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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Mar 28;69(Pt 4):m231. doi: 10.1107/S1600536813006831

catena-Poly[[copper(I)-μ-2,6-bis­[4-(pyridin-2-yl)thia­zol-2-yl]pyridine] hexa­fluoridophosphate acetonitrile monosolvate] from single-crystal synchrotron data

Linda Xiao a, Mohan Bhadbhade b, Anthony T Baker a,*
PMCID: PMC3629503  PMID: 23634021

Abstract

The title complex, {[Cu(C21H13N5S2)]PF6·CH3CN}n, was formed immediately on adding together a methanol solution containing copper(I) ions and a methanol solution of 2,6-bis­[4-(pyridin-2-yl)thia­zol-2-yl]pyridine. Crystallographic studies of the complex reveal a coordination polymer with the ligand acting as a bis­(bidentate) ligand with the pyridine N atom not coordinating a metal centre. The CuI atom is four-coordinate with approximately tetra­hedral stereochemistry: the N4 donor set is provided by bipyridine-like moieties of the two heterocyclic ligands. Parallel chains of the coordination polymer run along the b-axis direction with the disordered (0.50:0.50 occupancy ratio) PF6 anions and acetonitrile solvent mol­ecules located between the chains.

Related literature  

For a related complex, see: Baker & Matthews (1999).graphic file with name e-69-0m231-scheme1.jpg

Experimental  

Crystal data  

  • [Cu(C21H13N5S2)]PF6·C2H3N

  • M r = 649.05

  • Monoclinic, Inline graphic

  • a = 12.525 (3) Å

  • b = 13.950 (3) Å

  • c = 14.626 (3) Å

  • β = 97.72 (3)°

  • V = 2532.4 (9) Å3

  • Z = 4

  • Synchrotron radiation

  • λ = 0.71073 Å

  • μ = 1.16 mm−1

  • T = 100 K

  • 0.03 × 0.02 × 0.01 mm

Data collection  

  • 3-BM1 Australian Synchrotron diffractometer

  • 28022 measured reflections

  • 3890 independent reflections

  • 3641 reflections with I > 2σ(I)

  • R int = 0.024

  • θmax = 23.8°

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.031

  • wR(F 2) = 0.078

  • S = 1.08

  • 3890 reflections

  • 389 parameters

  • H-atom parameters constrained

  • Δρmax = 0.30 e Å−3

  • Δρmin = −0.57 e Å−3

Data collection: BLU-ICE (McPhillips et al., 2002); cell refinement: XDS (Kabsch, 1993); data reduction: XDS; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2008); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813006831/vm2190sup1.cif

e-69-0m231-sup1.cif (34.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813006831/vm2190Isup2.hkl

e-69-0m231-Isup2.hkl (190.7KB, hkl)

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

Acknowledgments

The authors thank the Australian Synchrotron Facility, Melbourne, for the X-ray data.

supplementary crystallographic information

Comment

We have prepared and studied many analogues of 2,2'-bipyridine and 2,2':6',2"-terpyridine (Baker and Matthews, 1999 and references therein) and have extended this work to the preparation of ligands analogous to quinquepyridine. For metal complexes of these quinquepyridine analogues, a number of features have been observed. The interpolation of a five-membered heterocycle appears to reduce the capacity of the ligands to employ all five donor atoms and we have seen several examples where the ligands act in a bis(bidentate) mode [2 + 2]. In such cases the ligands bridge between metal centres in binuclear complexes. Herein we report a coordination polymer shown in Scheme 1, again where the ligand binds in [2 + 2] mode. A thermal ellipsoid plot is shown in Fig. 1. Each copper centre has approximately tetrahedral stereochemistry as shown in Fig. 1. The principal cause of distortion being the bite angles of the bidentate ligand N2B—Cu1—N1B (82.47 (8)°) and N2Ai—Cu1—N1Ai (82.95 (8)°) (symmetry code: (i) -x + 1, y + 1/2, -z + 1/2) are considerably less than the ideal tetrahedral angle. Two 'thiazolylpyridine' moieties coordinate each copper(I) centre with the relevant bond lengths being Cu—N1Ai 2.098 (2) Å, Cu—N1B 2.050 (2) Å, Cu—N2A 1.992 (2) Å and Cu—N2B 2.024 (2) Å. The Cu—N bond lengths are similar but the Cu—Npyridinyl bonds are slightly shorter than the Cu—Nthiazolyl bonds. This indicates a slightly stronger interaction of the metal atom with the pyridinyl moiety, in line with base strength. A single chain of the coordination polymer, thus created, is depicted in Fig. 2 and packing of these chains that include PF6- anions and solvent molecules of acetonitriles are shown in Fig. 3.

