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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 11;67(Pt 7):m911–m912. doi: 10.1107/S1600536811021994

A second monoclinic polymorph of {bis­[5-methyl-3-(trifluoro­meth­yl)pyrazol-1-yl]borato}{tris­[5-methyl-3-(trifluoro­meth­yl)pyrazol-1-yl]borato}cobalt(II): a structure containing a B—H⋯Co agostic inter­action

Robert T Stibrany a,*, Joseph A Potenza a
PMCID: PMC3151874  PMID: 21836897

Abstract

The title compound, [Co(C10H10BF6N4)(C15H13BF9N6)], is a polymorph of the previously reported neutral cobalt(II) complex [Stibrany & Potenza (2010). Acta Cryst. E66, m506–m507], which contains one each of the monoanionic ligands, bis­[5-methyl-3-(trifluoro­meth­yl)pyrazol-1-yl]borate (Bp) and tris­[5-methyl-3-(trifluoro­meth­yl)pyrazol-1-yl]borate (Tp). A distorted octahedral coordination geometry of the CoII atom results from ligation of an H atom, which is part of an agostic B—H⋯Co inter­action [H⋯Co = 2.12 (3) Å], and by five imine N atoms, two from a Bp ligand and three from a Tp ligand. Weak intra- and inter­molecular C—F⋯π inter­actions with F⋯centroid distances ranging from 3.025 (4) to 3.605 (4) Å are observed.

Related literature

For our study of nitro­gen-containing heterocyles and their complexes with metal ions, see: Stibrany & Potenza (2006, 2009a ,b ); Stibrany et al. (1999, 2005, 2006). For a polymorph of the title compound, see: Stibrany & Potenza (2010). For oxidation studies of copper and cobalt complexes utilizing the title ligand, see: Gorun et al. (2000). For agostic inter­actions, see: Ruman et al. (2001, 2002); Siemer et al. (2001); Ghosh et al. (1998).graphic file with name e-67-0m911-scheme1.jpg

Experimental

Crystal data

  • [Co(C10H10BF6N4)(C15H13BF9N6)]

  • M r = 829.08

  • Monoclinic, Inline graphic

  • a = 18.593 (2) Å

  • b = 12.1167 (13) Å

  • c = 30.720 (3) Å

  • β = 102.721 (2)°

  • V = 6751.1 (13) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.63 mm−1

  • T = 298 K

  • 0.28 × 0.24 × 0.12 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Blessing, 1995) T min = 0.875, T max = 1.00

  • 32390 measured reflections

  • 7431 independent reflections

  • 5522 reflections with I > 2σ(I)

  • R int = 0.032

Refinement

  • R[F 2 > 2σ(F 2)] = 0.059

  • wR(F 2) = 0.167

  • S = 1.00

  • 7431 reflections

  • 495 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.69 e Å−3

  • Δρmin = −0.32 e Å−3

Data collection: SMART WNT/2000 (Bruker, 2000); cell refinement: SAINT-Plus (Bruker, 2000); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPIII (Burnett & Johnson, 1996) and ORTEP-32 (Farrugia, 1997); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S1600536811021994/rz2601sup1.cif

e-67-0m911-sup1.cif (31.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021994/rz2601Isup2.hkl

e-67-0m911-Isup2.hkl (363.7KB, hkl)

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

Table 1. Selected bond lengths (Å).

Co1—N7 2.100 (3)
Co1—H21B 2.12 (3)
Co1—N9 2.124 (3)
Co1—N3 2.124 (3)
Co1—N1 2.163 (3)
Co1—N5 2.172 (3)

Table 2. Flourine inter­action geometry (Å, °).

Cg1, Cg2, Cg3 and Cg4 are the centroids of the N3/N4/C9/C8/C7, N5/N6/C14/C13/C12, N7/N8/C19/C18/C17 and N9/N10/C24/C23/C22 rings, respectively.

