threefold axis. Both PF6 anions are located on special positions of site symmetry Inline graphic. The Cu—As bond of the independent arsine ligand is shorter than the Cu—As bonds of the three symmetry-related arsine ligands.

Related literature

For related literature, see: Bowmaker et al. (1990); Engelhardt et al. (1985).graphic file with name e-64-00m99-scheme1.jpg

Experimental

Crystal data

  • [Cu(C18H15As)4]PF6

  • M r = 1433.40

  • Trigonal, Inline graphic

  • a = 14.4025 (10) Å

  • c = 52.015 (4) Å

  • V = 9344.1 (12) Å3

  • Z = 6

  • Mo Kα radiation

  • μ = 2.55 mm−1

  • T = 296 K

  • 0.14 × 0.12 × 0.10 mm

Data collection

  • Stoe IPDS diffractometer

  • Absorption correction: refined from ΔF (Walker & Stuart, 1983) T min = 0.349, T max = 0.769

  • 23664 measured reflections

  • 4049 independent reflections

  • 3118 reflections with I > 2σ(I)

  • R int = 0.032

Refinement

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.097

  • S = 1.04

  • 4049 reflections

  • 254 parameters

  • H-atom parameters constrained

  • Δρmax = 1.77 e Å−3

  • Δρmin = −0.62 e Å−3

Data collection: IPDS Software (Stoe, 1998); cell refinement: IPDS Software; data reduction: IPDS Software; program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: PLATON.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536807064458/bt2651sup1.cif

e-64-00m99-sup1.cif (27.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807064458/bt2651Isup2.hkl

e-64-00m99-Isup2.hkl (198.8KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

As1—Cu1 2.5472 (5)
As1—C1 1.959 (4)
As1—C7 1.956 (3)
As1—C13 1.958 (5)
As2—Cu1 2.5044 (9)
As2—C19 1.950 (4)
Cu1—As1—C1 112.61 (13)
Cu1—As1—C7 117.80 (13)
Cu1—As1—C13 122.35 (11)
C1—As1—C7 101.64 (15)
C1—As1—C13 99.19 (17)
C7—As1—C13 99.85 (17)
Cu1—As2—C19 117.96 (10)
C19—As2—C19i 99.81 (18)
As1—Cu1—As2 109.30 (2)
As1—Cu1—As1i 109.65 (2)

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

supplementary crystallographic information

Comment

Crystals of the title compound were obtained as a side-product in the preparation of [(Ph-BIAN)Cu(I)(Ph3As)2][PF6] (Ph-BIAN = Bis(phenyl-imino)acenaphthene) in methylene chloride solution. To identify this compound a single-crystal structure analysis was performed.

The title compound contains [(Ph3As)4Cu]+ ions which are disposed about crystallographic threefold axes, the metal atom lying on a special position of symmetry 3 is coordinated by two independent ligands. One of it is totally independent, whereas the other three are symmetry-related completing the nearly regular tetrahedral environment of the copper atom. The bond angles are 109.30 (2) and 109.65 (2) ° for As1—Cu1—As2 and As1—Cu1—As1', respectively. Two independent phosphorus and fluorine atoms are found. The Cu—As2 bond of the independent (axial) arsine ligand is significantly shorter than the value for the off-axis Cu—As1 bonds (2.5044 (9) versus 2.5472 (5) Å). A similar distortion was previously found for the analogous salts [(Ph3P)4Cu]+ (with ClO4- or PF6- as anions), which also crystallize in the same space group (Bowmaker et al., 1990, Engelhardt et al., 1985).

Experimental

The title compound was isolated as a side-product in the preparation of [(Ph-BIAN)Cu(I)(Ph3As)2][PF6] (Ph-BIAN = Bis(phenyl-imino)acenaphthene). [Cu(NCMe)4]PF6 (50 mg, 0.13 mmol) and Ph3As (93 mg, 0.30 mmol) was stirred in methylene chloride (10 ml) for 2 h. Ph-BIAN (51 mg, 0.15 mmol) was added and stirring was continued for another 2 h. The product was precipitated with pentane. Slow diffusion of diethyl ether into a methylene chloride solution of the product mixture yielded a dark powder and the title compound as colourless crystals. To identify the colourless crystals a single-crystal analysis was performed.

