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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 May 10;70(Pt 6):m204–m205. doi: 10.1107/S1600536814009763

[μ-Butane-1,4-diylbis(di­phenyl­phos­phane)-κ2 P:P′]bis­{[butane-1,4-diylbis(di­phenyl­phosphane)-κ2 P,P′]copper(I)} bis­(hexa­fluorido­phosphate) diethyl ether disolvate

Michihiro Nishikawa a, Asumi Akiyama a, Taro Tsubomura a,*
PMCID: PMC4051095  PMID: 24940196

Abstract

In the centrosymmetric dinuclear copper(I) complex cation of the title compound, [Cu2(C28H28P2)3](PF6)2·2C4H10O, the CuI atom is bonded to three P atoms of two butane-1,4-diylbis(di­phenyl­phosphane) (dppb) ligands with a triangular coordination geometry. One of these P atoms belongs to a bridging dppb ligand [Cu—P = 2.2381 (5) Å] and two belong to a chelating dppb ligand [Cu—P = 2.2450 (6) and 2.2628 (5) Å]. The bridging dppb ligand lies on an inversion centre. In the crystal, the cation and the PF6 anion are linked by C—H⋯F inter­actions, forming a tape along [110]. The cation and the diethyl ether solvent mol­ecule are also linked by a C—H⋯O inter­action.

Related literature  

For general background to emissive copper(I) complexes, see: McMillin & McNett (1998). For copper(I) complexes bearing dppb ligands, see: Comba et al. (1999); Kitagawa et al. (1995). For our previous work related to the photophysical properties of copper(I) complexes bearing dppb and di­imine ligands, see: Saito et al. (2006).graphic file with name e-70-0m204-scheme1.jpg

Experimental  

Crystal data  

  • [Cu2(C28H28P2)3](PF6)2·2C4H10O

  • M r = 1844.61

  • Triclinic, Inline graphic

  • a = 12.7912 (13) Å

  • b = 13.7023 (16) Å

  • c = 14.3811 (13) Å

  • α = 105.595 (3)°

  • β = 90.858 (2)°

  • γ = 111.932 (3)°

  • V = 2233.2 (4) Å3

  • Z = 1

  • Mo Kα radiation

  • μ = 0.69 mm−1

  • T = 123 K

  • 0.5 × 0.5 × 0.4 mm

Data collection  

  • Rigaku Saturn70 CCD diffractometer

  • Absorption correction: multi-scan (REQAB; Rigaku, 1998) T min = 0.687, T max = 0.758

  • 20774 measured reflections

  • 9436 independent reflections

  • 8266 reflections with I > 2σ(I)

  • R int = 0.024

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.036

  • wR(F 2) = 0.090

  • S = 1.06

  • 9436 reflections

  • 523 parameters

  • H-atom parameters constrained

  • Δρmax = 0.41 e Å−3

  • Δρmin = −0.35 e Å−3

Data collection: CrystalClear (Rigaku, 2000); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814009763/is5355sup1.cif

e-70-0m204-sup1.cif (49.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814009763/is5355Isup2.hkl

e-70-0m204-Isup2.hkl (452.2KB, hkl)

CCDC reference: 1000315

Additional supporting information: crystallographic information; 3D view; checkCIF report

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

D—H⋯A D—H H⋯A DA D—H⋯A
C016—H016⋯F006 0.95 2.47 3.318 (3) 149
C018—H018⋯F008i 0.95 2.53 3.286 (3) 137
C043—H04C⋯F006 0.99 2.45 3.345 (3) 150
C043—H04C⋯F009 0.99 2.53 3.458 (3) 156
C049—H049⋯O012ii 0.95 2.46 3.393 (3) 169

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

Acknowledgments

This work was partially supported by a grant from Seikei University.

supplementary crystallographic information

1. Comment

Copper(I) complexes bearing diphosphane ligands are of much interest for luminescence devices (McMillin & McNett, 1998) and catalysts. The spectroscopic study for the coordination compounds of copper(I) ion and 1,4-bis(diphenylphosphino)butane(dppb) ligand has been reported (Comba et al., 1999). The crystal structure of a copper(I) complex bearing dppb, such as [Cu2(dppb)2(ClO4)2] where two copper atoms are bridged by two dppb unit, has been reported (Kitagawa et al., 1995). We have reported the crystal structure of an emissive dinuclear copper(I) complex bearing dppb and diimine ligands (Saito et al., 2006), in which the copper atoms are also bridged by two dppb ligands.

We describe herein the structure of a dinuclear copper(I) complex cation bearing two types of dppb ligands; one is a bridging ligand which connects two copper atoms using two phosphorus atoms, and the other is the chelating ligand which binds one copper atom using two phosphorus atoms. In other words, two copper atoms in the complex are bridged by one dppb ligand. The centre of inversion lies on the bridging dppb ligand. The asymmetric unit consists of a half of the complex cation, a PF6 anion and a diethylether solvent molecule (Fig. 1). Each copper atom is connected by three phosphorus atoms with a triangle coordination geometry. The bond length between copper and phosphorus atom of the bridging dppb ligand is Cu—P = 2.2381 (5) Å, and those between copper and phosphorus atoms of the chelating ligands are Cu—P = 2.2450 (6) and 2.2628 (5) Å. This finding is useful for strategy for creation of characteristic dinuclear copper(I) complexes which exhibit unique properties.