C—F⋯Cg C—F F⋯Cg C⋯Cg C—F⋯Cg
C1—F1⋯Cg4 1.333 (5) 3.319 (4) 3.798 (5) 100.7 (3)
C1—F2⋯Cg2i 1.331 (4) 3.341 (3) 4.565 (4) 152.6 (2)
C1—F3⋯Cg4 1.316 (5) 3.273 (3) 3.798 (5) 103.3 (3)
C11—F9⋯Cg3 1.295 (5) 3.025 (4) 3.826 (4) 119.1 (3)
C16—F10⋯Cg1 1.298 (5) 3.252 (4) 4.279 (4) 135.8 (3)
C16—F10⋯Cg2 1.298 (5) 3.208 (3) 4.061 (4) 122.8 (2)
C16—F11⋯Cg4ii 1.324 (5) 3.605 (4) 4.467 (4) 123.0 (3)
C21—F13⋯Cg1 1.321 (5) 3.373 (3) 4.346 (5) 130.3 (3)

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

Acknowledgments

Any acknowledgements?

supplementary crystallographic information

Comment

Our long-term interest in the synthesis and applications of nitrogen-containing heterocyles, such as expanded-ring imidazoles, and their complexes with metal ions (Stibrany & Potenza, 2009a) led us to prepare the title compound (I). With pyrazole, a variety of metal complexes has been prepared, predominantly with copper (Stibrany & Potenza, 2006), including the Cu(II) complex of an unusual (dimethylamino)methane bridged bis(pyrazole) ligand formed via a DMF aminalization (Stibrany et al., 1999) and a novel binuclear µ-oxalato(1-benzylpyrazole)2(CF3SO3)2copper(II) compound resulting from the fixation of carbon dioxide (Stibrany et al., 2005). A tris(pyrazolyl)arene ligand which forms geometrically constrained metal complexes has also been prepared (Stibrany et al., 2006), as has a sterically strained trigonal-bipyramidal Cu(II) complex containing a 1-benzylpyrazole ligand (Stibrany & Potenza, 2009b). Copper and cobalt complexes utlizing the title ligand were prepared for oxidation studies (Gorun et al., 2000).

Compound (I) (Fig. 1) contains a central Co(II) ion linked to a Tp and a Bp ligand. Ligation is effected by three imine N atoms of the Tp ligand, two imine N atoms of the Bp ligand, and an H atom which participates in a two-electron, three-center B—H···Co bond. The result is a distorted octahedral coordination geometry. Compound (I) is a polymorph of a previously reported structure of the same compound (II) (Stibrany & Potenza, 2010). The present polymorph was the result of a ligand displacement reaction in which a Tp ligand was added to a preformed Co(Bp)2 complex to form (I).

A number of cobalt(II) complexes containing mixed bis (Bp)- and tris pyrazolylborates (Tp) and C—H···Co agostic interactions have been reported, with H···Co distances ranging from 2.03 Å (Ruman et al., 2002), 2.035 Å (Ruman et al., 2001) to 2.334 Å (Siemer et al., 2001). The H···Co distance in (I), 2.12 (3) Å, lies between these two extremes. Infrared spectral results also support the existence of an agostic 2-electron, 3-center bond in (I). B—H stretching vibrations for BH2 groups in which one of the H atoms is involved in a 2-electron, 3-center bond with a metal ion typically lie in the range 2100–2500 cm-1, with the lower value corresponding to the agostic interaction (Ghosh et al., 1998). In (I), IR bands at 2570 and 2492 cm-1 are assigned as free B—H stretching vibrations, while the band at 2217 cm-1 is assigned to the bound B—H group.

The coordination geometries of both polymorphs are similar: in both, the largest deviations from octahedral symmetry are found with the H—Co—N angles associated with the bound hydrogen atom. The polymorphs differ fundamentally in the behavior of the trifluoromethyl groups. In the first polymorph, the molecules formed layers linked by intermolecular C—H···F hydrogen bonds in such a way as to form chains along the a cell direction. In contrast, the current polymorph exhibits no such hydrogen bonds; rather PLATON (Spek, 2009) reveals six intramolecular and two intermolecular C—F···Cg interactions (Table 2).