Experimental

The quinquedentate ligand 2,6-bis(4-(pyridin-2-yl)thiazol-2-yl)pyridine was prepared by adding a solution of 2-(bromoacetyl)pyridinium hydrobromide (5.6 g, 20 mmol) in hot ethanol (50 ml) to a solution of 2,6-di(thioamido)pyridine (2.0 g, 10 mmol) in hot ethanol (50 ml). The solution was heated for 5 min, a yellow precipitate of 2,6-bis(4-(pyridin-2-yl)thiazol-2-yl)pyridinium hydrobromide separated soon. The mixture was allowed to stand for 30 min s and the yellow precipitate was filtered and washed with sodium bicarbonate (5%) until effervescence ceased. Yield: 75%. The complex was prepared as follows: Tetrakis(acetonitrile)copper(I) hexafluorophosphate (200 mg, 0.54 mmol) in hot methanol (20 ml) was added to a solution of the ligand (214 mg, 0.54 mmol) in hot methanol (20 ml). The reaction mixture was heated on the water bath for 1 h. An orange solid formed during this time and once cooled the solid was collected, washed with cooled methanol and stored over silica gel (yield 164 mg, 50%). Crystals were grown by vapour diffusion of diethyl ether into a concentrated acetonitrile solution of the complex.

Refinement

All the H-atoms were fixed stereochemically and included in the refinement using riding model option in SHELXL97. The PF6 anion was found to exhibit orientational disorder, which was modelled over two positions.

H atoms were positioned geometrically with C—H = 0.93 - 0.96 Å. Uiso(H) values were set at 1.2Ueq (aromatic) or 1.5Ueq of the parent atom (methyl group).

Figures

Fig. 1.

Fig. 1.

Thermal ellipsoids plot (40% probability) of the part of the coordination polymer showing the geometry around Cu(I) ion. Hydrogen atoms, the PF6 anion and the solvent acetonitrile molecule are omitted for clarity. Symmetry code: (i) -x + 1, y + 1/2, -z + 1/2.

Fig. 2.

Fig. 2.

A single chain showing the construction of the coordination polymer formed with the ligand.

Fig. 3.

Fig. 3.

Packing of coordination polymers viewed down c axis that includes PF6 anions (disorder omitted for clarity) and solvent molecules (acetonitrile).

Crystal data

[Cu(C21H13N5S2)]PF6·C2H3N F(000) = 1304
Mr = 649.05 Dx = 1.702 Mg m3
Monoclinic, P21/c Synchrotron radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 9980 reflections
a = 12.525 (3) Å θ = 2.5–22.5°
b = 13.950 (3) Å µ = 1.16 mm1
c = 14.626 (3) Å T = 100 K
β = 97.72 (3)° Thin plates, blue
V = 2532.4 (9) Å3 0.03 × 0.02 × 0.01 mm
Z = 4

Data collection

3-BM1 Australian Synchrotron diffractometer 3641 reflections with I > 2σ(I)
Radiation source: Synchrotron BM Rint = 0.024
Si<111> monochromator θmax = 23.8°, θmin = 1.6°
φ scans h = −14→14
28022 measured reflections k = −15→15
3890 independent reflections l = −16→16

