Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Nov 24;68(Pt 12):m1508–m1509. doi: 10.1107/S1600536812046971

trans-Dichloridobis{tris­[4-(trifluoro­methyl)phen­yl]phosphane-κP}palla­dium(II) dichloro­methane monosolvate

Wade L Davis a, Alfred Muller a,*
PMCID: PMC3588757  PMID: 23468722

Abstract

The title compound, [PdCl2(C21H12F9P)2]·CH2Cl2, crystallizes with two independent complex molecules (each having the PdII atom situated on an inversion centre) and a dichloro­methane molecule in the asymmetric unit. The independent PdII atoms are in perfectly linear orientations of the ligands in mutually trans positions, but distortions of the Cl—Pd—P angles ranging from 86.151 (19) to 93.849 (19)° are evident. The effective cone angles for the tris­[4-(trifluoro­meth­yl)phen­yl]phosphane ligand were calculated to be 159 and 161°. In the crystal, weak C—H⋯Cl/F inter­actions create a three-dimensional supramolecular network. Loose packing at two of the –CF3 groups resulted in large thermal vibrations which were treated as two-component disorders [occupancy ratios 0.50:0.50 and 0.628 (15):0.372 (15)].

Related literature  

For background to catalysis of palladium compounds, see: Bedford et al. (2004). For a description of the Cambridge Structural Database, see: Allen (2002). For background to cone angles, see: Tolman (1977); Otto (2001). For details of the conformational fit between mol­ecules using Mercury, see: Macrae et al. (2006); Weng et al. (2008a ,b ).graphic file with name e-68-m1508-scheme1.jpg

Experimental  

Crystal data  

  • [PdCl2(C21H12F9P)2]·CH2Cl2

  • M r = 1194.78

  • Triclinic, Inline graphic

  • a = 12.1491 (10) Å

  • b = 14.0203 (13) Å

  • c = 14.4334 (13) Å

  • α = 72.764 (2)°

  • β = 78.362 (2)°

  • γ = 75.545 (2)°

  • V = 2252.0 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.83 mm−1

  • T = 100 K

  • 0.34 × 0.31 × 0.25 mm

Data collection  

  • Bruker APEX DUO 4K CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2008) T min = 0.766, T max = 0.820

  • 48517 measured reflections

  • 11209 independent reflections

  • 9475 reflections with I > 2σ(I)

  • R int = 0.03

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.032

  • wR(F 2) = 0.077

  • S = 1.02

  • 11209 reflections

  • 680 parameters

  • 116 restraints

  • H-atom parameters constrained

  • Δρmax = 1.14 e Å−3

  • Δρmin = −0.85 e Å−3

Data collection: APEX2 (Bruker, 2011); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT and XPREP (Bruker, 2008); program(s) used to solve structure: SIR97 (Altomare et al., 1999); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: publCIF (Westrip, 2010) and WinGX (Farrugia, 2012).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812046971/zq2189sup1.cif

e-68-m1508-sup1.cif (51.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046971/zq2189Isup2.hkl

e-68-m1508-Isup2.hkl (537KB, 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
C12—H12⋯Cl3 0.95 2.78 3.468 (2) 130
C7—H7B⋯Cl4 0.99 2.54 3.510 (4) 165
C65—H65⋯F6i 0.95 2.55 3.457 (3) 160
C7—H7A⋯Cl3ii 0.99 2.57 3.550 (5) 169
C15—H15⋯F17A iii 0.95 2.52 3.341 (6) 144
C33—H33⋯F10B 0.95 2.53 3.435 (4) 159

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

Acknowledgments

Financial assistance from the Research Fund of the University of Johannesburg is gratefully acknowledged.

supplementary crystallographic information

Comment

Complexes involving palladium metal centres are amongst some of the most popular catalytic precursors in organic synthesis due to their catalytic abilities. They are used in carbon-carbon bond formation reactions, e.g. the Heck, Stille and Suzuki reactions (Bedford et al., 2004). [PdCl2(L)2] (L = tertiary phosphine, arsine or stibine) complexes can conveniently be prepared by the substitution of 1,5-cyclooctadiene (COD) from [PdCl2(COD)]. Reported here is the product of the reaction with tris[4-(trifluoromethyl)phenyl]phosphane ligand.

The title compound (Fig.1 and 2) crystallizes in the triclinic space group P1 (Z = 2), with the independent Pd atoms on inversion centres and each accompanied by a dichloromethane solvate molecule. Each pair of equivalent ligands is in a mutually trans orientation and the geometry is, therefore, perfectly linear with only slight distortions in P1—Pd1—Cl3, P2—Pd2—Cl4 angles of 87.299 (19), 92.701 (19), 93.849 (19) and 86.151 (19)°, respectively. The Pd1—P1, Pd2—P2, Pd1—Cl3 and Pd2—Cl4 bond distances of 2.3174 (5), 2.3130 (6), 2.2897 (6) and 2.2871 (6) Å, respectively fit well into the typical range for complexes of this kind (Allen, 2002). The difference between the two Pd molecules in the asymmetric unit can be illustrated by superimposing their coordination sphere coordinates (see Fig.3) using Mercury (Macrae et al., 2006; Weng et al., 2008a; Weng et al., 2008b). This shows good fit between the two palladium molecules except in some of the CF3 regions.

To describe the steric demand of the phosphane ligands the Tolman cone angle (Tolman, 1977) is still the most commonly used model. Applying this model to the geometry obtained from the title compound (and adjusting the Pd—P bond distance to 2.28 Å) we calculated effective cone angles (Otto, 2001) of 161° and 159° for P1 and P2, respectively. These values are marginally larger than the average cone angle obtained from structures of this phosphane ligand in literature. Data extracted from the Cambridge Structural Database (Allen, 2002) shows an average cone angle of 154° for the phosphane from 16 hits, containing 17 useable observations with a standard deviation of ±4° and a spread from 149° to 165°. In the crystal, weak C—H···Cl/F interactions are observed with some of the CF3 groups showing disorder due to loose packing in these regions.

Experimental

Tris[4-(trifluoromethyl)phenyl]phosphane (10 mg, 0.021 mmol) was dissolved in CH2Cl2 (5 cm3). A solution of [Pd(COD)Cl2] (3.10 mg, 0.011 mmol) in CH2Cl2 (5 cm3) was added to the phosphane solution. The mixture was stirred for 2hr at room temperature, after which the solution was left to crystallize. Orange crystals of the title compound suitable for X-ray diffraction studies were obtained in 60% yield.