Experimental

Both Tp and Bp ligands were prepared as previously reported (Gorun et al., 2000). To a flask containing 10 ml of acetonitrile, 60 mg of Co(Bp)2 (0.088 mmol) was disssolved to give a red-purple solution. Then 44 mg of KTp (0.088 mmol) was added and the mixture was allowed to stir for 10 min. giving little color change. The mixture was filtered to remove any solids and yielded a clear red-purple solution, which was left to evaporate slowly. Upon evaporation, a major dichroic red-orange phase (compound (I)) was separated mechanically and characterized. IR (KBr pellet, cm-1); 2570(Tp, B—H, w), 2492(Bp, B—H, w), 2217(Bp, B—H···Co, w), 1471(s), 1262(s), 1163(s), 1126(s), 1002(s), 800(m), 650(m).

Refinement

Hydrogen atoms of the methyl groups were located on difference Fiourier maps and were restrained. H atoms of the pyrrole fragments were positioned geometrically using a riding model, with C—H = 0.98 Å for methyl H atoms, 0.95 Å for pyrrole H atoms, and with Uiso(H) = 1.2 Ueq(C). B—H hydrogen atom coordinates and isotropic displacement parameters were refined.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound showing displacement ellipsoids drawn at the 35% probability level. H atoms are shown as spheres of arbitrary radius.

Crystal data

[Co(C10H10BF6N4)(C15H13BF9N6)] F(000) = 3320
Mr = 829.08 Dx = 1.631 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 910 reflections
a = 18.593 (2) Å θ = 2.2–22.4°
b = 12.1167 (13) Å µ = 0.63 mm1
c = 30.720 (3) Å T = 298 K
β = 102.721 (2)° Prism, orange-red
V = 6751.1 (13) Å3 0.28 × 0.24 × 0.12 mm
Z = 8

Data collection

Bruker SMART CCD area-detector diffractometer 7431 independent reflections
Radiation source: fine-focus sealed tube 5522 reflections with I > 2σ(I)
graphite Rint = 0.032
φ and ω scans θmax = 27.1°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Blessing, 1995) h = −23→23
Tmin = 0.875, Tmax = 1.00 k = −15→15
32390 measured reflections l = −38→39