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)] = 0.031 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.078 H-atom parameters constrained
S = 1.08 w = 1/[σ2(Fo2) + (0.0359P)2 + 3.8973P],P = (Fo2 + 2Fc2)/3
3890 reflections (Δ/σ)max = 0.001
389 parameters Δρmax = 0.30 e Å3
0 restraints Δρmin = −0.57 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 Occ. (<1)
Cu1 0.70815 (2) 1.19154 (2) 0.36895 (2) 0.01965 (11)
N1 0.40269 (16) 0.95445 (14) 0.35587 (13) 0.0159 (4)
C1 0.5696 (2) 0.89759 (19) 0.25992 (17) 0.0211 (6)
H1 0.6257 0.8784 0.2285 0.025*
C2 0.4814 (2) 0.83892 (18) 0.26281 (17) 0.0197 (5)
H2 0.4773 0.7794 0.2339 0.024*
C3 0.3990 (2) 0.87086 (17) 0.30999 (16) 0.0165 (5)
C4 0.48924 (19) 1.00992 (17) 0.35293 (16) 0.0162 (5)
C5 0.5735 (2) 0.98545 (18) 0.30444 (17) 0.0197 (5)
H5 0.6311 1.0270 0.3020 0.024*
S1A 0.21354 (5) 0.84000 (5) 0.39190 (4) 0.02002 (16)
N1A 0.27744 (16) 0.73513 (14) 0.26615 (14) 0.0163 (4)
N2A 0.17898 (16) 0.59744 (15) 0.15433 (14) 0.0180 (4)
C1A 0.3024 (2) 0.81261 (17) 0.31486 (16) 0.0160 (5)
C2A 0.18499 (19) 0.69316 (17) 0.28980 (17) 0.0173 (5)
C3A 0.1400 (2) 0.74016 (19) 0.35688 (17) 0.0207 (5)
H3A 0.0781 0.7207 0.3803 0.025*
C4A 0.14469 (19) 0.60735 (18) 0.23785 (17) 0.0173 (5)
C5A 0.0784 (2) 0.5404 (2) 0.27187 (18) 0.0239 (6)
H5A 0.0574 0.5484 0.3300 0.029*
C6A 0.0438 (2) 0.4617 (2) 0.21859 (19) 0.0276 (6)
H6A −0.0001 0.4157 0.2405 0.033*
C7A 0.0757 (2) 0.4527 (2) 0.13181 (19) 0.0275 (6)
H7A 0.0520 0.4015 0.0937 0.033*
C8A 0.1432 (2) 0.52119 (18) 0.10326 (18) 0.0232 (6)
H8A 0.1652 0.5142 0.0454 0.028*
S1B 0.37811 (5) 1.12599 (5) 0.46088 (4) 0.02089 (16)
N1B 0.56301 (16) 1.16578 (14) 0.41446 (13) 0.0154 (4)
N2B 0.69867 (17) 1.31538 (14) 0.43946 (14) 0.0193 (5)
C1B 0.48752 (19) 1.09985 (18) 0.40534 (16) 0.0165 (5)
C2B 0.5353 (2) 1.24125 (18) 0.46810 (16) 0.0173 (5)
C3B 0.4376 (2) 1.23154 (18) 0.49859 (17) 0.0207 (5)
H4B 0.4076 1.2762 0.5349 0.025*
C4B 0.6105 (2) 1.32303 (18) 0.48297 (17) 0.0190 (5)
C5B 0.5930 (2) 1.40191 (19) 0.53706 (18) 0.0248 (6)
H5B 0.5330 1.4047 0.5682 0.030*
C6B 0.6670 (2) 1.47623 (19) 0.54353 (19) 0.0290 (6)