1H NMR (CDCl3, 400 MHz): δ (p.p.m.) 7.67 - 7.72 (m, 12H); 7.74 - 7.81 (m, 12 H).

31P NMR (CDCl3, 162.0 MHz): δ (p.p.m.) 23.11 (s, 1P).

FTIR (cm-1): 2360, 1610, 1398, 1321, 1168, 1121, 1060, 1015, 955, 828, 706, 696, 633.

Refinement

The aromatic and methylene H atoms were placed in geometrically idealized positions (C—H = 0.95 and 0.99 Å) and allowed to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C). Two of the CF3 groups for molecule 2 showed large thermal vibrations and were treated to disorder refinement. The disorder models for these two CF3 groups were significantly different with one of the carbon atoms (C6) also modeled disordered. To keep refinement stable ellipsoid restraints (SIMU and DELU) were employed and their default refinement parameters adjusted (see _iucr_refine_instructions_details). Initially the occupancies of the two components of both CF3 groups were linked to free variables to refine to unity. The CF3 containing C4 showed an almost 50:50 distribution and in the final cycles was constrained to this. The CF3 containing C6 refined to a ratio of 0.628 (15):0.372 (15).

Figures

Fig. 1.

Fig. 1.

A view of molecule 1 of the title complex, showing the atom-numbering scheme and 50% probability displacement ellipsoids. Accented lettering indicate atoms generated by symmetry code (i) = -x,-y,-z. H atoms omitted for clarity.

Fig. 2.

Fig. 2.

A view of molecule 2 and the dichloromethane solvate of the title complex, showing the atom-numbering scheme and 50% probability displacement ellipsoids. Accented lettering indicate atoms generated by symmetry code (ii) = 1 - x,-y,1 - z. H atoms and B component of disordered atoms omitted for clarity.

Fig. 3.

Fig. 3.

Conformational similarity between molecule 1 (blue) and molecule 2 (red) of the title complex. The root mean squared deviation; RMSD = 0.0279 Å.

Crystal data

[PdCl2(C21H12F9P)2]·CH2Cl2 Z = 2
Mr = 1194.78 F(000) = 1180
Triclinic, P1 Dx = 1.762 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 12.1491 (10) Å Cell parameters from 9887 reflections
b = 14.0203 (13) Å θ = 2.9–28.3°
c = 14.4334 (13) Å µ = 0.83 mm1
α = 72.764 (2)° T = 100 K
β = 78.362 (2)° Cuboid, yellow
γ = 75.545 (2)° 0.34 × 0.31 × 0.25 mm
V = 2252.0 (3) Å3

Data collection

Bruker APEX DUO 4K CCD diffractometer 11209 independent reflections
Radiation source: sealed tube 9475 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.03
Detector resolution: 8.4 pixels mm-1 θmax = 28.3°, θmin = 1.5°
φ and ω scans h = −16→16
Absorption correction: multi-scan (SADABS; Bruker, 2008) k = −18→18
Tmin = 0.766, Tmax = 0.820 l = −19→19
48517 measured 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)] = 0.032 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.077 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0273P)2 + 3.2668P] where P = (Fo2 + 2Fc2)/3
11209 reflections (Δ/σ)max = 0.001
680 parameters Δρmax = 1.14 e Å3
116 restraints Δρmin = −0.85 e Å3