2. Experimental

Under an argon atmosphere, [Cu(MeCN)4]PF6 (75 mg, 0.20 mmol) was added to dppb (82 mg, 0.30 mmol) in a 5 mL dichloromethane. The reaction mixture was stirred for 30 min at room temperature. Diethyl ether was added to the solution to precipitate the product as a white solid, which was filtered and washed with diethyl ether: yield, 126 mg (0.162 mmol, 81%). Elemental Analysis Calcd. for C84H84F12P8Cu2: C 59.47, H 4.99, found C 58.58, H 4.92. Single crystals suitable for X-ray diffraction were obtained by slow diffusion of diethylether in a dichloromethane solution of the complex.

3. Refinement

All H atoms were positioned geometrically and refined using a riding model, with C—H = 0.99 Å and Uiso(H) = 1.2Ueq(C) for methylene groups, C—H = 0.98 Å and Uiso(H) = 1.5Ueq(C) for methyl groups, and C—H = 0.95 Å and Uiso(H) = 1.2Ueq(C) for aromatic groups.

Figures

Fig. 1.

Fig. 1.

ORTEP drawing of [Cu2(µ-dppb)(dppb)2](PF6)2·2Et2O, showing 50% probability displacement ellipsoids. Hydrogen atoms are omitted for clarity. Symmetry code (A); –x + 1, –y, –z + 1.

Crystal data

[Cu2(C28H28P2)3](PF6)2·2C4H10O Z = 1
Mr = 1844.61 F(000) = 958
Triclinic, P1 Dx = 1.372 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.7107 Å
a = 12.7912 (13) Å Cell parameters from 5352 reflections
b = 13.7023 (16) Å θ = 3.1–27.5°
c = 14.3811 (13) Å µ = 0.69 mm1
α = 105.595 (3)° T = 123 K
β = 90.858 (2)° Block, colorless
γ = 111.932 (3)° 0.5 × 0.5 × 0.4 mm
V = 2233.2 (4) Å3

Data collection

Rigaku Saturn70 CCD diffractometer 9436 independent reflections
Graphite monochromator 8266 reflections with I > 2σ(I)
Detector resolution: 28.5714 pixels mm-1 Rint = 0.024
ω scans θmax = 27.5°, θmin = 3.1°
Absorption correction: multi-scan (REQAB; Rigaku, 1998) h = −16→16
Tmin = 0.687, Tmax = 0.758 k = −17→17
20774 measured reflections l = −18→18