H6B 0.6566 1.5303 0.5785 0.035*
C7B 0.7559 (2) 1.46972 (19) 0.49804 (18) 0.0263 (6)
H7B 0.8059 1.5193 0.5013 0.032*
C8B 0.7696 (2) 1.38795 (19) 0.44740 (18) 0.0239 (6)
H8B 0.8305 1.3831 0.4176 0.029*
P1 0.91781 (5) 0.77051 (5) 0.06197 (5) 0.02250 (17)
F1 1.02028 (15) 0.72763 (13) 0.02232 (14) 0.0467 (5)
F2 0.9637 (5) 0.7561 (5) 0.1692 (5) 0.0320 (13) 0.50
F3 0.8706 (11) 0.6650 (9) 0.0595 (7) 0.034 (2) 0.50
F4 0.8738 (5) 0.7876 (5) −0.0432 (4) 0.0503 (15) 0.50
F5 0.9640 (8) 0.8778 (6) 0.0694 (4) 0.0348 (15) 0.50
F2' 1.0012 (6) 0.7796 (6) 0.1511 (5) 0.064 (2) 0.50
F3' 0.8878 (13) 0.6654 (11) 0.0896 (8) 0.063 (4) 0.50
F4' 0.8345 (5) 0.7575 (6) −0.0299 (5) 0.063 (2) 0.50
F5' 0.9533 (8) 0.8721 (7) 0.0272 (6) 0.080 (3) 0.50
F6 0.81523 (16) 0.81302 (15) 0.10063 (17) 0.0572 (6)
C1AN 0.1934 (3) 0.1022 (3) 0.2238 (2) 0.0507 (9)
H1A1 0.1468 0.0772 0.1718 0.076*
H1A2 0.1637 0.1606 0.2442 0.076*
H1A3 0.2001 0.0562 0.2730 0.076*
C2AN 0.2998 (3) 0.1214 (2) 0.19694 (19) 0.0297 (7)
N1AN 0.3824 (2) 0.13309 (19) 0.17597 (18) 0.0368 (6)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cu1 0.02253 (19) 0.01556 (18) 0.02245 (18) 0.00197 (12) 0.00884 (13) −0.00093 (12)
N1 0.0184 (11) 0.0143 (10) 0.0151 (10) 0.0000 (8) 0.0026 (8) 0.0017 (8)
C1 0.0218 (13) 0.0219 (14) 0.0209 (13) 0.0003 (11) 0.0083 (10) −0.0021 (11)
C2 0.0243 (14) 0.0154 (13) 0.0195 (13) −0.0016 (10) 0.0031 (10) −0.0016 (10)
C3 0.0198 (13) 0.0146 (12) 0.0146 (12) 0.0000 (10) 0.0012 (10) 0.0032 (10)
C4 0.0214 (13) 0.0130 (12) 0.0137 (12) −0.0013 (10) 0.0000 (10) 0.0016 (10)
C5 0.0195 (13) 0.0194 (13) 0.0210 (13) −0.0038 (10) 0.0058 (10) 0.0006 (10)
S1A 0.0198 (3) 0.0213 (3) 0.0196 (3) 0.0006 (3) 0.0054 (2) −0.0028 (3)
N1A 0.0173 (10) 0.0145 (11) 0.0172 (10) 0.0002 (8) 0.0024 (8) 0.0026 (9)
N2A 0.0174 (10) 0.0165 (11) 0.0199 (11) 0.0017 (9) 0.0022 (8) 0.0025 (9)
C1A 0.0179 (12) 0.0151 (13) 0.0150 (12) 0.0023 (10) 0.0025 (10) 0.0023 (10)
C2A 0.0157 (12) 0.0173 (13) 0.0188 (12) 0.0003 (10) 0.0016 (10) 0.0047 (10)
C3A 0.0173 (13) 0.0243 (14) 0.0211 (13) −0.0019 (11) 0.0046 (10) 0.0023 (11)
C4A 0.0148 (12) 0.0160 (13) 0.0207 (13) 0.0019 (10) 0.0009 (10) 0.0041 (10)