Refinement

The H-atoms were calculated geometrically and refined using a riding model with C—H = 0.93Å and U(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

: View of the title compound with the atom numbering scheme. Displacement ellipsoids for non-H atoms are drawn at the 50% probability level.

Crystal data

[Cu(C18H15As)4]PF6 Z = 6
Mr = 1433.40 F000 = 4332
Trigonal, R3 Cell parameters were determined by indexing 8000 reflections with I/sigma limit 6.0.
Hall symbol: -R 3 Dx = 1.528 Mg m3
a = 14.4025 (10) Å Mo Kα radiation λ = 0.71073 Å
b = 14.4025 (10) Å Cell parameters from 8000 reflections
c = 52.015 (4) Å θ = 2.4–25.9º
α = 90º µ = 2.55 mm1
β = 90º T = 296 K
γ = 120º Prism, light yellow, translucent
V = 9344.1 (12) Å3 0.14 × 0.12 × 0.10 mm

Data collection

Stoe IPDS diffractometer 4049 independent reflections
Radiation source: fine-focus sealed tube 3118 reflections with I > 2σ(I)
Monochromator: graphite Rint = 0.032
T = 296(1) K θmax = 25.9º
rotation scans θmin = 2.4º
Absorption correction: part of the refinement model (ΔF)refined from delta-F (Walker & Stuart, 1983) h = −17→17
Tmin = 0.349, Tmax = 0.769 k = −17→17
23664 measured reflections l = −63→61

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)] = 0.037 H-atom parameters constrained
wR(F2) = 0.097   w = 1/[σ2(Fo2) + (0.P)2] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.001
4049 reflections Δρmax = 1.77 e Å3
254 parameters Δρmin = −0.62 e Å3
Primary atom site location: structure-invariant direct methods Extinction correction: none