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)] = 0.036 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.090 H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0437P)2 + 1.0988P] where P = (Fo2 + 2Fc2)/3
9436 reflections (Δ/σ)max = 0.001
523 parameters Δρmax = 0.41 e Å3
0 restraints Δρmin = −0.35 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
Cu01 0.736171 (18) 0.110853 (17) 0.302039 (16) 0.01521 (7)
P002 0.54853 (4) 0.01284 (4) 0.26739 (3) 0.01428 (10)
P003 0.84597 (4) 0.28839 (4) 0.32139 (3) 0.01596 (10)
P004 0.83982 (4) 0.01424 (4) 0.32330 (4) 0.01677 (11)
P005 0.86536 (5) 0.27004 (4) 0.66681 (4) 0.02525 (12)
F006 0.81271 (11) 0.20082 (10) 0.55514 (9) 0.0341 (3)
F007 0.81659 (13) 0.15823 (12) 0.69569 (12) 0.0501 (4)
F008 0.91334 (11) 0.37992 (10) 0.63536 (10) 0.0366 (3)
F009 0.98020 (11) 0.25176 (12) 0.64561 (11) 0.0425 (3)
F010 0.74923 (13) 0.28665 (13) 0.68407 (12) 0.0511 (4)
F011 0.91859 (15) 0.33750 (13) 0.77641 (10) 0.0540 (4)
O012 0.73139 (16) 0.56078 (14) 0.97322 (12) 0.0419 (4)
C013 0.34145 (16) 0.02452 (16) 0.21426 (14) 0.0196 (4)
H013 0.3106 −0.0537 0.1947 0.023*
C014 0.45566 (15) 0.08317 (15) 0.25249 (13) 0.0158 (4)
C015 0.8519 (2) −0.04572 (18) 0.12452 (15) 0.0298 (5)
H015 0.8053 −0.0064 0.1211 0.036*
C016 0.74237 (17) 0.37377 (16) 0.47064 (14) 0.0222 (4)
H016 0.7317 0.3085 0.4875 0.027*
C017 0.52540 (15) 0.02814 (15) 0.46177 (12) 0.0164 (4)
H01A 0.4992 0.0882 0.4644 0.02*
H01B 0.6093 0.0611 0.4763 0.02*
C018 0.96731 (19) 0.38988 (17) 0.18627 (15) 0.0269 (4)
H018 1.027 0.4346 0.2381 0.032*
C019 0.75556 (17) −0.07541 (18) 0.47393 (15) 0.0252 (4)
H019 0.8023 −0.0054 0.5171 0.03*
C020 0.86868 (17) 0.31242 (15) 0.20336 (14) 0.0198 (4)
C021 0.88492 (17) −0.05330 (15) 0.21397 (14) 0.0204 (4)
C022 0.27251 (17) 0.08035 (18) 0.20464 (15) 0.0250 (4)
H022 0.1948 0.0401 0.1782 0.03*
C023 0.7826 (2) 0.24778 (18) 0.12597 (15) 0.0295 (5)
H023 0.7147 0.1943 0.1365 0.035*
C024 0.79829 (15) 0.39306 (15) 0.39064 (13) 0.0171 (4)
C025 0.70245 (18) 0.44887 (17) 0.52550 (15) 0.0265 (4)
H025 0.6657 0.4357 0.5805 0.032*
C026 0.61412 (19) −0.25764 (19) 0.44828 (19) 0.0346 (5)
H026 0.564 −0.3124 0.4737 0.042*
C027 0.51341 (16) −0.09941 (15) 0.15446 (13) 0.0173 (4)
C028 0.31688 (18) 0.19436 (18) 0.23353 (15) 0.0257 (4)
H028 0.2697 0.2322 0.2266 0.031*
C029 1.06889 (16) 0.17199 (16) 0.37292 (15) 0.0228 (4)
H02A 1.1016 0.1267 0.3269 0.027*
H02B 1.1285 0.2195 0.4288 0.027*
C030 0.49050 (16) −0.05367 (15) 0.35987 (13) 0.0166 (4)
H03A 0.4065 −0.0877 0.3459 0.02*
H03B 0.5178 −0.113 0.3571 0.02*
C031 0.77138 (19) 0.56291 (17) 0.42141 (16) 0.0289 (5)
H031 0.7812 0.6279 0.4045 0.035*
C032 0.98833 (16) 0.32387 (16) 0.38117 (14) 0.0196 (4)
H03C 1.0367 0.4014 0.3865 0.024*
H03D 0.9833 0.3164 0.4477 0.024*
C033 0.95356 (17) −0.11111 (16) 0.21745 (15) 0.0241 (4)
H033 0.9766 −0.1171 0.2781 0.029*
C034 0.53314 (19) −0.15555 (18) −0.01643 (15) 0.0293 (5)
H034 0.5591 −0.1366 −0.0732 0.035*
C035 0.4782 (2) −0.26468 (18) −0.02033 (15) 0.0327 (5)
H035 0.4677 −0.321 −0.0794 0.039*
C036 0.49914 (16) 0.19781 (16) 0.28186 (13) 0.0193 (4)
H036 0.5767 0.2384 0.3085 0.023*
C037 0.81278 (17) 0.48876 (16) 0.36653 (15) 0.0237 (4)
H037 0.851 0.5032 0.3125 0.028*