Special details

Experimental. The intensity data was collected on a Bruker Apex DUO 4 K CCD diffractometer using an exposure time of 2 s/frame. A total of 2216 frames were collected with a frame width of 0.5° covering up to θ = 28.31° with 99.8% completeness accomplished.
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 Occ. (<1)
C1 −0.6245 (2) 0.0991 (2) 0.0983 (2) 0.0318 (6)
C2 −0.1366 (2) 0.4058 (2) −0.46255 (19) 0.0303 (6)
C3 −0.0591 (2) 0.4411 (2) 0.18078 (19) 0.0284 (5)
C4 0.3291 (2) 0.4352 (2) 0.10003 (18) 0.0267 (4)
C5 1.0812 (2) 0.0902 (2) 0.34731 (18) 0.0281 (5)
C7 0.2146 (5) 0.1811 (3) 0.7105 (2) 0.0708 (13)
H7A 0.159 0.1363 0.7429 0.085*
H7B 0.2912 0.1363 0.7032 0.085*
C6A 0.4634 (7) 0.4207 (7) 0.7336 (6) 0.0304 (8) 0.628 (15)
F16A 0.5626 (4) 0.4237 (5) 0.7608 (7) 0.0519 (17) 0.628 (15)
F17A 0.3961 (7) 0.3874 (3) 0.8166 (3) 0.0458 (12) 0.628 (15)
F18A 0.4156 (7) 0.5196 (12) 0.6939 (14) 0.0361 (14) 0.628 (15)
C6B 0.4798 (11) 0.4328 (12) 0.7194 (9) 0.0276 (11) 0.372 (15)
F16B 0.5757 (5) 0.4637 (8) 0.7107 (9) 0.0412 (19) 0.372 (15)
F17B 0.4512 (12) 0.3887 (6) 0.8140 (5) 0.0447 (18) 0.372 (15)
F18B 0.3952 (12) 0.514 (2) 0.700 (2) 0.0319 (18) 0.372 (15)
C11 −0.27757 (17) 0.13693 (16) −0.00228 (15) 0.0157 (4)
C12 −0.30036 (19) 0.04677 (17) 0.06399 (16) 0.0198 (4)
H12 −0.2387 −0.0058 0.0881 0.024*
C13 −0.4131 (2) 0.03313 (19) 0.09514 (17) 0.0231 (5)
H13 −0.4282 −0.0283 0.1407 0.028*
C14 −0.50253 (19) 0.10928 (19) 0.05941 (17) 0.0226 (5)
C15 −0.48108 (19) 0.19894 (18) −0.00889 (18) 0.0233 (5)
H15 −0.5429 0.2506 −0.034 0.028*
C16 −0.36857 (19) 0.21229 (17) −0.03999 (17) 0.0204 (4)
H16 −0.3535 0.2729 −0.0871 0.024*
C21 −0.12624 (17) 0.22880 (16) −0.16527 (15) 0.0149 (4)
C22 −0.15437 (18) 0.18948 (16) −0.23388 (16) 0.0173 (4)
H22 −0.1722 0.1235 −0.2143 0.021*
C23 −0.15639 (18) 0.24660 (17) −0.33047 (16) 0.0187 (4)
H23 −0.175 0.2197 −0.3772 0.022*
C24 −0.13104 (19) 0.34358 (17) −0.35855 (16) 0.0198 (4)
C25 −0.1002 (2) 0.38204 (18) −0.29173 (17) 0.0238 (5)
H25 −0.0809 0.4475 −0.3118 0.029*
C26 −0.0975 (2) 0.32466 (17) −0.19515 (17) 0.0207 (4)
H26 −0.076 0.3509 −0.1493 0.025*
C31 −0.11086 (18) 0.24085 (16) 0.02702 (15) 0.0153 (4)
C32 −0.00019 (19) 0.24363 (18) 0.03740 (18) 0.0228 (5)
H32 0.0639 0.2007 0.0105 0.027*
C33 0.0168 (2) 0.30858 (19) 0.08666 (18) 0.0251 (5)
H33 0.0924 0.3107 0.093 0.03*
C34 −0.0771 (2) 0.37070 (17) 0.12684 (16) 0.0195 (4)
C35 −0.18652 (19) 0.36912 (18) 0.11652 (17) 0.0207 (4)
H35 −0.2504 0.4125 0.1432 0.025*
C36 −0.20374 (18) 0.30376 (17) 0.06670 (17) 0.0197 (4)
H36 −0.2795 0.3024 0.06 0.024*
C41 0.49547 (18) 0.23512 (16) 0.34096 (15) 0.0156 (4)
C42 0.37650 (19) 0.25054 (18) 0.34546 (17) 0.0220 (5)
H42 0.3328 0.2164 0.4023 0.026*
C43 0.32186 (19) 0.31526 (19) 0.26759 (17) 0.0229 (5)
H43 0.2409 0.3265 0.2713 0.027*
C44 0.38674 (19) 0.36354 (17) 0.18416 (16) 0.0185 (4)
C45 0.50467 (19) 0.34654 (17) 0.17821 (16) 0.0203 (4)
H45 0.5484 0.3791 0.1205 0.024*
C46 0.55962 (18) 0.28196 (17) 0.25635 (16) 0.0194 (4)
H46 0.6408 0.2699 0.2518 0.023*
C51 0.71490 (17) 0.13601 (16) 0.41710 (15) 0.0147 (4)
C52 0.77923 (18) 0.04078 (17) 0.40947 (16) 0.0180 (4)
H52 0.7416 −0.0139 0.419 0.022*
C53 0.89861 (19) 0.02496 (18) 0.38793 (16) 0.0201 (4)
H53 0.9421 −0.0402 0.3827 0.024*
C54 0.95330 (18) 0.10452 (18) 0.37429 (16) 0.0200 (4)
C55 0.8901 (2) 0.20013 (19) 0.38200 (17) 0.0234 (5)
H55 0.9281 0.2545 0.3726 0.028*
C56 0.77117 (19) 0.21581 (17) 0.40352 (17) 0.0205 (4)
H56 0.728 0.2809 0.409 0.025*
C61 0.52760 (17) 0.23591 (16) 0.53204 (15) 0.0153 (4)
C62 0.57533 (18) 0.20004 (17) 0.61943 (16) 0.0181 (4)
H62 0.6222 0.1337 0.6348 0.022*
C63 0.55443 (19) 0.26092 (18) 0.68380 (17) 0.0212 (4)
H63 0.5861 0.2362 0.7436 0.025*
C64 0.4868 (2) 0.35857 (18) 0.66035 (18) 0.0225 (4)
C65 0.4378 (2) 0.39403 (18) 0.57491 (19) 0.0265 (5)
H65 0.3902 0.4601 0.5602 0.032*
C66 0.4581 (2) 0.33302 (18) 0.51059 (18) 0.0233 (5)
H66 0.4245 0.3575 0.4518 0.028*
F1 −0.69349 (13) 0.13989 (14) 0.02873 (14) 0.0442 (4)
F2 −0.63601 (13) 0.00201 (13) 0.13737 (12) 0.0388 (4)
F3 −0.66742 (15) 0.14722 (18) 0.16893 (16) 0.0619 (6)
F4 −0.1467 (2) 0.50458 (13) −0.47281 (13) 0.0570 (6)
F5 −0.04432 (16) 0.37665 (16) −0.52398 (12) 0.0494 (5)
F6 −0.22635 (15) 0.39581 (12) −0.49792 (12) 0.0378 (4)
F7 −0.15025 (15) 0.46546 (15) 0.24452 (14) 0.0475 (5)
F8 0.02798 (14) 0.39949 (14) 0.23403 (12) 0.0388 (4)
F9 −0.0348 (2) 0.52766 (14) 0.12020 (14) 0.0581 (6)
F13 1.12727 (13) 0.13753 (13) 0.39375 (13) 0.0395 (4)
F14 1.13493 (12) −0.00744 (13) 0.36863 (13) 0.0370 (4)
F15 1.11021 (14) 0.12869 (19) 0.25188 (12) 0.0627 (7)
P1 −0.12923 (4) 0.15375 (4) −0.03807 (4) 0.01399 (10)
P2 0.55964 (4) 0.15397 (4) 0.44843 (4) 0.01338 (10)
Cl1 0.18015 (7) 0.24502 (7) 0.59502 (6) 0.0509 (2)
Cl2 0.21710 (9) 0.25246 (9) 0.78749 (8) 0.0671 (3)
Cl3 −0.04796 (5) 0.00495 (4) 0.16053 (4) 0.02532 (12)
Cl4 0.46271 (5) 0.00177 (4) 0.66133 (4) 0.02431 (12)
Pd1 0 0 0 0.01447 (5)
Pd2 0.5 0 0.5 0.01233 (5)
F10A 0.3811 (5) 0.4275 (4) 0.0137 (3) 0.0651 (14) 0.5
F11A 0.3409 (4) 0.5371 (3) 0.0914 (3) 0.0521 (9) 0.5
F12A 0.2217 (3) 0.4472 (4) 0.1057 (4) 0.0647 (13) 0.5
F10B 0.2741 (4) 0.3792 (3) 0.0638 (3) 0.0485 (9) 0.5
F11B 0.2484 (5) 0.5026 (4) 0.1261 (3) 0.0696 (13) 0.5
F12B 0.3964 (4) 0.4703 (4) 0.0266 (4) 0.0546 (12) 0.5