C5A 0.0221 (14) 0.0262 (14) 0.0233 (13) −0.0032 (11) 0.0029 (11) 0.0052 (11)
C6A 0.0258 (14) 0.0227 (14) 0.0337 (15) −0.0093 (11) 0.0023 (12) 0.0069 (12)
C7A 0.0317 (15) 0.0188 (14) 0.0310 (15) −0.0073 (12) 0.0004 (12) −0.0022 (12)
C8A 0.0272 (14) 0.0199 (14) 0.0226 (13) −0.0005 (11) 0.0036 (11) −0.0002 (11)
S1B 0.0197 (3) 0.0201 (3) 0.0244 (3) −0.0023 (3) 0.0085 (3) −0.0034 (3)
N1B 0.0189 (11) 0.0132 (10) 0.0146 (10) 0.0000 (8) 0.0038 (8) 0.0009 (8)
N2B 0.0225 (11) 0.0152 (11) 0.0197 (11) 0.0005 (9) 0.0010 (9) 0.0010 (9)
C1B 0.0181 (12) 0.0178 (13) 0.0141 (12) 0.0018 (10) 0.0039 (10) 0.0021 (10)
C2B 0.0230 (13) 0.0148 (12) 0.0142 (12) 0.0020 (10) 0.0025 (10) 0.0001 (10)
C3B 0.0231 (14) 0.0186 (13) 0.0212 (13) 0.0005 (11) 0.0059 (10) −0.0051 (11)
C4B 0.0229 (13) 0.0166 (13) 0.0172 (12) 0.0019 (10) 0.0013 (10) 0.0019 (10)
C5B 0.0294 (15) 0.0196 (14) 0.0253 (14) 0.0035 (11) 0.0037 (11) −0.0033 (11)
C6B 0.0404 (17) 0.0173 (14) 0.0288 (15) 0.0022 (12) 0.0022 (13) −0.0060 (11)
C7B 0.0336 (16) 0.0153 (13) 0.0283 (15) −0.0057 (11) −0.0021 (12) −0.0008 (11)
C8B 0.0236 (14) 0.0212 (14) 0.0269 (14) −0.0031 (11) 0.0030 (11) 0.0038 (11)
P1 0.0214 (4) 0.0218 (4) 0.0244 (4) 0.0027 (3) 0.0035 (3) 0.0035 (3)
F1 0.0402 (11) 0.0389 (11) 0.0688 (13) 0.0088 (8) 0.0354 (10) 0.0116 (9)
F2 0.046 (4) 0.029 (2) 0.021 (2) 0.009 (2) 0.003 (2) 0.0040 (16)
F3 0.033 (4) 0.020 (4) 0.051 (5) −0.010 (3) 0.016 (3) −0.016 (4)
F4 0.064 (5) 0.061 (4) 0.023 (2) 0.018 (3) −0.008 (3) 0.011 (2)
F5 0.046 (3) 0.017 (2) 0.046 (3) −0.001 (2) 0.024 (3) −0.002 (3)
F2' 0.053 (5) 0.092 (6) 0.039 (4) 0.035 (4) −0.018 (3) −0.038 (4)
F3' 0.051 (6) 0.043 (5) 0.103 (10) 0.004 (4) 0.037 (6) 0.032 (6)
F4' 0.031 (3) 0.113 (6) 0.041 (3) 0.001 (3) −0.010 (2) 0.001 (3)
F5' 0.038 (3) 0.030 (4) 0.176 (9) 0.006 (3) 0.027 (6) 0.054 (6)
F6 0.0392 (11) 0.0510 (13) 0.0864 (16) 0.0157 (9) 0.0267 (11) −0.0079 (11)
C1AN 0.0362 (19) 0.077 (3) 0.0421 (19) −0.0020 (18) 0.0159 (15) 0.0064 (19)
C2AN 0.0368 (18) 0.0305 (16) 0.0215 (14) 0.0006 (13) 0.0026 (13) 0.0061 (12)
N1AN 0.0347 (16) 0.0418 (16) 0.0340 (14) −0.0042 (12) 0.0049 (12) 0.0149 (12)