C038 0.4563 (2) −0.21002 (17) 0.14908 (15) 0.0303 (5)
H038 0.4295 −0.2294 0.2055 0.036*
C039 0.75975 (16) −0.09669 (16) 0.37369 (15) 0.0205 (4)
C040 1.04248 (16) 0.24690 (16) 0.32190 (15) 0.0214 (4)
H04A 0.9906 0.1996 0.2612 0.026*
H04B 1.1141 0.2931 0.3031 0.026*
C041 0.68313 (18) −0.1564 (2) 0.51040 (17) 0.0310 (5)
H041 0.6811 −0.142 0.5786 0.037*
C042 0.9791 (2) 0.40231 (19) 0.09362 (17) 0.0367 (6)
H042 1.047 0.4552 0.0823 0.044*
C043 0.96989 (16) 0.09423 (16) 0.41050 (14) 0.0211 (4)
H04C 0.951 0.1384 0.4693 0.025*
H04D 0.9956 0.0422 0.4304 0.025*
C044 0.71597 (18) 0.54341 (18) 0.50043 (16) 0.0286 (5)
H044 0.6873 0.5944 0.5373 0.034*
C045 0.98856 (19) −0.15988 (18) 0.13317 (17) 0.0314 (5)
H045 1.0358 −0.1987 0.1364 0.038*
C046 0.42993 (18) 0.25338 (17) 0.27254 (14) 0.0236 (4)
H046 0.4602 0.3316 0.2929 0.028*
C047 0.55046 (18) −0.07349 (17) 0.07042 (14) 0.0253 (4)
H047 0.5882 0.0015 0.0725 0.03*
C048 0.9550 (2) −0.1523 (2) 0.04439 (17) 0.0380 (6)
H048 0.9787 −0.1862 −0.0134 0.046*
C049 0.4382 (2) −0.29210 (19) 0.06203 (17) 0.0392 (6)
H049 0.3983 −0.3672 0.0589 0.047*
C050 0.6176 (2) −0.27972 (18) 0.34889 (19) 0.0356 (5)
H050 0.5701 −0.3497 0.3062 0.043*
C051 0.8868 (2) −0.0953 (2) 0.04013 (17) 0.0415 (6)
H051 0.8636 −0.0899 −0.0207 0.05*
C052 0.69051 (18) −0.19939 (17) 0.31144 (17) 0.0276 (5)
H052 0.693 −0.2148 0.2432 0.033*
C053 0.8923 (2) 0.3379 (2) 0.01796 (16) 0.0379 (6)
H053 0.9003 0.3473 −0.045 0.046*
C054 0.7946 (2) 0.2605 (2) 0.03378 (16) 0.0382 (6)
H054 0.7354 0.2156 −0.0184 0.046*
C055 0.7128 (3) 0.6010 (2) 1.07002 (19) 0.0475 (7)
H05A 0.6304 0.5702 1.0752 0.057*
H05B 0.7396 0.6822 1.0887 0.057*
C056 0.6958 (3) 0.5383 (3) 0.8049 (2) 0.0558 (8)
H05C 0.6541 0.5551 0.7578 0.084*
H05D 0.6711 0.4583 0.7899 0.084*
H05E 0.7775 0.5713 0.8011 0.084*
C057 0.6727 (3) 0.5841 (2) 0.90481 (19) 0.0464 (6)
H05F 0.6968 0.6649 0.9198 0.056*
H05G 0.5901 0.5517 0.9085 0.056*
C058 0.7755 (3) 0.5687 (2) 1.1374 (2) 0.0533 (7)
H05H 0.7622 0.5966 1.2044 0.08*
H05I 0.8571 0.6001 1.1327 0.08*
H05J 0.7483 0.4882 1.1191 0.08*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu01 0.01457 (12) 0.01581 (12) 0.01666 (12) 0.00650 (9) 0.00247 (8) 0.00621 (9)
P002 0.0150 (2) 0.0165 (2) 0.0123 (2) 0.00630 (19) 0.00294 (17) 0.00560 (17)
P003 0.0153 (2) 0.0153 (2) 0.0180 (2) 0.00644 (19) 0.00140 (18) 0.00544 (18)
P004 0.0173 (2) 0.0177 (2) 0.0192 (2) 0.00926 (19) 0.00360 (18) 0.00798 (19)
P005 0.0228 (3) 0.0251 (3) 0.0236 (3) 0.0035 (2) 0.0038 (2) 0.0090 (2)
F006 0.0344 (7) 0.0299 (7) 0.0327 (7) 0.0125 (6) −0.0080 (6) 0.0017 (5)
F007 0.0513 (9) 0.0383 (8) 0.0586 (10) 0.0030 (7) 0.0066 (7) 0.0320 (7)
F008 0.0379 (8) 0.0276 (7) 0.0348 (7) 0.0002 (6) −0.0031 (6) 0.0130 (6)
F009 0.0270 (7) 0.0575 (9) 0.0471 (8) 0.0182 (7) 0.0010 (6) 0.0200 (7)
F010 0.0401 (8) 0.0523 (9) 0.0642 (10) 0.0218 (7) 0.0275 (8) 0.0160 (8)
F011 0.0779 (12) 0.0463 (9) 0.0216 (7) 0.0082 (8) −0.0026 (7) 0.0081 (6)
O012 0.0539 (11) 0.0360 (9) 0.0362 (9) 0.0183 (8) 0.0060 (8) 0.0104 (7)
C013 0.0174 (9) 0.0223 (9) 0.0193 (9) 0.0061 (8) 0.0041 (7) 0.0090 (8)
C014 0.0172 (9) 0.0218 (9) 0.0113 (8) 0.0084 (8) 0.0057 (7) 0.0082 (7)
C015 0.0411 (13) 0.0323 (11) 0.0246 (11) 0.0223 (10) 0.0048 (9) 0.0107 (9)