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0218 (12) 0.0436 (15) 0.0402 (15) −0.0142 (11) 0.0053 (10) −0.0261 (13)
C2 0.0418 (15) 0.0267 (13) 0.0249 (13) −0.0135 (11) −0.0113 (11) −0.0006 (10)
C3 0.0343 (13) 0.0273 (12) 0.0287 (13) −0.0119 (10) −0.0062 (11) −0.0085 (10)
C4 0.0243 (9) 0.0319 (11) 0.0202 (9) −0.0003 (8) −0.0044 (8) −0.0049 (9)
C5 0.0177 (11) 0.0429 (15) 0.0210 (12) −0.0082 (10) −0.0016 (9) −0.0032 (11)
C7 0.130 (4) 0.0336 (17) 0.0309 (17) 0.007 (2) −0.004 (2) −0.0063 (14)
C6A 0.0347 (19) 0.0256 (18) 0.036 (2) 0.0015 (17) −0.0091 (14) −0.0192 (14)
F16A 0.0510 (17) 0.049 (3) 0.076 (4) 0.0070 (16) −0.033 (2) −0.045 (3)
F17A 0.071 (3) 0.0403 (17) 0.0263 (12) −0.002 (2) −0.0015 (16) −0.0193 (11)
F18A 0.045 (3) 0.0232 (16) 0.044 (3) 0.002 (3) −0.009 (3) −0.0198 (12)
C6B 0.030 (2) 0.026 (3) 0.031 (2) −0.0021 (17) −0.005 (2) −0.0170 (18)
F16B 0.035 (2) 0.042 (4) 0.062 (5) −0.0056 (19) −0.013 (2) −0.035 (3)
F17B 0.070 (5) 0.038 (3) 0.0276 (16) −0.004 (3) −0.006 (3) −0.0173 (16)
F18B 0.033 (3) 0.027 (3) 0.039 (4) 0.001 (3) −0.003 (4) −0.021 (2)
C11 0.0152 (9) 0.0195 (10) 0.0146 (10) −0.0041 (8) −0.0008 (7) −0.0081 (8)
C12 0.0218 (10) 0.0209 (11) 0.0158 (10) −0.0040 (9) −0.0019 (8) −0.0040 (8)
C13 0.0274 (12) 0.0268 (12) 0.0172 (11) −0.0129 (10) 0.0031 (9) −0.0068 (9)
C14 0.0190 (10) 0.0316 (12) 0.0239 (11) −0.0094 (9) 0.0036 (9) −0.0181 (10)
C15 0.0162 (10) 0.0251 (12) 0.0307 (13) −0.0012 (9) −0.0023 (9) −0.0133 (10)
C16 0.0192 (10) 0.0179 (10) 0.0247 (11) −0.0037 (8) −0.0025 (9) −0.0069 (9)
C21 0.0126 (9) 0.0153 (9) 0.0155 (10) −0.0004 (7) −0.0017 (7) −0.0041 (8)
C22 0.0168 (10) 0.0157 (10) 0.0203 (10) −0.0041 (8) −0.0043 (8) −0.0040 (8)
C23 0.0192 (10) 0.0210 (11) 0.0183 (10) −0.0055 (8) −0.0056 (8) −0.0054 (9)
C24 0.0209 (10) 0.0190 (10) 0.0189 (11) −0.0051 (8) −0.0046 (8) −0.0020 (9)
C25 0.0333 (13) 0.0188 (11) 0.0213 (11) −0.0119 (9) −0.0036 (10) −0.0027 (9)
C26 0.0257 (11) 0.0207 (11) 0.0190 (11) −0.0082 (9) −0.0033 (9) −0.0068 (9)
C31 0.0170 (9) 0.0153 (9) 0.0136 (9) −0.0030 (8) −0.0026 (8) −0.0036 (8)
C32 0.0158 (10) 0.0266 (12) 0.0277 (12) −0.0016 (9) −0.0026 (9) −0.0120 (10)
C33 0.0179 (10) 0.0302 (13) 0.0313 (13) −0.0071 (9) −0.0064 (9) −0.0104 (10)
C34 0.0257 (11) 0.0188 (10) 0.0158 (10) −0.0093 (9) −0.0022 (8) −0.0037 (8)
C35 0.0196 (10) 0.0227 (11) 0.0220 (11) −0.0039 (9) 0.0004 (8) −0.0115 (9)
C36 0.0147 (9) 0.0235 (11) 0.0239 (11) −0.0025 (8) −0.0022 (8) −0.0121 (9)
C41 0.0182 (10) 0.0136 (9) 0.0152 (10) −0.0037 (8) −0.0027 (8) −0.0035 (8)
C42 0.0188 (10) 0.0282 (12) 0.0180 (11) −0.0096 (9) −0.0006 (8) −0.0018 (9)
C43 0.0166 (10) 0.0290 (12) 0.0232 (11) −0.0067 (9) −0.0038 (9) −0.0047 (10)
C44 0.0220 (10) 0.0181 (10) 0.0162 (10) −0.0030 (8) −0.0038 (8) −0.0059 (8)
C45 0.0187 (10) 0.0218 (11) 0.0159 (10) −0.0029 (8) 0.0011 (8) −0.0017 (9)
C46 0.0158 (10) 0.0218 (11) 0.0185 (10) −0.0038 (8) −0.0001 (8) −0.0035 (9)
C51 0.0145 (9) 0.0174 (10) 0.0116 (9) −0.0057 (8) −0.0002 (7) −0.0020 (8)
C52 0.0186 (10) 0.0184 (10) 0.0169 (10) −0.0055 (8) 0.0001 (8) −0.0045 (8)
C53 0.0184 (10) 0.0223 (11) 0.0173 (10) −0.0014 (8) −0.0001 (8) −0.0054 (9)
C54 0.0148 (10) 0.0301 (12) 0.0136 (10) −0.0064 (9) −0.0005 (8) −0.0028 (9)
C55 0.0217 (11) 0.0265 (12) 0.0235 (11) −0.0123 (9) −0.0019 (9) −0.0035 (9)
C56 0.0206 (10) 0.0177 (10) 0.0234 (11) −0.0055 (8) −0.0024 (9) −0.0048 (9)
C61 0.0151 (9) 0.0159 (10) 0.0166 (10) −0.0058 (8) 0.0001 (8) −0.0061 (8)
C62 0.0165 (10) 0.0171 (10) 0.0218 (11) −0.0023 (8) −0.0037 (8) −0.0066 (8)
C63 0.0206 (10) 0.0247 (11) 0.0215 (11) −0.0025 (9) −0.0058 (9) −0.0104 (9)
C64 0.0215 (10) 0.0222 (9) 0.0278 (10) −0.0024 (8) −0.0033 (8) −0.0141 (8)
C65 0.0288 (12) 0.0183 (11) 0.0334 (13) 0.0040 (9) −0.0100 (10) −0.0117 (10)
C66 0.0260 (11) 0.0201 (11) 0.0240 (12) 0.0001 (9) −0.0082 (9) −0.0070 (9)
F1 0.0203 (7) 0.0501 (10) 0.0642 (12) −0.0100 (7) −0.0067 (8) −0.0149 (9)
F2 0.0314 (8) 0.0481 (10) 0.0433 (9) −0.0260 (7) 0.0036 (7) −0.0121 (8)
F3 0.0365 (10) 0.0993 (17) 0.0772 (14) −0.0365 (10) 0.0311 (9) −0.0708 (13)
F4 0.1168 (18) 0.0246 (8) 0.0369 (10) −0.0290 (10) −0.0353 (11) 0.0097 (7)
F5 0.0493 (10) 0.0729 (13) 0.0185 (8) −0.0178 (10) −0.0010 (7) 0.0010 (8)
F6 0.0475 (9) 0.0352 (9) 0.0324 (8) −0.0108 (7) −0.0241 (7) 0.0032 (7)
F7 0.0410 (9) 0.0617 (12) 0.0588 (12) −0.0089 (9) −0.0033 (8) −0.0473 (10)
F8 0.0395 (9) 0.0510 (10) 0.0386 (9) −0.0146 (8) −0.0154 (7) −0.0194 (8)
F9 0.1088 (17) 0.0348 (10) 0.0461 (11) −0.0419 (11) −0.0261 (11) −0.0006 (8)
F13 0.0216 (7) 0.0422 (9) 0.0590 (11) −0.0112 (7) −0.0112 (7) −0.0119 (8)
F14 0.0181 (7) 0.0436 (9) 0.0507 (10) 0.0020 (6) −0.0041 (7) −0.0215 (8)
F15 0.0218 (8) 0.1211 (19) 0.0235 (8) −0.0156 (10) 0.0034 (7) 0.0101 (10)
P1 0.0127 (2) 0.0144 (2) 0.0142 (2) −0.00056 (19) −0.00135 (19) −0.0049 (2)
P2 0.0141 (2) 0.0137 (2) 0.0128 (2) −0.00480 (19) −0.00022 (19) −0.00356 (19)
Cl1 0.0465 (4) 0.0494 (5) 0.0441 (4) 0.0040 (4) −0.0071 (3) −0.0042 (4)
Cl2 0.0607 (6) 0.0907 (8) 0.0635 (6) −0.0249 (5) −0.0045 (5) −0.0351 (6)
Cl3 0.0308 (3) 0.0253 (3) 0.0136 (2) 0.0078 (2) −0.0033 (2) −0.0067 (2)
Cl4 0.0412 (3) 0.0232 (3) 0.0120 (2) −0.0157 (2) 0.0024 (2) −0.0062 (2)
Pd1 0.01427 (10) 0.01495 (11) 0.01231 (10) 0.00138 (8) −0.00132 (8) −0.00470 (8)
Pd2 0.01413 (10) 0.01324 (10) 0.01027 (10) −0.00574 (8) 0.00068 (8) −0.00314 (8)
F10A 0.082 (3) 0.067 (3) 0.0178 (14) 0.042 (2) −0.0129 (17) −0.013 (2)
F11A 0.077 (3) 0.0268 (13) 0.054 (2) −0.0044 (15) −0.040 (2) 0.0026 (14)
F12A 0.0296 (12) 0.088 (3) 0.052 (2) −0.0220 (18) −0.0237 (14) 0.039 (2)
F10B 0.055 (2) 0.050 (2) 0.046 (2) −0.0195 (15) −0.0381 (17) 0.0079 (15)
F11B 0.081 (3) 0.062 (3) 0.039 (2) 0.051 (2) −0.0252 (18) −0.0162 (19)
F12B 0.0292 (16) 0.076 (3) 0.037 (2) −0.0215 (18) −0.0146 (12) 0.033 (2)