Geometric parameters (Å, º)

Cu1—N2Ai 1.992 (2) C8A—H8A 0.9300
Cu1—N2B 2.024 (2) S1B—C3B 1.708 (3)
Cu1—N1B 2.050 (2) S1B—C1B 1.723 (2)
Cu1—N1Ai 2.098 (2) N1B—C1B 1.313 (3)
N1—C4 1.337 (3) N1B—C2B 1.385 (3)
N1—C3 1.343 (3) N2B—C8B 1.342 (3)
C1—C2 1.380 (4) N2B—C4B 1.351 (3)
C1—C5 1.386 (4) C2B—C3B 1.364 (4)
C1—H1 0.9300 C2B—C4B 1.476 (4)
C2—C3 1.390 (4) C3B—H4B 0.9300
C2—H2 0.9300 C4B—C5B 1.390 (4)
C3—C1A 1.467 (3) C5B—C6B 1.385 (4)
C4—C5 1.391 (4) C5B—H5B 0.9300
C4—C1B 1.472 (3) C6B—C7B 1.375 (4)
C5—H5 0.9300 C6B—H6B 0.9300
S1A—C3A 1.710 (3) C7B—C8B 1.383 (4)
S1A—C1A 1.730 (2) C7B—H7B 0.9300
N1A—C1A 1.309 (3) C8B—H8B 0.9300
N1A—C2A 1.382 (3) P1—F2' 1.562 (7)
N1A—Cu1ii 2.098 (2) P1—F3' 1.580 (16)
N2A—C8A 1.342 (3) P1—F4 1.581 (6)
N2A—C4A 1.355 (3) P1—F3 1.585 (13)
N2A—Cu1ii 1.992 (2) P1—F6 1.587 (2)
C2A—C3A 1.363 (4) P1—F5' 1.589 (9)
C2A—C4A 1.470 (4) P1—F1 1.5941 (18)
C3A—H3A 0.9300 P1—F4' 1.597 (7)
C4A—C5A 1.385 (4) P1—F5 1.603 (9)
C5A—C6A 1.382 (4) P1—F2 1.609 (7)
C5A—H5A 0.9300 C1AN—C2AN 1.464 (4)
C6A—C7A 1.387 (4) C1AN—H1A1 0.9600
C6A—H6A 0.9300 C1AN—H1A2 0.9600
C7A—C8A 1.377 (4) C1AN—H1A3 0.9600
C7A—H7A 0.9300 C2AN—N1AN 1.130 (4)
N2Ai—Cu1—N2B 137.85 (9) S1B—C3B—H4B 124.7
N2Ai—Cu1—N1B 128.37 (8) N2B—C4B—C5B 122.1 (2)
N2B—Cu1—N1B 82.47 (8) N2B—C4B—C2B 114.5 (2)
N2Ai—Cu1—N1Ai 82.95 (8) C5B—C4B—C2B 123.3 (2)
N2B—Cu1—N1Ai 104.53 (8) C6B—C5B—C4B 118.5 (3)
N1B—Cu1—N1Ai 123.28 (8) C6B—C5B—H5B 120.8
C4—N1—C3 117.4 (2) C4B—C5B—H5B 120.8
C2—C1—C5 119.2 (2) C7B—C6B—C5B 119.7 (3)
C2—C1—H1 120.4 C7B—C6B—H6B 120.1
C5—C1—H1 120.4 C5B—C6B—H6B 120.1
C1—C2—C3 118.4 (2) C6B—C7B—C8B 118.7 (3)
C1—C2—H2 120.8 C6B—C7B—H7B 120.7
C3—C2—H2 120.8 C8B—C7B—H7B 120.7
N1—C3—C2 123.3 (2) N2B—C8B—C7B 122.7 (3)
N1—C3—C1A 115.5 (2) N2B—C8B—H8B 118.6
C2—C3—C1A 121.3 (2) C7B—C8B—H8B 118.6
N1—C4—C5 123.3 (2) F2'—P1—F3' 91.0 (5)
N1—C4—C1B 114.1 (2) F2'—P1—F4 155.0 (4)
C5—C4—C1B 122.7 (2) F3'—P1—F4 109.0 (5)
C1—C5—C4 118.4 (2) F2'—P1—F3 107.4 (5)
C1—C5—H5 120.8 F3'—P1—F3 16.8 (6)
C4—C5—H5 120.8 F4—P1—F3 92.2 (5)
C3A—S1A—C1A 89.57 (12) F2'—P1—F6 98.9 (3)
C1A—N1A—C2A 111.1 (2) F3'—P1—F6 91.4 (6)
C1A—N1A—Cu1ii 135.01 (17) F4—P1—F6 95.6 (3)
C2A—N1A—Cu1ii 107.09 (15) F3—P1—F6 92.2 (5)
C8A—N2A—C4A 117.4 (2) F2'—P1—F5' 90.6 (5)