C016 0.0250 (10) 0.0217 (10) 0.0197 (10) 0.0084 (8) 0.0014 (8) 0.0067 (8)
C017 0.0169 (9) 0.0200 (9) 0.0137 (9) 0.0075 (7) 0.0036 (7) 0.0065 (7)
C018 0.0327 (12) 0.0247 (10) 0.0237 (10) 0.0101 (9) 0.0090 (9) 0.0090 (8)
C019 0.0233 (10) 0.0330 (11) 0.0289 (11) 0.0168 (9) 0.0070 (8) 0.0160 (9)
C020 0.0268 (10) 0.0170 (9) 0.0192 (9) 0.0126 (8) 0.0038 (8) 0.0050 (7)
C021 0.0220 (10) 0.0183 (9) 0.0209 (9) 0.0074 (8) 0.0043 (8) 0.0066 (7)
C022 0.0159 (9) 0.0374 (12) 0.0254 (10) 0.0110 (9) 0.0052 (8) 0.0141 (9)
C023 0.0336 (12) 0.0300 (11) 0.0236 (11) 0.0117 (10) −0.0012 (9) 0.0071 (9)
C024 0.0135 (9) 0.0183 (9) 0.0177 (9) 0.0058 (7) −0.0020 (7) 0.0033 (7)
C025 0.0251 (11) 0.0317 (11) 0.0214 (10) 0.0113 (9) 0.0054 (8) 0.0054 (9)
C026 0.0294 (12) 0.0351 (12) 0.0573 (16) 0.0185 (10) 0.0195 (11) 0.0326 (12)
C027 0.0192 (9) 0.0202 (9) 0.0144 (9) 0.0098 (8) 0.0018 (7) 0.0050 (7)
C028 0.0266 (11) 0.0379 (12) 0.0256 (11) 0.0215 (10) 0.0111 (8) 0.0169 (9)
C029 0.0179 (9) 0.0253 (10) 0.0281 (11) 0.0116 (8) 0.0025 (8) 0.0077 (8)
C030 0.0181 (9) 0.0187 (9) 0.0139 (9) 0.0072 (7) 0.0027 (7) 0.0062 (7)
C031 0.0348 (12) 0.0238 (10) 0.0347 (12) 0.0172 (10) 0.0054 (9) 0.0105 (9)
C032 0.0167 (9) 0.0207 (9) 0.0227 (10) 0.0082 (8) 0.0016 (7) 0.0073 (8)
C033 0.0256 (10) 0.0250 (10) 0.0248 (10) 0.0131 (9) 0.0046 (8) 0.0077 (8)
C034 0.0322 (12) 0.0371 (12) 0.0151 (10) 0.0110 (10) 0.0079 (8) 0.0058 (9)
C035 0.0479 (14) 0.0306 (11) 0.0182 (10) 0.0205 (11) 0.0014 (9) −0.0019 (9)
C036 0.0180 (9) 0.0232 (10) 0.0164 (9) 0.0076 (8) 0.0030 (7) 0.0060 (7)
C037 0.0260 (10) 0.0222 (10) 0.0260 (10) 0.0113 (9) 0.0051 (8) 0.0094 (8)
C038 0.0475 (14) 0.0224 (10) 0.0190 (10) 0.0097 (10) 0.0038 (9) 0.0087 (8)
C039 0.0200 (10) 0.0226 (10) 0.0284 (10) 0.0138 (8) 0.0077 (8) 0.0142 (8)
C040 0.0166 (9) 0.0238 (10) 0.0260 (10) 0.0081 (8) 0.0049 (8) 0.0104 (8)
C041 0.0273 (11) 0.0471 (14) 0.0375 (13) 0.0241 (11) 0.0152 (10) 0.0282 (11)
C042 0.0527 (15) 0.0316 (12) 0.0366 (13) 0.0213 (12) 0.0243 (12) 0.0192 (10)
C043 0.0209 (10) 0.0241 (10) 0.0209 (10) 0.0115 (8) 0.0017 (8) 0.0070 (8)
C044 0.0261 (11) 0.0292 (11) 0.0301 (11) 0.0161 (9) 0.0022 (9) 0.0010 (9)
C045 0.0335 (12) 0.0292 (11) 0.0352 (12) 0.0176 (10) 0.0106 (10) 0.0076 (9)
C046 0.0294 (11) 0.0237 (10) 0.0231 (10) 0.0149 (9) 0.0073 (8) 0.0088 (8)
C047 0.0258 (11) 0.0248 (10) 0.0201 (10) 0.0033 (9) 0.0063 (8) 0.0079 (8)
C048 0.0525 (15) 0.0363 (13) 0.0290 (12) 0.0233 (12) 0.0167 (11) 0.0064 (10)
C049 0.0653 (17) 0.0211 (11) 0.0265 (12) 0.0130 (11) 0.0015 (11) 0.0057 (9)
C050 0.0327 (12) 0.0226 (11) 0.0552 (16) 0.0113 (10) 0.0122 (11) 0.0164 (11)
C051 0.0646 (17) 0.0483 (15) 0.0198 (11) 0.0307 (14) 0.0071 (11) 0.0102 (10)
C052 0.0313 (11) 0.0231 (10) 0.0327 (12) 0.0136 (9) 0.0082 (9) 0.0106 (9)
C053 0.0695 (18) 0.0430 (14) 0.0214 (11) 0.0405 (14) 0.0166 (11) 0.0141 (10)
C054 0.0543 (16) 0.0433 (14) 0.0196 (11) 0.0258 (13) −0.0025 (10) 0.0041 (10)
C055 0.0595 (18) 0.0430 (15) 0.0371 (14) 0.0219 (14) 0.0069 (12) 0.0050 (12)
C056 0.080 (2) 0.0540 (17) 0.0420 (16) 0.0326 (17) 0.0099 (15) 0.0193 (13)
C057 0.0589 (17) 0.0430 (15) 0.0440 (15) 0.0261 (14) 0.0047 (13) 0.0145 (12)
C058 0.080 (2) 0.0392 (15) 0.0381 (15) 0.0245 (15) 0.0001 (14) 0.0071 (12)