Geometric parameters (Å, º)

C1—F3 1.336 (3) C25—H25 0.95
C1—F1 1.340 (3) C26—H26 0.95
C1—F2 1.341 (3) C31—C36 1.386 (3)
C1—C14 1.501 (3) C31—C32 1.394 (3)
C2—F4 1.325 (3) C31—P1 1.823 (2)
C2—F5 1.340 (3) C32—C33 1.383 (3)
C2—F6 1.346 (3) C32—H32 0.95
C2—C24 1.501 (3) C33—C34 1.390 (3)
C3—F9 1.330 (3) C33—H33 0.95
C3—F7 1.333 (3) C34—C35 1.374 (3)
C3—F8 1.343 (3) C35—C36 1.396 (3)
C3—C34 1.504 (3) C35—H35 0.95
C4—F12B 1.255 (5) C36—H36 0.95
C4—F12A 1.262 (4) C41—C46 1.388 (3)
C4—F11B 1.263 (4) C41—C42 1.398 (3)
C4—F10A 1.301 (5) C41—P2 1.819 (2)
C4—F10B 1.408 (4) C42—C43 1.387 (3)
C4—F11A 1.437 (4) C42—H42 0.95
C4—C44 1.498 (3) C43—C44 1.389 (3)
C5—F15 1.331 (3) C43—H43 0.95
C5—F14 1.334 (3) C44—C45 1.382 (3)
C5—F13 1.343 (3) C45—C46 1.391 (3)
C5—C54 1.501 (3) C45—H45 0.95
C7—Cl2 1.710 (4) C46—H46 0.95
C7—Cl1 1.722 (4) C51—C52 1.392 (3)
C7—H7A 0.99 C51—C56 1.398 (3)
C7—H7B 0.99 C51—P2 1.820 (2)
C6A—F17A 1.336 (7) C52—C53 1.396 (3)
C6A—F16A 1.356 (8) C52—H52 0.95
C6A—F18A 1.359 (15) C53—C54 1.383 (3)
C6A—C64 1.503 (10) C53—H53 0.95
C6B—F16B 1.312 (13) C54—C55 1.392 (3)
C6B—F17B 1.336 (12) C55—C56 1.390 (3)
C6B—F18B 1.34 (2) C55—H55 0.95
C6B—C64 1.506 (17) C56—H56 0.95
C11—C12 1.393 (3) C61—C66 1.394 (3)
C11—C16 1.398 (3) C61—C62 1.398 (3)
C11—P1 1.826 (2) C61—P2 1.827 (2)
C12—C13 1.395 (3) C62—C63 1.387 (3)
C12—H12 0.95 C62—H62 0.95
C13—C14 1.381 (3) C63—C64 1.393 (3)
C13—H13 0.95 C63—H63 0.95
C14—C15 1.395 (3) C64—C65 1.381 (3)
C15—C16 1.391 (3) C65—C66 1.388 (3)
C15—H15 0.95 C65—H65 0.95
C16—H16 0.95 C66—H66 0.95
C21—C26 1.394 (3) P1—Pd1 2.3174 (5)
C21—C22 1.398 (3) P2—Pd2 2.3130 (6)
C21—P1 1.824 (2) Cl3—Pd1 2.2897 (6)
C22—C23 1.388 (3) Cl4—Pd2 2.2871 (6)
C22—H22 0.95 Pd1—Cl3i 2.2897 (6)
C23—C24 1.393 (3) Pd1—P1i 2.3174 (5)
C23—H23 0.95 Pd2—Cl4ii 2.2871 (6)
C24—C25 1.384 (3) Pd2—P2ii 2.3130 (6)
C25—C26 1.390 (3)
F3—C1—F1 106.6 (2) C36—C31—C32 119.3 (2)
F3—C1—F2 106.3 (2) C36—C31—P1 121.84 (16)
F1—C1—F2 107.1 (2) C32—C31—P1 118.88 (17)
F3—C1—C14 111.1 (2) C33—C32—C31 120.4 (2)
F1—C1—C14 112.1 (2) C33—C32—H32 119.8
F2—C1—C14 113.2 (2) C31—C32—H32 119.8
F4—C2—F5 107.4 (2) C32—C33—C34 119.8 (2)
F4—C2—F6 106.8 (2) C32—C33—H33 120.1
F5—C2—F6 104.9 (2) C34—C33—H33 120.1
F4—C2—C24 112.9 (2) C35—C34—C33 120.3 (2)
F5—C2—C24 112.7 (2) C35—C34—C3 119.6 (2)
F6—C2—C24 111.8 (2) C33—C34—C3 120.0 (2)
F9—C3—F7 107.6 (2) C34—C35—C36 119.9 (2)
F9—C3—F8 106.4 (2) C34—C35—H35 120.1
F7—C3—F8 105.2 (2) C36—C35—H35 120.1
F9—C3—C34 112.1 (2) C31—C36—C35 120.3 (2)
F7—C3—C34 112.6 (2) C31—C36—H36 119.8
F8—C3—C34 112.5 (2) C35—C36—H36 119.8
F12B—C4—F12A 126.7 (3) C46—C41—C42 119.59 (19)
F12B—C4—F11B 113.5 (4) C46—C41—P2 122.65 (16)
F12A—C4—F11B 49.0 (3) C42—C41—P2 117.75 (16)
F12A—C4—F10A 111.8 (4) C43—C42—C41 120.5 (2)
F11B—C4—F10A 131.2 (4) C43—C42—H42 119.8
F12B—C4—F10B 102.9 (4) C41—C42—H42 119.8
F12A—C4—F10B 55.6 (3) C42—C43—C44 119.3 (2)
F11B—C4—F10B 104.1 (4) C42—C43—H43 120.3
F10A—C4—F10B 70.3 (4) C44—C43—H43 120.3
F12B—C4—F11A 65.7 (3) C45—C44—C43 120.4 (2)
F12A—C4—F11A 101.2 (4) C45—C44—C4 119.4 (2)
F11B—C4—F11A 56.3 (4) C43—C44—C4 120.1 (2)
F10A—C4—F11A 98.1 (4) C44—C45—C46 120.3 (2)
F10B—C4—F11A 142.7 (3) C44—C45—H45 119.8
F12B—C4—C44 114.6 (3) C46—C45—H45 119.8
F12A—C4—C44 118.4 (3) C41—C46—C45 119.8 (2)
F11B—C4—C44 112.6 (3) C41—C46—H46 120.1
F10A—C4—C44 115.1 (3) C45—C46—H46 120.1
F10B—C4—C44 107.9 (2) C52—C51—C56 119.31 (19)