C8A—N2A—Cu1ii 128.23 (18) F3'—P1—F5' 174.9 (7)
C4A—N2A—Cu1ii 113.89 (16) F4—P1—F5' 68.3 (4)
N1A—C1A—C3 124.7 (2) F3—P1—F5' 160.2 (5)
N1A—C1A—S1A 114.16 (18) F6—P1—F5' 93.2 (3)
C3—C1A—S1A 121.09 (18) F2'—P1—F1 81.6 (3)
C3A—C2A—N1A 114.7 (2) F3'—P1—F1 88.6 (6)
C3A—C2A—C4A 128.1 (2) F4—P1—F1 84.0 (3)
N1A—C2A—C4A 117.2 (2) F3—P1—F1 87.7 (5)
C2A—C3A—S1A 110.47 (19) F6—P1—F1 179.52 (13)
C2A—C3A—H3A 124.8 F5'—P1—F1 86.8 (3)
S1A—C3A—H3A 124.8 F2'—P1—F4' 177.9 (4)
N2A—C4A—C5A 122.2 (2) F3'—P1—F4' 87.6 (5)
N2A—C4A—C2A 114.9 (2) F4—P1—F4' 25.2 (2)
C5A—C4A—C2A 122.9 (2) F3—P1—F4' 71.1 (5)
C6A—C5A—C4A 119.4 (2) F6—P1—F4' 82.8 (3)
C6A—C5A—H5A 120.3 F5'—P1—F4' 90.7 (4)
C4A—C5A—H5A 120.3 F1—P1—F4' 96.8 (3)
C5A—C6A—C7A 118.8 (2) F2'—P1—F5 70.9 (4)
C5A—C6A—H6A 120.6 F3'—P1—F5 161.0 (4)
C7A—C6A—H6A 120.6 F4—P1—F5 90.0 (3)
C8A—C7A—C6A 118.6 (3) F3—P1—F5 177.2 (5)
C8A—C7A—H7A 120.7 F6—P1—F5 86.0 (3)
C6A—C7A—H7A 120.7 F5'—P1—F5 22.4 (4)
N2A—C8A—C7A 123.6 (2) F1—P1—F5 94.2 (3)
N2A—C8A—H8A 118.2 F4'—P1—F5 110.7 (4)
C7A—C8A—H8A 118.2 F2'—P1—F2 23.9 (3)
C3B—S1B—C1B 89.68 (12) F3'—P1—F2 72.6 (4)
C1B—N1B—C2B 111.0 (2) F4—P1—F2 178.4 (3)
C1B—N1B—Cu1 138.40 (17) F3—P1—F2 89.4 (4)
C2B—N1B—Cu1 110.56 (16) F6—P1—F2 84.2 (2)
C8B—N2B—C4B 118.3 (2) F5'—P1—F2 110.2 (4)
C8B—N2B—Cu1 127.22 (18) F1—P1—F2 96.2 (2)
C4B—N2B—Cu1 114.53 (17) F4'—P1—F2 156.0 (3)
N1B—C1B—C4 126.1 (2) F5—P1—F2 88.4 (3)
N1B—C1B—S1B 114.28 (18) C2AN—C1AN—H1A1 109.5
C4—C1B—S1B 119.61 (18) C2AN—C1AN—H1A2 109.5
C3B—C2B—N1B 114.4 (2) H1A1—C1AN—H1A2 109.5
C3B—C2B—C4B 127.6 (2) C2AN—C1AN—H1A3 109.5
N1B—C2B—C4B 117.9 (2) H1A1—C1AN—H1A3 109.5
C2B—C3B—S1B 110.60 (19) H1A2—C1AN—H1A3 109.5
C2B—C3B—H4B 124.7 N1AN—C2AN—C1AN 177.8 (4)
C5—C1—C2—C3 0.5 (4) N2B—Cu1—N1B—C1B 176.7 (3)
C4—N1—C3—C2 2.0 (3) N1Ai—Cu1—N1B—C1B 74.2 (3)
C4—N1—C3—C1A −179.8 (2) N2Ai—Cu1—N1B—C2B 147.28 (15)
C1—C2—C3—N1 −2.6 (4) N2B—Cu1—N1B—C2B −0.84 (16)
C1—C2—C3—C1A 179.3 (2) N1Ai—Cu1—N1B—C2B −103.31 (16)
C3—N1—C4—C5 0.6 (3) N2Ai—Cu1—N2B—C8B 39.4 (3)
C3—N1—C4—C1B −179.6 (2) N1B—Cu1—N2B—C8B −178.7 (2)
C2—C1—C5—C4 1.9 (4) N1Ai—Cu1—N2B—C8B −56.2 (2)
N1—C4—C5—C1 −2.6 (4) N2Ai—Cu1—N2B—C4B −140.17 (17)
C1B—C4—C5—C1 177.7 (2) N1B—Cu1—N2B—C4B 1.73 (17)
C2A—N1A—C1A—C3 176.6 (2) N1Ai—Cu1—N2B—C4B 124.25 (17)