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)] = 0.059 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.167 H atoms treated by a mixture of independent and constrained refinement
S = 1.00 w = 1/[σ2(Fo2) + (0.0985P)2 + 6.350P] where P = (Fo2 + 2Fc2)/3
7431 reflections (Δ/σ)max = 0.001
495 parameters Δρmax = 0.69 e Å3
0 restraints Δρmin = −0.32 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
Co1 0.28653 (2) 0.88792 (3) 0.876253 (13) 0.04318 (14)
F1 0.2096 (2) 1.0806 (3) 0.97276 (12) 0.1186 (11)
F2 0.16548 (16) 0.9517 (3) 1.00620 (9) 0.1087 (10)
F3 0.15337 (14) 0.9479 (3) 0.93573 (9) 0.1045 (9)
F4 0.34590 (19) 1.0689 (3) 0.81275 (12) 0.1270 (12)
F5 0.4369 (3) 1.0278 (4) 0.78800 (13) 0.178 (2)
F6 0.4449 (3) 1.1573 (3) 0.83096 (17) 0.1721 (19)
F7 0.15694 (15) 0.6605 (3) 0.85333 (12) 0.1158 (11)
F8 0.18416 (17) 0.4977 (2) 0.84101 (12) 0.1135 (10)
F9 0.1996 (2) 0.6240 (3) 0.79751 (10) 0.1371 (14)
F10 0.38793 (14) 0.7600 (3) 0.81139 (9) 0.1108 (11)
F11 0.33643 (17) 0.6704 (3) 0.75392 (12) 0.1122 (10)
F12 0.38456 (17) 0.8212 (3) 0.74664 (13) 0.1245 (12)
F13 0.36640 (15) 1.1157 (2) 0.93361 (10) 0.1001 (9)
F14 0.36229 (18) 1.2527 (3) 0.89093 (12) 0.1275 (12)
F15 0.3115 (2) 1.2626 (3) 0.94472 (13) 0.1412 (14)
N1 0.30398 (14) 0.8830 (2) 0.94819 (8) 0.0483 (6)
N2 0.36749 (14) 0.8317 (2) 0.96912 (8) 0.0500 (6)
N3 0.40019 (15) 0.9216 (2) 0.88139 (9) 0.0533 (6)
N4 0.44793 (14) 0.8664 (2) 0.91406 (9) 0.0520 (6)
N5 0.30701 (14) 0.7122 (2) 0.88605 (9) 0.0488 (6)
N6 0.37587 (15) 0.6891 (2) 0.91109 (8) 0.0509 (6)
N7 0.25381 (13) 0.8603 (2) 0.80721 (8) 0.0482 (6)
N8 0.18320 (13) 0.8959 (2) 0.79314 (9) 0.0502 (6)
N9 0.24139 (13) 1.0495 (2) 0.87252 (8) 0.0483 (6)
N10 0.17078 (13) 1.0446 (2) 0.84856 (8) 0.0476 (6)
C1 0.2001 (2) 0.9716 (4) 0.97340 (14) 0.0728 (10)
C2 0.2703 (2) 0.9112 (3) 0.98080 (11) 0.0546 (8)
C3 0.3116 (2) 0.8782 (3) 1.02190 (12) 0.0673 (10)
H3 0.2997 0.8882 1.0495 0.081*
C4 0.3728 (2) 0.8286 (3) 1.01390 (11) 0.0605 (8)
C5 0.4365 (3) 0.7800 (4) 1.04622 (13) 0.0868 (13)
H5A 0.4474 0.7084 1.0360 0.130*
H5B 0.4244 0.7733 1.0749 0.130*
H5C 0.4788 0.8271 1.0486 0.130*
C6 0.4145 (3) 1.0583 (4) 0.82312 (17) 0.0884 (13)
C7 0.4429 (2) 0.9846 (3) 0.86181 (13) 0.0643 (9)
C8 0.5164 (2) 0.9703 (4) 0.88129 (15) 0.0771 (11)
H8 0.5564 1.0047 0.8734 0.093*
C9 0.51825 (19) 0.8952 (3) 0.91462 (14) 0.0681 (10)
C10 0.5832 (2) 0.8483 (6) 0.94721 (19) 0.1079 (18)
H10A 0.5791 0.8656 0.9771 0.162*
H10B 0.6278 0.8797 0.9418 0.162*
H10C 0.5842 0.7697 0.9436 0.162*
C11 0.2065 (2) 0.6009 (3) 0.83940 (14) 0.0686 (10)
C12 0.2820 (2) 0.6161 (3) 0.86740 (11) 0.0561 (8)
C13 0.3333 (2) 0.5337 (3) 0.87903 (13) 0.0668 (9)
H13 0.3286 0.4603 0.8700 0.080*