Special details

Experimental. Data were collected applying an imaging plate system (Stoe) with the following measurement parameters:Detector distance [mm] 70 Phi movement mode Oscillation Phi incr. [degrees] 1.0 Number of exposures 192 Irradiation / exposure [min] 2.50For a detailed description of the method see: Sheldrick, G.M., Paulus, E. Vertesy, L. & Hahn, F. (1995) Acta Cryst. B51, 89–98.
Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles
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
As1 0.47917 (3) 0.20088 (3) 0.06525 (1) 0.0440 (1)
As2 0.66667 0.33333 0.12958 (1) 0.0398 (1)
Cu1 0.66667 0.33333 0.08144 (1) 0.0466 (2)
C1 0.4361 (3) 0.0520 (3) 0.07350 (6) 0.0448 (10)
C2 0.5099 (3) 0.0188 (3) 0.06918 (8) 0.0610 (14)
C3 0.4877 (4) −0.0818 (4) 0.07706 (10) 0.0771 (19)
C4 0.3929 (4) −0.1499 (3) 0.08911 (9) 0.0730 (16)
C5 0.3189 (4) −0.1186 (3) 0.09291 (9) 0.0699 (16)
C6 0.3402 (3) −0.0175 (3) 0.08519 (7) 0.0564 (12)
C7 0.4540 (3) 0.1926 (3) 0.02816 (6) 0.0491 (11)
C8 0.3857 (4) 0.0974 (4) 0.01602 (8) 0.0779 (18)
C9 0.3650 (6) 0.0970 (5) −0.00996 (10) 0.106 (3)
C10 0.4128 (6) 0.1912 (5) −0.02384 (9) 0.096 (2)
C11 0.4819 (5) 0.2846 (5) −0.01205 (9) 0.082 (2)
C12 0.5020 (3) 0.2858 (3) 0.01399 (7) 0.0604 (12)
C13 0.3514 (3) 0.2028 (3) 0.07735 (6) 0.0457 (10)
C14 0.2602 (3) 0.1674 (4) 0.06245 (8) 0.0648 (14)
C15 0.1694 (4) 0.1644 (4) 0.07263 (9) 0.0786 (19)
C16 0.1697 (4) 0.1970 (4) 0.09752 (9) 0.0730 (17)
C17 0.2590 (4) 0.2334 (4) 0.11206 (8) 0.0699 (16)
C18 0.3503 (3) 0.2367 (3) 0.10222 (7) 0.0584 (12)
C19 0.7988 (3) 0.4342 (3) 0.14716 (6) 0.0420 (10)
C20 0.8947 (3) 0.4451 (3) 0.13850 (7) 0.0541 (11)
C21 0.9898 (3) 0.5153 (3) 0.15034 (9) 0.0653 (16)
C22 0.9904 (4) 0.5749 (4) 0.17108 (9) 0.0732 (17)
C23 0.8955 (4) 0.5649 (4) 0.17971 (9) 0.0786 (17)
C24 0.7999 (3) 0.4955 (3) 0.16784 (7) 0.0620 (14)
P1 0.00000 0.00000 0.00000 0.0713 (7)
F1 0.0013 (5) 0.0885 (4) 0.01719 (9) 0.185 (3)
P2 1.33333 0.66667 0.16667 0.0504 (6)
F2 1.2304 (2) 0.6030 (3) 0.18418 (6) 0.0990 (11)
H2 0.57430 0.06430 0.06100 0.0730*
H3 0.53770 −0.10360 0.07420 0.0930*
H4 0.37920 −0.21700 0.09470 0.0880*
H5 0.25380 −0.16520 0.10070 0.0830*
H6 0.28950 0.00340 0.08790 0.0680*
H8 0.35360 0.03350 0.02530 0.0940*
H9 0.31860 0.03270 −0.01810 0.1270*
H10 0.39760 0.19070 −0.04120 0.1160*
H11 0.51590 0.34790 −0.02150 0.0990*
H12 0.54850 0.35030 0.02200 0.0730*
H14 0.25960 0.14560 0.04560 0.0780*
H15 0.10820 0.14010 0.06260 0.0940*
H16 0.10850 0.19410 0.10430 0.0870*
H17 0.25940 0.25630 0.12880 0.0840*
H18 0.41120 0.26190 0.11240 0.0700*
H20 0.89480 0.40460 0.12460 0.0650*
H21 1.05390 0.52250 0.14430 0.0780*
H22 1.05460 0.62170 0.17920 0.0880*
H23 0.89590 0.60540 0.19370 0.0950*
H24 0.73620 0.48980 0.17370 0.0740*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
As1 0.0427 (2) 0.0399 (2) 0.0462 (2) 0.0183 (2) −0.0025 (1) −0.0001 (1)
As2 0.0426 (2) 0.0426 (2) 0.0341 (3) 0.0213 (1) 0.0000 0.0000
Cu1 0.0483 (3) 0.0483 (3) 0.0431 (4) 0.0241 (1) 0.0000 0.0000
C1 0.0454 (19) 0.0368 (17) 0.0476 (17) 0.0171 (15) −0.0056 (14) −0.0021 (13)
C2 0.051 (2) 0.050 (2) 0.081 (3) 0.0245 (19) 0.0029 (19) 0.0043 (19)
C3 0.079 (3) 0.063 (3) 0.106 (4) 0.048 (3) 0.000 (3) 0.002 (2)
C4 0.087 (3) 0.043 (2) 0.087 (3) 0.031 (2) −0.010 (2) 0.003 (2)
C5 0.064 (3) 0.047 (2) 0.083 (3) 0.016 (2) 0.012 (2) 0.012 (2)
C6 0.050 (2) 0.045 (2) 0.070 (2) 0.0205 (18) 0.0069 (17) 0.0076 (17)
C7 0.049 (2) 0.053 (2) 0.0471 (17) 0.0269 (17) −0.0011 (14) −0.0021 (15)
C8 0.102 (4) 0.061 (3) 0.055 (2) 0.029 (3) −0.014 (2) −0.0080 (19)
C9 0.148 (6) 0.099 (4) 0.065 (3) 0.058 (4) −0.034 (3) −0.032 (3)
C10 0.145 (5) 0.129 (5) 0.047 (2) 0.093 (5) −0.008 (3) −0.002 (3)
C11 0.110 (4) 0.099 (4) 0.061 (3) 0.070 (4) 0.017 (3) 0.024 (3)
C12 0.061 (2) 0.060 (2) 0.060 (2) 0.030 (2) 0.0038 (18) 0.0097 (18)
C13 0.0430 (18) 0.0395 (18) 0.0536 (18) 0.0199 (15) −0.0032 (14) 0.0017 (14)
C14 0.059 (2) 0.080 (3) 0.061 (2) 0.039 (2) −0.0094 (19) −0.009 (2)
C15 0.056 (3) 0.105 (4) 0.085 (3) 0.048 (3) −0.013 (2) −0.004 (3)
C16 0.067 (3) 0.076 (3) 0.087 (3) 0.044 (3) 0.015 (2) 0.010 (2)
C17 0.079 (3) 0.071 (3) 0.063 (2) 0.040 (3) 0.011 (2) −0.002 (2)
C18 0.055 (2) 0.058 (2) 0.058 (2) 0.025 (2) −0.0021 (17) −0.0078 (17)
C19 0.0421 (18) 0.0405 (17) 0.0400 (15) 0.0181 (15) 0.0002 (13) 0.0029 (13)
C20 0.054 (2) 0.058 (2) 0.0539 (19) 0.0306 (19) −0.0005 (16) −0.0032 (16)
C21 0.041 (2) 0.067 (3) 0.088 (3) 0.027 (2) 0.0015 (19) 0.005 (2)
C22 0.054 (3) 0.065 (3) 0.093 (3) 0.024 (2) −0.020 (2) −0.014 (2)
C23 0.067 (3) 0.080 (3) 0.081 (3) 0.031 (3) −0.020 (2) −0.039 (2)
C24 0.051 (2) 0.069 (3) 0.062 (2) 0.027 (2) −0.0027 (17) −0.0179 (19)
P1 0.0817 (12) 0.0817 (12) 0.0507 (13) 0.0409 (6) 0.0000 0.0000
F1 0.229 (6) 0.182 (5) 0.173 (4) 0.124 (5) −0.008 (4) −0.076 (4)
P2 0.0409 (7) 0.0409 (7) 0.0694 (14) 0.0205 (4) 0.0000 0.0000
F2 0.0655 (17) 0.101 (2) 0.117 (2) 0.0315 (17) 0.0315 (16) 0.0196 (18)