F11A—C4—C44 109.1 (2) C52—C51—P2 119.73 (16)
F15—C5—F14 106.9 (2) C56—C51—P2 120.94 (16)
F15—C5—F13 106.4 (2) C51—C52—C53 120.5 (2)
F14—C5—F13 106.46 (19) C51—C52—H52 119.7
F15—C5—C54 111.37 (19) C53—C52—H52 119.7
F14—C5—C54 113.3 (2) C54—C53—C52 119.7 (2)
F13—C5—C54 112.0 (2) C54—C53—H53 120.2
Cl2—C7—Cl1 117.7 (2) C52—C53—H53 120.2
Cl2—C7—H7A 107.9 C53—C54—C55 120.4 (2)
Cl1—C7—H7A 107.9 C53—C54—C5 120.5 (2)
Cl2—C7—H7B 107.9 C55—C54—C5 119.0 (2)
Cl1—C7—H7B 107.9 C56—C55—C54 119.8 (2)
H7A—C7—H7B 107.2 C56—C55—H55 120.1
F17A—C6A—F16A 105.9 (6) C54—C55—H55 120.1
F17A—C6A—F18A 107.6 (10) C55—C56—C51 120.2 (2)
F16A—C6A—F18A 105.3 (8) C55—C56—H56 119.9
F17A—C6A—C64 115.6 (6) C51—C56—H56 119.9
F16A—C6A—C64 110.6 (6) C66—C61—C62 119.4 (2)
F18A—C6A—C64 111.2 (12) C66—C61—P2 121.87 (17)
F16B—C6B—F17B 107.7 (11) C62—C61—P2 118.68 (16)
F16B—C6B—F18B 108.8 (15) C63—C62—C61 120.2 (2)
F17B—C6B—F18B 103.9 (16) C63—C62—H62 119.9
F16B—C6B—C64 114.2 (10) C61—C62—H62 119.9
F17B—C6B—C64 109.0 (10) C62—C63—C64 119.6 (2)
F18B—C6B—C64 113 (2) C62—C63—H63 120.2
C12—C11—C16 119.3 (2) C64—C63—H63 120.2
C12—C11—P1 119.15 (16) C65—C64—C63 120.5 (2)
C16—C11—P1 121.52 (17) C65—C64—C6A 121.5 (4)
C11—C12—C13 120.4 (2) C63—C64—C6A 117.9 (4)
C11—C12—H12 119.8 C65—C64—C6B 118.2 (6)
C13—C12—H12 119.8 C63—C64—C6B 120.7 (6)
C14—C13—C12 119.7 (2) C64—C65—C66 119.9 (2)
C14—C13—H13 120.1 C64—C65—H65 120
C12—C13—H13 120.1 C66—C65—H65 120
C13—C14—C15 120.6 (2) C65—C66—C61 120.2 (2)
C13—C14—C1 120.2 (2) C65—C66—H66 119.9
C15—C14—C1 119.1 (2) C61—C66—H66 119.9
C16—C15—C14 119.6 (2) C31—P1—C21 104.08 (10)
C16—C15—H15 120.2 C31—P1—C11 106.84 (10)
C14—C15—H15 120.2 C21—P1—C11 103.49 (9)
C15—C16—C11 120.3 (2) C31—P1—Pd1 110.60 (7)
C15—C16—H16 119.9 C21—P1—Pd1 119.18 (7)
C11—C16—H16 119.9 C11—P1—Pd1 111.70 (7)
C26—C21—C22 119.5 (2) C41—P2—C51 108.07 (9)
C26—C21—P1 121.38 (17) C41—P2—C61 103.66 (10)
C22—C21—P1 119.12 (16) C51—P2—C61 103.09 (10)
C23—C22—C21 120.2 (2) C41—P2—Pd2 110.58 (7)
C23—C22—H22 119.9 C51—P2—Pd2 111.57 (7)
C21—C22—H22 119.9 C61—P2—Pd2 119.04 (7)
C22—C23—C24 119.7 (2) Cl3—Pd1—Cl3i 180
C22—C23—H23 120.2 Cl3—Pd1—P1 87.299 (19)
C24—C23—H23 120.2 Cl3i—Pd1—P1 92.701 (19)
C25—C24—C23 120.5 (2) Cl3—Pd1—P1i 92.701 (19)
C25—C24—C2 120.3 (2) Cl3i—Pd1—P1i 87.299 (19)
C23—C24—C2 119.2 (2) P1—Pd1—P1i 180.00 (4)
C24—C25—C26 119.8 (2) Cl4—Pd2—Cl4ii 180
C24—C25—H25 120.1 Cl4—Pd2—P2ii 86.151 (19)
C26—C25—H25 120.1 Cl4ii—Pd2—P2ii 93.849 (19)
C25—C26—C21 120.3 (2) Cl4—Pd2—P2 93.849 (19)
C25—C26—H26 119.9 Cl4ii—Pd2—P2 86.151 (19)
C21—C26—H26 119.9 P2ii—Pd2—P2 180
C16—C11—C12—C13 −2.2 (3) C5—C54—C55—C56 177.7 (2)
P1—C11—C12—C13 177.89 (17) C54—C55—C56—C51 −0.2 (3)
C11—C12—C13—C14 0.5 (3) C52—C51—C56—C55 0.4 (3)
C12—C13—C14—C15 1.2 (4) P2—C51—C56—C55 178.40 (18)
C12—C13—C14—C1 −175.1 (2) C66—C61—C62—C63 −0.5 (3)
F3—C1—C14—C13 96.0 (3) P2—C61—C62—C63 178.88 (17)
F1—C1—C14—C13 −144.9 (2) C61—C62—C63—C64 −0.8 (3)
F2—C1—C14—C13 −23.5 (3) C62—C63—C64—C65 1.9 (4)
F3—C1—C14—C15 −80.4 (3) C62—C63—C64—C6A 178.2 (4)
F1—C1—C14—C15 38.8 (3) C62—C63—C64—C6B −169.1 (5)
F2—C1—C14—C15 160.1 (2) F17A—C6A—C64—C65 107.7 (7)
C13—C14—C15—C16 −1.0 (4) F16A—C6A—C64—C65 −132.0 (6)
C1—C14—C15—C16 175.3 (2) F18A—C6A—C64—C65 −15.3 (9)
C14—C15—C16—C11 −0.7 (3) F17A—C6A—C64—C63 −68.5 (7)
C12—C11—C16—C15 2.4 (3) F16A—C6A—C64—C63 51.8 (6)
P1—C11—C16—C15 −177.77 (18) F18A—C6A—C64—C63 168.4 (6)