C14 0.3926 (2) 0.5815 (3) 0.90657 (12) 0.0630 (9)
C15 0.4641 (3) 0.5313 (4) 0.92941 (17) 0.0940 (14)
H15A 0.5040 0.5758 0.9241 0.141*
H15B 0.4679 0.4583 0.9179 0.141*
H15C 0.4665 0.5273 0.9609 0.141*
C16 0.3460 (2) 0.7703 (4) 0.77177 (13) 0.0711 (10)
C17 0.27437 (18) 0.8250 (3) 0.77033 (11) 0.0553 (8)
C18 0.2182 (2) 0.8380 (3) 0.73323 (12) 0.0637 (9)
H18 0.2188 0.8197 0.7039 0.076*
C19 0.16104 (19) 0.8835 (3) 0.74851 (11) 0.0583 (8)
C20 0.0860 (2) 0.9147 (4) 0.72326 (14) 0.0837 (13)
H20A 0.0529 0.8539 0.7232 0.126*
H20B 0.0878 0.9329 0.6931 0.126*
H20C 0.0689 0.9775 0.7372 0.126*
C21 0.3222 (2) 1.1949 (3) 0.91380 (15) 0.0767 (11)
C22 0.25220 (19) 1.1548 (3) 0.88547 (11) 0.0553 (8)
C23 0.1893 (2) 1.2165 (3) 0.86992 (13) 0.0632 (9)
H23 0.1830 1.2915 0.8742 0.076*
C24 0.13797 (19) 1.1441 (3) 0.84681 (11) 0.0546 (8)
C25 0.0598 (2) 1.1627 (4) 0.82443 (15) 0.0764 (11)
H25A 0.0505 1.1322 0.7949 0.115*
H25B 0.0498 1.2405 0.8227 0.115*
H25C 0.0284 1.1275 0.8412 0.115*
B1 0.4190 (2) 0.7788 (3) 0.94208 (12) 0.0532 (8)
B2 0.1443 (2) 0.9287 (3) 0.83098 (13) 0.0528 (8)
H1B 0.4671 (19) 0.741 (3) 0.9652 (12) 0.060 (9)*
H21B 0.1701 (18) 0.870 (3) 0.8601 (12) 0.055 (9)*
H22B 0.085 (2) 0.929 (3) 0.8187 (12) 0.061 (9)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Co1 0.0438 (2) 0.0430 (2) 0.0410 (2) 0.00260 (16) 0.00549 (15) 0.00325 (16)
F1 0.143 (3) 0.0821 (18) 0.145 (3) 0.0403 (18) 0.063 (2) 0.0102 (18)
F2 0.1070 (19) 0.156 (3) 0.0809 (17) 0.0325 (19) 0.0585 (15) 0.0171 (17)
F3 0.0719 (15) 0.173 (3) 0.0713 (16) 0.0321 (17) 0.0217 (13) −0.0014 (17)
F4 0.103 (2) 0.150 (3) 0.122 (3) −0.007 (2) 0.0127 (19) 0.072 (2)
F5 0.238 (5) 0.208 (5) 0.111 (3) 0.051 (4) 0.089 (3) 0.060 (3)
F6 0.196 (4) 0.096 (2) 0.207 (5) −0.045 (3) 0.007 (3) 0.055 (3)
F7 0.0792 (17) 0.095 (2) 0.161 (3) −0.0026 (15) 0.0009 (18) −0.042 (2)
F8 0.110 (2) 0.0618 (14) 0.163 (3) −0.0306 (14) 0.018 (2) −0.0054 (16)
F9 0.129 (3) 0.192 (4) 0.0765 (19) −0.080 (2) −0.0068 (17) 0.014 (2)
F10 0.0732 (15) 0.178 (3) 0.0759 (16) 0.0625 (18) 0.0036 (13) −0.0179 (17)
F11 0.108 (2) 0.093 (2) 0.137 (3) 0.0313 (16) 0.0305 (18) −0.0323 (18)
F12 0.100 (2) 0.135 (3) 0.162 (3) 0.0265 (19) 0.080 (2) 0.032 (2)
F13 0.0914 (17) 0.0696 (15) 0.113 (2) −0.0057 (13) −0.0352 (15) −0.0066 (13)
F14 0.115 (2) 0.119 (2) 0.135 (3) −0.054 (2) −0.002 (2) 0.019 (2)
F15 0.136 (3) 0.120 (2) 0.144 (3) 0.008 (2) −0.020 (2) −0.084 (2)
N1 0.0522 (14) 0.0476 (13) 0.0450 (13) 0.0039 (11) 0.0104 (11) 0.0029 (11)
N2 0.0582 (15) 0.0491 (14) 0.0400 (13) 0.0015 (12) 0.0047 (11) 0.0040 (11)
N3 0.0535 (15) 0.0562 (15) 0.0500 (14) −0.0023 (12) 0.0106 (12) 0.0088 (12)
N4 0.0429 (13) 0.0603 (16) 0.0512 (15) −0.0009 (11) 0.0065 (11) −0.0004 (12)