Geometric parameters (Å, °)

As1—Cu1 2.5472 (5) C13—C14 1.384 (6)
As1—C1 1.959 (4) C13—C18 1.386 (5)
As1—C7 1.956 (3) C14—C15 1.391 (8)
As1—C13 1.958 (5) C15—C16 1.376 (7)
As2—Cu1 2.5044 (9) C16—C17 1.352 (8)
As2—C19 1.950 (4) C17—C18 1.390 (8)
As2—C19i 1.950 (5) C19—C20 1.385 (7)
As2—C19ii 1.950 (4) C19—C24 1.387 (5)
P1—F1iii 1.549 (8) C20—C21 1.376 (6)
P1—F1iv 1.549 (5) C21—C22 1.376 (7)
P1—F1v 1.549 (7) C22—C23 1.376 (9)
P1—F1vi 1.549 (8) C23—C24 1.378 (7)
P1—F1vii 1.549 (7) C2—H2 0.9300
P1—F1 1.549 (5) C3—H3 0.9300
P2—F2viii 1.584 (5) C4—H4 0.9300
P2—F2 1.584 (3) C5—H5 0.9300
P2—F2ix 1.583 (5) C6—H6 0.9300
P2—F2x 1.585 (3) C8—H8 0.9300
P2—F2xi 1.584 (3) C9—H9 0.9300
P2—F2xii 1.584 (3) C10—H10 0.9300
C1—C2 1.385 (7) C11—H11 0.9300
C1—C6 1.377 (6) C12—H12 0.9300
C2—C3 1.381 (6) C14—H14 0.9300
C3—C4 1.371 (8) C15—H15 0.9300
C4—C5 1.363 (8) C16—H16 0.9300
C5—C6 1.389 (6) C17—H17 0.9300
C7—C8 1.378 (6) C18—H18 0.9300
C7—C12 1.377 (5) C20—H20 0.9300
C8—C9 1.383 (7) C21—H21 0.9300
C9—C10 1.379 (8) C22—H22 0.9300
C10—C11 1.356 (9) C23—H23 0.9300
C11—C12 1.383 (6) C24—H24 0.9300
As1···H2ii 3.1700 C14···H9vi 3.0700
Cu1···H2 3.5700 C19···H24ii 2.6000
Cu1···H12 3.6000 C19···H18ii 2.6700
Cu1···H18 3.6600 C20···H24ii 3.0000
Cu1···H20 3.6800 C20···H18ii 2.8000
Cu1···H2i 3.5700 C21···H22x 2.9700
Cu1···H12i 3.6000 C24···H24ii 3.0700
Cu1···H18i 3.6600 H2···Cu1 3.5700
Cu1···H20i 3.6800 H2···C13i 2.9300
Cu1···H2ii 3.5700 H2···As1i 3.1700
Cu1···H12ii 3.6000 H3···H10xiii 2.5600
Cu1···H18ii 3.6600 H4···H4xiv 2.5300
Cu1···H20ii 3.6800 H4···H4xv 2.5300
F2···C22 3.343 (7) H6···C14 2.9200
F1···H14vii 2.7500 H6···C13 2.6000
F1···H15 2.7100 H8···C1 2.7300
F2···H22 2.6900 H8···C11v 3.0300
C6···C14 3.590 (7) H9···C14v 3.0700
C8···C14 3.455 (7) H10···H3xiii 2.5600
C14···C8 3.455 (7) H12···Cu1 3.6000
C14···C6 3.590 (7) H12···C12ii 3.0000
C18···C19i 3.574 (6) H12···C7ii 2.8000
C18···C20i 3.551 (6) H14···C7 2.6900
C19···C18ii 3.574 (5) H14···C8 2.7200
C20···C24ii 3.590 (6) H14···F1iii 2.7500
C20···C18ii 3.551 (6) H15···F1 2.7100
C22···F2 3.343 (7) H18···C20i 2.8000
C24···C20i 3.590 (7) H18···Cu1 3.6600
C1···H8 2.7300 H18···C19i 2.6700
C1···H20ii 2.8200 H20···C1i 2.8200
C6···H20ii 3.0000 H20···C6i 3.0000
C7···H12i 2.8000 H20···Cu1 3.6800