C26—C21—C22—C23 −1.6 (3) F17A—C6A—C64—C6B −176 (5)
P1—C21—C22—C23 177.88 (16) F16A—C6A—C64—C6B −55 (4)
C21—C22—C23—C24 −0.5 (3) F18A—C6A—C64—C6B 61 (4)
C22—C23—C24—C25 2.1 (3) F16B—C6B—C64—C65 −103.6 (11)
C22—C23—C24—C2 −178.4 (2) F17B—C6B—C64—C65 135.9 (9)
F4—C2—C24—C25 −20.5 (3) F18B—C6B—C64—C65 21.1 (14)
F5—C2—C24—C25 101.3 (3) F16B—C6B—C64—C63 67.5 (11)
F6—C2—C24—C25 −140.9 (2) F17B—C6B—C64—C63 −53.0 (10)
F4—C2—C24—C23 160.0 (2) F18B—C6B—C64—C63 −167.7 (11)
F5—C2—C24—C23 −78.2 (3) F16B—C6B—C64—C6A 147 (5)
F6—C2—C24—C23 39.6 (3) F17B—C6B—C64—C6A 26 (3)
C23—C24—C25—C26 −1.8 (4) F18B—C6B—C64—C6A −89 (4)
C2—C24—C25—C26 178.7 (2) C63—C64—C65—C66 −1.5 (4)
C24—C25—C26—C21 −0.3 (4) C6A—C64—C65—C66 −177.7 (4)
C22—C21—C26—C25 2.0 (3) C6B—C64—C65—C66 169.6 (5)
P1—C21—C26—C25 −177.48 (18) C64—C65—C66—C61 0.2 (4)
C36—C31—C32—C33 −0.1 (3) C62—C61—C66—C65 0.9 (3)
P1—C31—C32—C33 −179.78 (19) P2—C61—C66—C65 −178.52 (19)
C31—C32—C33—C34 0.6 (4) C36—C31—P1—C21 90.20 (19)
C32—C33—C34—C35 −1.1 (4) C32—C31—P1—C21 −90.12 (19)
C32—C33—C34—C3 179.8 (2) C36—C31—P1—C11 −18.9 (2)
F9—C3—C34—C35 −96.9 (3) C32—C31—P1—C11 160.78 (17)
F7—C3—C34—C35 24.6 (3) C36—C31—P1—Pd1 −140.65 (17)
F8—C3—C34—C35 143.3 (2) C32—C31—P1—Pd1 39.02 (19)
F9—C3—C34—C33 82.3 (3) C26—C21—P1—C31 8.4 (2)
F7—C3—C34—C33 −156.2 (2) C22—C21—P1—C31 −171.03 (16)
F8—C3—C34—C33 −37.5 (3) C26—C21—P1—C11 119.96 (18)
C33—C34—C35—C36 1.0 (3) C22—C21—P1—C11 −59.48 (18)
C3—C34—C35—C36 −179.9 (2) C26—C21—P1—Pd1 −115.33 (17)
C32—C31—C36—C35 0.0 (3) C22—C21—P1—Pd1 65.23 (18)
P1—C31—C36—C35 179.66 (17) C12—C11—P1—C31 −104.14 (18)
C34—C35—C36—C31 −0.4 (3) C16—C11—P1—C31 76.0 (2)
C46—C41—C42—C43 −2.5 (4) C12—C11—P1—C21 146.35 (17)
P2—C41—C42—C43 177.08 (19) C16—C11—P1—C21 −33.5 (2)
C41—C42—C43—C44 1.0 (4) C12—C11—P1—Pd1 16.93 (19)
C42—C43—C44—C45 0.7 (4) C16—C11—P1—Pd1 −162.93 (16)
C42—C43—C44—C4 −178.8 (2) C46—C41—P2—C51 −6.8 (2)
F12B—C4—C44—C45 4.0 (5) C42—C41—P2—C51 173.62 (18)
F12A—C4—C44—C45 177.8 (4) C46—C41—P2—C61 102.1 (2)
F11B—C4—C44—C45 −127.8 (4) C42—C41—P2—C61 −77.44 (19)
F10A—C4—C44—C45 41.8 (5) C46—C41—P2—Pd2 −129.21 (17)
F10B—C4—C44—C45 117.9 (3) C42—C41—P2—Pd2 51.23 (19)
F11A—C4—C44—C45 −67.3 (3) C52—C51—P2—C41 −110.65 (18)
F12B—C4—C44—C43 −176.5 (4) C56—C51—P2—C41 71.37 (19)
F12A—C4—C44—C43 −2.6 (5) C52—C51—P2—C61 140.02 (17)
F11B—C4—C44—C43 51.7 (5) C56—C51—P2—C61 −38.0 (2)
F10A—C4—C44—C43 −138.7 (4) C52—C51—P2—Pd2 11.13 (19)
F10B—C4—C44—C43 −62.5 (3) C56—C51—P2—Pd2 −166.86 (15)
F11A—C4—C44—C43 112.3 (3) C66—C61—P2—C41 5.8 (2)
C43—C44—C45—C46 −0.9 (4) C62—C61—P2—C41 −173.60 (17)
C4—C44—C45—C46 178.6 (2) C66—C61—P2—C51 118.38 (19)
C42—C41—C46—C45 2.2 (3) C62—C61—P2—C51 −61.00 (18)
P2—C41—C46—C45 −177.30 (18) C66—C61—P2—Pd2 −117.50 (18)
C44—C45—C46—C41 −0.6 (4) C62—C61—P2—Pd2 63.12 (18)
C56—C51—C52—C53 −0.4 (3) C31—P1—Pd1—Cl3 45.42 (7)
P2—C51—C52—C53 −178.39 (17) C21—P1—Pd1—Cl3 165.92 (8)
C51—C52—C53—C54 0.1 (3) C11—P1—Pd1—Cl3 −73.43 (7)
C52—C53—C54—C55 0.1 (3) C31—P1—Pd1—Cl3i −134.58 (7)
C52—C53—C54—C5 −177.7 (2) C21—P1—Pd1—Cl3i −14.08 (8)
F15—C5—C54—C53 100.5 (3) C11—P1—Pd1—Cl3i 106.57 (7)
F14—C5—C54—C53 −20.0 (3) C41—P2—Pd2—Cl4 −134.36 (8)
F13—C5—C54—C53 −140.5 (2) C51—P2—Pd2—Cl4 105.32 (7)
F15—C5—C54—C55 −77.2 (3) C61—P2—Pd2—Cl4 −14.56 (8)
F14—C5—C54—C55 162.2 (2) C41—P2—Pd2—Cl4ii 45.64 (8)
F13—C5—C54—C55 41.8 (3) C51—P2—Pd2—Cl4ii −74.68 (7)
C53—C54—C55—C56 0.0 (3) C61—P2—Pd2—Cl4ii 165.44 (8)