Geometric parameters (Å, º)

Cu01—P002 2.2381 (5) C029—H02A 0.99
Cu01—P003 2.2450 (6) C029—H02B 0.99
Cu01—P004 2.2628 (5) C030—H03A 0.99
P002—C027 1.8232 (18) C030—H03B 0.99
P002—C030 1.8239 (18) C031—C044 1.382 (3)
P002—C014 1.8287 (19) C031—C037 1.385 (3)
P003—C020 1.821 (2) C031—H031 0.95
P003—C024 1.8233 (19) C032—C040 1.549 (3)
P003—C032 1.8326 (19) C032—H03C 0.99
P004—C021 1.8179 (19) C032—H03D 0.99
P004—C039 1.827 (2) C033—C045 1.386 (3)
P004—C043 1.838 (2) C033—H033 0.95
P005—F011 1.5865 (15) C034—C035 1.379 (3)
P005—F008 1.5914 (13) C034—C047 1.387 (3)
P005—F007 1.5952 (14) C034—H034 0.95
P005—F010 1.5979 (15) C035—C049 1.385 (3)
P005—F009 1.6001 (14) C035—H035 0.95
P005—F006 1.6136 (13) C036—C046 1.391 (3)
O012—C057 1.400 (3) C036—H036 0.95
O012—C055 1.412 (3) C037—H037 0.95
C013—C022 1.393 (3) C038—C049 1.388 (3)
C013—C014 1.394 (3) C038—H038 0.95
C013—H013 0.95 C039—C052 1.391 (3)
C014—C036 1.393 (3) C040—H04A 0.99
C015—C051 1.390 (3) C040—H04B 0.99
C015—C021 1.390 (3) C041—H041 0.95
C015—H015 0.95 C042—C053 1.382 (4)
C016—C025 1.382 (3) C042—H042 0.95
C016—C024 1.397 (3) C043—H04C 0.99
C016—H016 0.95 C043—H04D 0.99
C017—C030 1.525 (2) C044—H044 0.95
C017—C017i 1.526 (4) C045—C048 1.383 (3)
C017—H01A 0.99 C045—H045 0.95
C017—H01B 0.99 C046—H046 0.95
C018—C020 1.388 (3) C047—H047 0.95
C018—C042 1.391 (3) C048—C051 1.382 (4)
C018—H018 0.95 C048—H048 0.95
C019—C041 1.388 (3) C049—H049 0.95
C019—C039 1.398 (3) C050—C052 1.392 (3)
C019—H019 0.95 C050—H050 0.95
C020—C023 1.393 (3) C051—H051 0.95
C021—C033 1.393 (3) C052—H052 0.95
C022—C028 1.384 (3) C053—C054 1.374 (4)
C022—H022 0.95 C053—H053 0.95
C023—C054 1.386 (3) C054—H054 0.95
C023—H023 0.95 C055—C058 1.501 (4)
C024—C037 1.393 (3) C055—H05A 0.99
C025—C044 1.387 (3) C055—H05B 0.99
C025—H025 0.95 C056—C057 1.488 (4)
C026—C041 1.377 (3) C056—H05C 0.98
C026—C050 1.384 (4) C056—H05D 0.98
C026—H026 0.95 C056—H05E 0.98
C027—C047 1.391 (3) C057—H05F 0.99
C027—C038 1.395 (3) C057—H05G 0.99
C028—C046 1.385 (3) C058—H05H 0.98
C028—H028 0.95 C058—H05I 0.98
C029—C043 1.534 (3) C058—H05J 0.98
C029—C040 1.537 (3)
P002—Cu01—P003 133.28 (2) C040—C032—P003 110.13 (13)
P002—Cu01—P004 114.80 (2) C040—C032—H03C 109.6
P003—Cu01—P004 111.92 (2) P003—C032—H03C 109.6
C027—P002—C030 105.01 (8) C040—C032—H03D 109.6
C027—P002—C014 104.23 (8) P003—C032—H03D 109.6
C030—P002—C014 103.78 (8) H03C—C032—H03D 108.1
C027—P002—Cu01 111.49 (6) C045—C033—C021 120.5 (2)
C030—P002—Cu01 112.37 (6) C045—C033—H033 119.7
C014—P002—Cu01 118.73 (6) C021—C033—H033 119.7
C020—P003—C024 106.26 (8) C035—C034—C047 120.0 (2)
C020—P003—C032 104.91 (9) C035—C034—H034 120
C024—P003—C032 105.67 (8) C047—C034—H034 120
C020—P003—Cu01 110.32 (6) C034—C035—C049 119.93 (19)
C024—P003—Cu01 118.20 (6) C034—C035—H035 120
C032—P003—Cu01 110.57 (6) C049—C035—H035 120
C021—P004—C039 104.70 (9) C046—C036—C014 120.56 (18)
C021—P004—C043 105.34 (9) C046—C036—H036 119.7
C039—P004—C043 103.73 (9) C014—C036—H036 119.7
C021—P004—Cu01 115.92 (7) C031—C037—C024 119.88 (19)
C039—P004—Cu01 111.21 (6) C031—C037—H037 120.1
C043—P004—Cu01 114.76 (7) C024—C037—H037 120.1
F011—P005—F008 90.76 (8) C049—C038—C027 120.6 (2)
F011—P005—F007 90.56 (9) C049—C038—H038 119.7
F008—P005—F007 178.65 (8) C027—C038—H038 119.7
F011—P005—F010 91.82 (10) C052—C039—C019 119.30 (19)
F008—P005—F010 89.62 (8) C052—C039—P004 119.75 (16)
F007—P005—F010 90.62 (9) C019—C039—P004 120.41 (16)
F011—P005—F009 90.11 (9) C029—C040—C032 116.42 (16)
F008—P005—F009 90.01 (8) C029—C040—H04A 108.2
F007—P005—F009 89.70 (9) C032—C040—H04A 108.2
F010—P005—F009 178.04 (9) C029—C040—H04B 108.2
F011—P005—F006 179.17 (9) C032—C040—H04B 108.2
F008—P005—F006 89.42 (7) H04A—C040—H04B 107.3
F007—P005—F006 89.25 (8) C026—C041—C019 120.4 (2)
F010—P005—F006 88.99 (8) C026—C041—H041 119.8
F009—P005—F006 89.08 (7) C019—C041—H041 119.8
C057—O012—C055 113.7 (2) C053—C042—C018 120.2 (2)
C022—C013—C014 120.15 (18) C053—C042—H042 119.9
C022—C013—H013 119.9 C018—C042—H042 119.9
C014—C013—H013 119.9 C029—C043—P004 115.32 (14)
C036—C014—C013 119.15 (17) C029—C043—H04C 108.4
C036—C014—P002 119.39 (14) P004—C043—H04C 108.4
C013—C014—P002 121.44 (14) C029—C043—H04D 108.4
C051—C015—C021 120.4 (2) P004—C043—H04D 108.4
C051—C015—H015 119.8 H04C—C043—H04D 107.5
C021—C015—H015 119.8 C031—C044—C025 119.59 (19)
C025—C016—C024 120.52 (19) C031—C044—H044 120.2
C025—C016—H016 119.7 C025—C044—H044 120.2
C024—C016—H016 119.7 C048—C045—C033 120.3 (2)
C030—C017—C017i 111.06 (19) C048—C045—H045 119.8
C030—C017—H01A 109.4 C033—C045—H045 119.8
C017i—C017—H01A 109.4 C028—C046—C036 119.84 (19)
C030—C017—H01B 109.4 C028—C046—H046 120.1
C017i—C017—H01B 109.4 C036—C046—H046 120.1
H01A—C017—H01B 108 C034—C047—C027 120.96 (19)
C020—C018—C042 120.3 (2) C034—C047—H047 119.5
C020—C018—H018 119.8 C027—C047—H047 119.5
C042—C018—H018 119.8 C051—C048—C045 119.6 (2)
C041—C019—C039 120.0 (2) C051—C048—H048 120.2
C041—C019—H019 120 C045—C048—H048 120.2
C039—C019—H019 120 C035—C049—C038 120.1 (2)
C018—C020—C023 118.60 (19) C035—C049—H049 120
C018—C020—P003 123.66 (15) C038—C049—H049 120
C023—C020—P003 117.73 (16) C026—C050—C052 120.0 (2)
C015—C021—C033 118.84 (18) C026—C050—H050 120
C015—C021—P004 119.39 (15) C052—C050—H050 120