C7···H14 2.6900 H21···H22x 2.3900
C8···H14 2.7200 H22···F2 2.6900
C11···H8vi 3.0300 H22···C21ix 2.9700
C12···H12i 3.0000 H22···H21ix 2.3900
C13···H6 2.6000 H24···C20i 3.0000
C13···H2ii 2.9300 H24···C24i 3.0700
C14···H6 2.9200 H24···C19i 2.6000
Cu1—As1—C1 112.61 (13) C8—C9—C10 120.5 (5)
Cu1—As1—C7 117.80 (13) C9—C10—C11 119.8 (5)
Cu1—As1—C13 122.35 (11) C10—C11—C12 120.0 (5)
C1—As1—C7 101.64 (15) C7—C12—C11 120.8 (4)
C1—As1—C13 99.19 (17) As1—C13—C18 118.8 (3)
C7—As1—C13 99.85 (17) C14—C13—C18 118.5 (4)
Cu1—As2—C19 117.96 (10) As1—C13—C14 122.7 (3)
Cu1—As2—C19i 117.96 (11) C13—C14—C15 120.2 (4)
Cu1—As2—C19ii 117.96 (10) C14—C15—C16 120.3 (5)
C19—As2—C19i 99.81 (18) C15—C16—C17 119.9 (6)
C19—As2—C19ii 99.81 (18) C16—C17—C18 120.5 (4)
C19i—As2—C19ii 99.8 (2) C13—C18—C17 120.6 (4)
As1—Cu1—As2 109.30 (2) As2—C19—C24 122.3 (4)
As1—Cu1—As1i 109.65 (2) C20—C19—C24 119.1 (4)
As1—Cu1—As1ii 109.65 (2) As2—C19—C20 118.6 (3)
As1i—Cu1—As2 109.30 (2) C19—C20—C21 120.5 (4)
As1ii—Cu1—As2 109.30 (2) C20—C21—C22 120.2 (5)
As1i—Cu1—As1ii 109.65 (2) C21—C22—C23 119.6 (5)
F1vii—P1—F1iv 90.0 (3) C22—C23—C24 120.6 (4)
F1vii—P1—F1v 180.00 C19—C24—C23 119.9 (5)
F1vii—P1—F1vi 90.0 (3) C1—C2—H2 120.00
F1iii—P1—F1iv 90.0 (3) C3—C2—H2 120.00
F1iii—P1—F1v 90.0 (3) C4—C3—H3 120.00
F1iii—P1—F1vi 180.00 C2—C3—H3 120.00
F1iv—P1—F1v 90.0 (3) C3—C4—H4 120.00
F1iv—P1—F1vi 90.0 (3) C5—C4—H4 120.00
F1v—P1—F1vi 90.0 (3) C4—C5—H5 120.00
F1—P1—F1vii 90.0 (3) C6—C5—H5 120.00
F1—P1—F1iii 90.0 (3) C1—C6—H6 120.00
F1—P1—F1iv 180.00 C5—C6—H6 120.00
F1—P1—F1v 90.0 (3) C9—C8—H8 120.00
F1—P1—F1vi 90.0 (3) C7—C8—H8 120.00
F1vii—P1—F1iii 90.0 (3) C8—C9—H9 120.00
F2viii—P2—F2ix 180.00 C10—C9—H9 120.00
F2viii—P2—F2x 89.8 (2) C11—C10—H10 120.00
F2xi—P2—F2xii 89.8 (2) C9—C10—H10 120.00
F2xi—P2—F2ix 89.8 (2) C10—C11—H11 120.00
F2xi—P2—F2x 180.00 C12—C11—H11 120.00
F2xii—P2—F2ix 90.2 (2) C7—C12—H12 120.00
F2xii—P2—F2x 90.2 (2) C11—C12—H12 120.00
F2ix—P2—F2x 90.2 (2) C15—C14—H14 120.00
F2viii—P2—F2xii 89.8 (2) C13—C14—H14 120.00
F2—P2—F2viii 90.2 (2) C16—C15—H15 120.00
F2—P2—F2xi 90.2 (2) C14—C15—H15 120.00
F2—P2—F2xii 180.00 C15—C16—H16 120.00
F2—P2—F2ix 89.8 (2) C17—C16—H16 120.00
F2—P2—F2x 89.8 (2) C16—C17—H17 120.00