Cu1ii—N1A—C1A—C3 −37.1 (4) C2B—N1B—C1B—C4 179.8 (2)
C2A—N1A—C1A—S1A −0.7 (3) Cu1—N1B—C1B—C4 2.3 (4)
Cu1ii—N1A—C1A—S1A 145.62 (16) C2B—N1B—C1B—S1B 0.3 (3)
N1—C3—C1A—N1A 171.2 (2) Cu1—N1B—C1B—S1B −177.16 (14)
C2—C3—C1A—N1A −10.5 (4) N1—C4—C1B—N1B 179.0 (2)
N1—C3—C1A—S1A −11.7 (3) C5—C4—C1B—N1B −1.2 (4)
C2—C3—C1A—S1A 166.63 (19) N1—C4—C1B—S1B −1.5 (3)
C3A—S1A—C1A—N1A 0.76 (19) C5—C4—C1B—S1B 178.24 (19)
C3A—S1A—C1A—C3 −176.6 (2) C3B—S1B—C1B—N1B −0.1 (2)
C1A—N1A—C2A—C3A 0.2 (3) C3B—S1B—C1B—C4 −179.6 (2)
Cu1ii—N1A—C2A—C3A −155.55 (18) C1B—N1B—C2B—C3B −0.5 (3)
C1A—N1A—C2A—C4A 177.6 (2) Cu1—N1B—C2B—C3B 177.75 (17)
Cu1ii—N1A—C2A—C4A 21.8 (2) C1B—N1B—C2B—C4B −178.3 (2)
N1A—C2A—C3A—S1A 0.3 (3) Cu1—N1B—C2B—C4B −0.1 (3)
C4A—C2A—C3A—S1A −176.7 (2) N1B—C2B—C3B—S1B 0.4 (3)
C1A—S1A—C3A—C2A −0.6 (2) C4B—C2B—C3B—S1B 178.0 (2)
C8A—N2A—C4A—C5A 2.3 (3) C1B—S1B—C3B—C2B −0.2 (2)
Cu1ii—N2A—C4A—C5A −170.47 (19) C8B—N2B—C4B—C5B −1.8 (4)
C8A—N2A—C4A—C2A −178.9 (2) Cu1—N2B—C4B—C5B 177.81 (19)
Cu1ii—N2A—C4A—C2A 8.3 (3) C8B—N2B—C4B—C2B 178.2 (2)
C3A—C2A—C4A—N2A 155.6 (2) Cu1—N2B—C4B—C2B −2.2 (3)
N1A—C2A—C4A—N2A −21.4 (3) C3B—C2B—C4B—N2B −176.0 (2)
C3A—C2A—C4A—C5A −25.6 (4) N1B—C2B—C4B—N2B 1.5 (3)
N1A—C2A—C4A—C5A 157.4 (2) C3B—C2B—C4B—C5B 4.0 (4)
N2A—C4A—C5A—C6A −1.4 (4) N1B—C2B—C4B—C5B −178.5 (2)
C2A—C4A—C5A—C6A 179.9 (2) N2B—C4B—C5B—C6B 2.3 (4)
C4A—C5A—C6A—C7A −0.7 (4) C2B—C4B—C5B—C6B −177.7 (2)
C5A—C6A—C7A—C8A 1.8 (4) C4B—C5B—C6B—C7B −1.0 (4)
C4A—N2A—C8A—C7A −1.1 (4) C5B—C6B—C7B—C8B −0.6 (4)
Cu1ii—N2A—C8A—C7A 170.5 (2) C4B—N2B—C8B—C7B 0.0 (4)
C6A—C7A—C8A—N2A −1.0 (4) Cu1—N2B—C8B—C7B −179.53 (19)
N2Ai—Cu1—N1B—C1B −35.2 (3) C6B—C7B—C8B—N2B 1.2 (4)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: VM2190).

References

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  2. Kabsch, W. (1993). J. Appl. Cryst. 26, 795–800.
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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/S1600536813006831/vm2190sup1.cif

e-69-0m231-sup1.cif (34.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813006831/vm2190Isup2.hkl

e-69-0m231-Isup2.hkl (190.7KB, hkl)

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


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