C033—C021—P004 121.76 (15) C048—C051—C015 120.3 (2)
C028—C022—C013 120.17 (19) C048—C051—H051 119.9
C028—C022—H022 119.9 C015—C051—H051 119.9
C013—C022—H022 119.9 C039—C052—C050 120.1 (2)
C054—C023—C020 120.9 (2) C039—C052—H052 119.9
C054—C023—H023 119.5 C050—C052—H052 119.9
C020—C023—H023 119.5 C054—C053—C042 120.0 (2)
C037—C024—C016 119.11 (17) C054—C053—H053 120
C037—C024—P003 123.42 (15) C042—C053—H053 120
C016—C024—P003 117.45 (14) C053—C054—C023 119.9 (2)
C016—C025—C044 120.1 (2) C053—C054—H054 120
C016—C025—H025 120 C023—C054—H054 120
C044—C025—H025 120 O012—C055—C058 109.8 (2)
C041—C026—C050 120.1 (2) O012—C055—H05A 109.7
C041—C026—H026 119.9 C058—C055—H05A 109.7
C050—C026—H026 119.9 O012—C055—H05B 109.7
C047—C027—C038 118.45 (18) C058—C055—H05B 109.7
C047—C027—P002 118.10 (15) H05A—C055—H05B 108.2
C038—C027—P002 123.38 (15) C057—C056—H05C 109.5
C022—C028—C046 120.12 (18) C057—C056—H05D 109.5
C022—C028—H028 119.9 H05C—C056—H05D 109.5
C046—C028—H028 119.9 C057—C056—H05E 109.5
C043—C029—C040 117.31 (16) H05C—C056—H05E 109.5
C043—C029—H02A 108 H05D—C056—H05E 109.5
C040—C029—H02A 108 O012—C057—C056 110.4 (2)
C043—C029—H02B 108 O012—C057—H05F 109.6
C040—C029—H02B 108 C056—C057—H05F 109.6
H02A—C029—H02B 107.2 O012—C057—H05G 109.6
C017—C030—P002 111.60 (12) C056—C057—H05G 109.6
C017—C030—H03A 109.3 H05F—C057—H05G 108.1
P002—C030—H03A 109.3 C055—C058—H05H 109.5
C017—C030—H03B 109.3 C055—C058—H05I 109.5
P002—C030—H03B 109.3 H05H—C058—H05I 109.5
H03A—C030—H03B 108 C055—C058—H05J 109.5
C044—C031—C037 120.8 (2) H05H—C058—H05J 109.5
C044—C031—H031 119.6 H05I—C058—H05J 109.5
C037—C031—H031 119.6
P003—Cu01—P002—C027 119.57 (7) Cu01—P002—C027—C038 120.60 (17)
P004—Cu01—P002—C027 −60.79 (7) C013—C022—C028—C046 −0.3 (3)
P003—Cu01—P002—C030 −122.85 (7) C017i—C017—C030—P002 179.00 (16)
P004—Cu01—P002—C030 56.79 (7) C027—P002—C030—C017 173.01 (13)
P003—Cu01—P002—C014 −1.56 (7) C014—P002—C030—C017 −77.86 (14)
P004—Cu01—P002—C014 178.07 (6) Cu01—P002—C030—C017 51.64 (14)
P002—Cu01—P003—C020 −79.86 (7) C020—P003—C032—C040 −62.16 (15)
P004—Cu01—P003—C020 100.50 (7) C024—P003—C032—C040 −174.22 (13)
P002—Cu01—P003—C024 42.64 (8) Cu01—P003—C032—C040 56.76 (14)
P004—Cu01—P003—C024 −137.00 (7) C015—C021—C033—C045 0.2 (3)
P002—Cu01—P003—C032 164.55 (7) P004—C021—C033—C045 −178.67 (16)
P004—Cu01—P003—C032 −15.09 (7) C047—C034—C035—C049 1.4 (4)
P002—Cu01—P004—C021 88.21 (7) C013—C014—C036—C046 −0.5 (3)
P003—Cu01—P004—C021 −92.08 (7) P002—C014—C036—C046 −179.15 (14)
P002—Cu01—P004—C039 −31.21 (8) C044—C031—C037—C024 0.3 (3)
P003—Cu01—P004—C039 148.50 (7) C016—C024—C037—C031 −0.3 (3)
P002—Cu01—P004—C043 −148.56 (7) P003—C024—C037—C031 178.27 (16)
P003—Cu01—P004—C043 31.15 (7) C047—C027—C038—C049 0.8 (3)
C022—C013—C014—C036 0.8 (3) P002—C027—C038—C049 −176.02 (19)
C022—C013—C014—P002 179.38 (15) C041—C019—C039—C052 0.2 (3)
C027—P002—C014—C036 −137.70 (15) C041—C019—C039—P004 171.72 (15)
C030—P002—C014—C036 112.59 (15) C021—P004—C039—C052 −37.54 (18)
Cu01—P002—C014—C036 −12.95 (17) C043—P004—C039—C052 −147.75 (16)
C027—P002—C014—C013 43.71 (17) Cu01—P004—C039—C052 88.38 (16)
C030—P002—C014—C013 −66.00 (16) C021—P004—C039—C019 151.01 (15)
Cu01—P002—C014—C013 168.45 (12) C043—P004—C039—C019 40.79 (17)
C042—C018—C020—C023 0.1 (3) Cu01—P004—C039—C019 −83.08 (16)
C042—C018—C020—P003 179.00 (16) C043—C029—C040—C032 56.8 (2)
C024—P003—C020—C018 82.72 (18) P003—C032—C040—C029 −116.84 (16)
C032—P003—C020—C018 −28.92 (19) C050—C026—C041—C019 0.8 (3)
Cu01—P003—C020—C018 −148.02 (15) C039—C019—C041—C026 −0.8 (3)
C024—P003—C020—C023 −98.42 (16) C020—C018—C042—C053 0.3 (3)
C032—P003—C020—C023 149.94 (16) C040—C029—C043—P004 48.1 (2)
Cu01—P003—C020—C023 30.85 (17) C021—P004—C043—C029 52.85 (16)
C051—C015—C021—C033 0.2 (3) C039—P004—C043—C029 162.59 (14)
C051—C015—C021—P004 179.04 (19) Cu01—P004—C043—C029 −75.88 (14)
C039—P004—C021—C015 121.03 (17) C037—C031—C044—C025 0.5 (3)
C043—P004—C021—C015 −129.92 (17) C016—C025—C044—C031 −1.2 (3)
Cu01—P004—C021—C015 −1.88 (19) C021—C033—C045—C048 −0.5 (3)
C039—P004—C021—C033 −60.12 (18) C022—C028—C046—C036 0.6 (3)
C043—P004—C021—C033 48.93 (19) C014—C036—C046—C028 −0.1 (3)
Cu01—P004—C021—C033 176.96 (14) C035—C034—C047—C027 0.2 (3)
C014—C013—C022—C028 −0.4 (3) C038—C027—C047—C034 −1.2 (3)
C018—C020—C023—C054 −0.2 (3) P002—C027—C047—C034 175.70 (17)
P003—C020—C023—C054 −179.12 (17) C033—C045—C048—C051 0.4 (4)
C025—C016—C024—C037 −0.3 (3) C034—C035—C049—C038 −1.9 (4)
C025—C016—C024—P003 −179.02 (15) C027—C038—C049—C035 0.8 (4)
C020—P003—C024—C037 −17.76 (19) C041—C026—C050—C052 −0.3 (3)
C032—P003—C024—C037 93.35 (17) C045—C048—C051—C015 0.0 (4)
Cu01—P003—C024—C037 −142.28 (14) C021—C015—C051—C048 −0.2 (4)
C020—P003—C024—C016 160.86 (15) C019—C039—C052—C050 0.3 (3)
C032—P003—C024—C016 −88.03 (16) P004—C039—C052—C050 −171.28 (16)
Cu01—P003—C024—C016 36.34 (16) C026—C050—C052—C039 −0.2 (3)
C024—C016—C025—C044 1.1 (3) C018—C042—C053—C054 −0.8 (3)
C030—P002—C027—C047 −178.12 (15) C042—C053—C054—C023 0.8 (4)
C014—P002—C027—C047 73.07 (17) C020—C023—C054—C053 −0.3 (3)
Cu01—P002—C027—C047 −56.18 (17) C057—O012—C055—C058 178.0 (2)
C030—P002—C027—C038 −1.3 (2) C055—O012—C057—C056 −179.5 (2)
C014—P002—C027—C038 −110.14 (18)