F2viii—P2—F2xi 90.2 (2) C18—C17—H17 120.00
C2—C1—C6 119.0 (4) C17—C18—H18 120.00
As1—C1—C2 117.7 (3) C13—C18—H18 120.00
As1—C1—C6 123.1 (3) C19—C20—H20 120.00
C1—C2—C3 120.0 (4) C21—C20—H20 120.00
C2—C3—C4 120.8 (5) C22—C21—H21 120.00
C3—C4—C5 119.6 (4) C20—C21—H21 120.00
C4—C5—C6 120.4 (4) C21—C22—H22 120.00
C1—C6—C5 120.3 (5) C23—C22—H22 120.00
As1—C7—C8 122.1 (3) C24—C23—H23 120.00
C8—C7—C12 119.1 (3) C22—C23—H23 120.00
As1—C7—C12 118.8 (3) C23—C24—H24 120.00
C7—C8—C9 119.8 (5) C19—C24—H24 120.00
C1—As1—Cu1—As2 −66.60 (12) Cu1—As2—C19—C24 134.7 (3)
C7—As1—Cu1—As2 175.59 (14) C19i—As2—C19—C24 5.6 (3)
C13—As1—Cu1—As2 51.33 (12) C19ii—As2—C19—C24 −96.2 (3)
C1—As1—Cu1—As1i 53.18 (12) As1—C1—C2—C3 173.5 (3)
C7—As1—Cu1—As1i −64.63 (15) As1—C1—C6—C5 −173.4 (3)
C13—As1—Cu1—As1i 171.12 (12) C2—C1—C6—C5 1.1 (6)
C1—As1—Cu1—As1ii 173.61 (12) C6—C1—C2—C3 −1.4 (6)
C7—As1—Cu1—As1ii 55.80 (15) C1—C2—C3—C4 0.2 (7)
C13—As1—Cu1—As1ii −68.45 (13) C2—C3—C4—C5 1.3 (7)
C13—As1—C1—C2 −176.1 (3) C3—C4—C5—C6 −1.5 (7)
Cu1—As1—C1—C6 129.4 (3) C4—C5—C6—C1 0.3 (6)
Cu1—As1—C13—C14 151.9 (3) C12—C7—C8—C9 −1.1 (9)
C1—As1—C13—C14 −83.8 (4) As1—C7—C8—C9 175.6 (6)
C7—As1—C13—C14 19.8 (4) C8—C7—C12—C11 0.3 (8)
Cu1—As1—C1—C2 −45.2 (3) As1—C7—C12—C11 −176.5 (5)
C7—As1—C1—C2 81.8 (3) C7—C8—C9—C10 0.4 (12)
C13—As1—C7—C8 −80.5 (5) C8—C9—C10—C11 1.1 (13)
Cu1—As1—C7—C12 −38.7 (4) C9—C10—C11—C12 −1.8 (13)
C7—As1—C1—C6 −103.6 (3) C10—C11—C12—C7 1.2 (10)
C13—As1—C1—C6 −1.5 (3) As1—C13—C14—C15 176.0 (4)
C13—As1—C7—C12 96.2 (4) C14—C13—C18—C17 1.1 (6)
Cu1—As1—C7—C8 144.6 (4) C18—C13—C14—C15 −1.2 (7)
C1—As1—C7—C8 21.1 (5) As1—C13—C18—C17 −176.2 (3)
C1—As1—C13—C18 93.4 (3) C13—C14—C15—C16 0.3 (7)
Cu1—As1—C13—C18 −30.9 (3) C14—C15—C16—C17 0.8 (8)
C1—As1—C7—C12 −162.2 (4) C15—C16—C17—C18 −1.0 (7)
C7—As1—C13—C18 −163.0 (3) C16—C17—C18—C13 0.0 (7)
C19ii—As2—C19—C20 84.2 (3) As2—C19—C20—C21 −180.0 (3)
C19ii—As2—Cu1—As1 63.5 (2) C24—C19—C20—C21 0.4 (6)
C19—As2—Cu1—As1 −176.49 (15) As2—C19—C24—C23 179.4 (3)
C19—As2—Cu1—As1ii −56.49 (15) C20—C19—C24—C23 −1.0 (6)
C19i—As2—Cu1—As1 −56.49 (17) C19—C20—C21—C22 0.5 (6)
C19—As2—Cu1—As1i 63.51 (15) C20—C21—C22—C23 −0.8 (7)
Cu1—As2—C19—C20 −44.9 (3) C21—C22—C23—C24 0.2 (7)
C19i—As2—C19—C20 −174.0 (3) C22—C23—C24—C19 0.7 (7)