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

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C12—H12···Cl3 0.95 2.78 3.468 (2) 130
C7—H7B···Cl4 0.99 2.54 3.510 (4) 165
C65—H65···F6iii 0.95 2.55 3.457 (3) 160
C7—H7A···Cl3iv 0.99 2.57 3.550 (5) 169
C15—H15···F17Av 0.95 2.52 3.341 (6) 144
C33—H33···F10B 0.95 2.53 3.435 (4) 159

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZQ2189).

References

  1. Allen, F. H. (2002). Acta Cryst. B58, 380–388. [DOI] [PubMed]
  2. 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.
  3. Bedford, R. B., Cazin, C. S. J. & Holder, D. (2004). Coord. Chem. Rev. 248, 2283–2321.
  4. Brandenburg, K. & Putz, H. (2005). DIAMOND Crystal Impact GbR, Bonn, Germany.
  5. Bruker (2008). SADABS, SAINT and XPREP Bruker AXS Inc., Madison, Wisconsin, USA.
  6. Bruker (2011). APEX2 Bruker AXS Inc., Madison, Wisconsin, USA.
  7. Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
  8. Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.
  9. Otto, S. (2001). Acta Cryst. C57, 793–795. [DOI] [PubMed]
  10. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  11. Tolman, C. A. (1977). Chem. Rev. 77, 313–348.
  12. Weng, Z. F., Motherwell, W. D. S., Allen, F. H. & Cole, J. M. (2008a). Acta Cryst. B64, 348–362. [DOI] [PubMed]
  13. Weng, Z. F., Motherwell, W. D. S. & Cole, J. M. (2008b). J. Appl. Cryst. 41, 955–957.
  14. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

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) global, I. DOI: 10.1107/S1600536812046971/zq2189sup1.cif

e-68-m1508-sup1.cif (51.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812046971/zq2189Isup2.hkl

e-68-m1508-Isup2.hkl (537KB, 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