Symmetry code: (i) −x+1, −y, −z+1.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C016—H016···F006 0.95 2.47 3.318 (3) 149
C018—H018···F008ii 0.95 2.53 3.286 (3) 137
C043—H04C···F006 0.99 2.45 3.345 (3) 150
C043—H04C···F009 0.99 2.53 3.458 (3) 156
C049—H049···O012i 0.95 2.46 3.393 (3) 169

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

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: IS5355).

References

  1. Altomare, A., Cascarano, G., Giacovazzo, C. & Guagliardi, A. (1993). J. Appl. Cryst. 26, 343–350.
  2. Comba, P., Katsichtis, C., Nuber, B. & Pritzkow, H. (1999). Eur. J. Inorg. Chem. pp. 777–783.
  3. Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
  4. Kitagawa, S., Kondo, M., Kawata, S., Wada, S., Maekawa, M. & Megumu, M. (1995). Inorg. Chem. 34, 1455–1465.
  5. McMillin, D. R. & McNett, K. M. (1998). Chem. Rev. 98, 1201–1220. [DOI] [PubMed]
  6. Rigaku (1998). REQAB. Rigaku Corporation, Tokyo, Japan.
  7. Rigaku (2000). CrystalClear Rigaku Corporation, Tokyo, Japan.
  8. Saito, K., Arai, T., Takahashi, N., Tsukuda, T. & Tsubomura, T. (2006). Dalton Trans. pp. 4444–4448. [DOI] [PubMed]
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  10. 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/S1600536814009763/is5355sup1.cif

e-70-0m204-sup1.cif (49.5KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814009763/is5355Isup2.hkl

e-70-0m204-Isup2.hkl (452.2KB, hkl)

CCDC reference: 1000315

Additional supporting information: 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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