Symmetry codes: (i) −y+1, xy, z; (ii) −x+y+1, −x+1, z; (iii) −x+y, −x, z; (iv) −x, −y, −z; (v) y, −x+y, −z; (vi) xy, x, −z; (vii) −y, xy, z; (viii) −y+2, xy, z; (ix) y+2/3, −x+y+4/3, −z+1/3; (x) xy+2/3, x−2/3, −z+1/3; (xi) −x+y+2, −x+2, z; (xii) −x+8/3, −y+4/3, −z+1/3; (xiii) −x+1, −y, −z; (xiv) −y, xy−1, z; (xv) −x+y+1, −x, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2651).

References

  1. Altomare, A., Burla, M. C., Camalli, M., Cascarano, G. L., Giacovazzo, C., Guagliardi, A., Moliterni, A. G. G., Polidori, G. & Spagna, R. (1999). J. Appl. Cryst.32, 115–119.
  2. Bowmaker, G. A., Healy, P. C., Engelhardt, L. M., Kildea, J. D., Skelton, B. W. & White, A. H. (1990). Aust. J. Chem.43, 1697–1705.
  3. Engelhardt, L. M., Pakawatchai, C., White, A. H. & Healy, P. C. (1985). J. Chem. Soc. Dalton Trans. pp. 125–133.
  4. Sheldrick, G. M. (1997). SHELXL97 University of Göttingen, Germany.
  5. Spek, A. L. (2003). J. Appl. Cryst.36, 7–13.
  6. Stoe (1998). IPDS Software Version 2.89. Stoe & Cie GmbH, Darmstadt, Germany.
  7. Walker, N. & Stuart, D. (1983). Acta Cryst. A39, 158–166.

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/S1600536807064458/bt2651sup1.cif

e-64-00m99-sup1.cif (27.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807064458/bt2651Isup2.hkl

e-64-00m99-Isup2.hkl (198.8KB, 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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