N5 0.0528 (14) 0.0433 (13) 0.0492 (14) 0.0012 (11) 0.0088 (11) 0.0015 (11)
N6 0.0626 (16) 0.0455 (14) 0.0437 (13) 0.0090 (12) 0.0097 (12) 0.0072 (11)
N7 0.0433 (13) 0.0543 (14) 0.0451 (13) 0.0074 (11) 0.0058 (10) −0.0027 (11)
N8 0.0422 (13) 0.0571 (15) 0.0476 (14) 0.0037 (11) 0.0022 (10) −0.0063 (11)
N9 0.0477 (13) 0.0472 (14) 0.0454 (13) 0.0040 (11) 0.0007 (11) 0.0004 (11)
N10 0.0440 (13) 0.0531 (14) 0.0448 (13) 0.0069 (11) 0.0076 (10) 0.0010 (11)
C1 0.083 (3) 0.081 (3) 0.062 (2) 0.013 (2) 0.034 (2) 0.001 (2)
C2 0.068 (2) 0.0515 (18) 0.0476 (17) −0.0029 (15) 0.0201 (15) −0.0016 (13)
C3 0.092 (3) 0.069 (2) 0.0425 (17) 0.002 (2) 0.0194 (17) −0.0003 (16)
C4 0.077 (2) 0.058 (2) 0.0428 (17) −0.0026 (17) 0.0049 (16) −0.0010 (14)
C5 0.102 (3) 0.105 (3) 0.0439 (19) 0.014 (3) −0.005 (2) 0.006 (2)
C6 0.095 (3) 0.085 (3) 0.095 (3) −0.012 (3) 0.041 (3) 0.022 (3)
C7 0.068 (2) 0.063 (2) 0.065 (2) −0.0081 (17) 0.0233 (17) 0.0013 (17)
C8 0.063 (2) 0.088 (3) 0.087 (3) −0.020 (2) 0.032 (2) −0.005 (2)
C9 0.0462 (18) 0.085 (3) 0.073 (2) −0.0031 (17) 0.0143 (16) −0.015 (2)
C10 0.042 (2) 0.167 (5) 0.107 (4) −0.002 (3) −0.001 (2) 0.011 (4)
C11 0.081 (3) 0.053 (2) 0.071 (2) −0.0135 (18) 0.016 (2) −0.0053 (17)
C12 0.075 (2) 0.0457 (17) 0.0487 (17) −0.0050 (16) 0.0167 (16) −0.0002 (14)
C13 0.093 (3) 0.0423 (17) 0.065 (2) 0.0041 (18) 0.017 (2) −0.0015 (16)
C14 0.086 (3) 0.0514 (18) 0.0540 (19) 0.0207 (18) 0.0209 (18) 0.0124 (15)
C15 0.109 (3) 0.079 (3) 0.091 (3) 0.045 (3) 0.015 (3) 0.013 (2)
C16 0.069 (2) 0.084 (3) 0.064 (2) 0.020 (2) 0.0221 (19) −0.001 (2)
C17 0.0560 (18) 0.060 (2) 0.0492 (17) 0.0090 (15) 0.0106 (14) −0.0003 (15)
C18 0.068 (2) 0.075 (2) 0.0458 (18) 0.0087 (19) 0.0090 (16) −0.0024 (16)
C19 0.0547 (18) 0.069 (2) 0.0460 (17) 0.0036 (16) −0.0002 (14) −0.0044 (15)
C20 0.062 (2) 0.115 (4) 0.063 (2) 0.016 (2) −0.0099 (18) −0.011 (2)
C21 0.085 (3) 0.050 (2) 0.085 (3) −0.009 (2) −0.003 (2) −0.003 (2)
C22 0.067 (2) 0.0434 (16) 0.0527 (18) 0.0017 (15) 0.0069 (15) 0.0021 (14)
C23 0.077 (2) 0.0462 (17) 0.068 (2) 0.0150 (17) 0.0185 (18) 0.0057 (16)
C24 0.0571 (18) 0.0566 (18) 0.0516 (18) 0.0141 (15) 0.0153 (14) 0.0050 (14)
C25 0.060 (2) 0.084 (3) 0.087 (3) 0.023 (2) 0.020 (2) 0.017 (2)
B1 0.055 (2) 0.057 (2) 0.0445 (18) 0.0105 (17) 0.0045 (15) 0.0072 (16)
B2 0.0422 (18) 0.060 (2) 0.056 (2) −0.0015 (16) 0.0101 (15) −0.0080 (17)

Geometric parameters (Å, °)

Co1—N7 2.100 (3) C2—C3 1.384 (5)
Co1—H21B 2.12 (3) C3—C4 1.356 (5)
Co1—N9 2.124 (3) C3—H3 0.9300
Co1—N3 2.124 (3) C4—C5 1.489 (5)
Co1—N1 2.163 (3) C5—H5A 0.9600
Co1—N5 2.172 (3) C5—H5B 0.9600
F1—C1 1.333 (5) C5—H5C 0.9600
F2—C1 1.331 (4) C6—C7 1.487 (6)
F3—C1 1.316 (5) C7—C8 1.376 (6)
F4—C6 1.252 (6) C8—C9 1.365 (6)
F5—C6 1.293 (6) C8—H8 0.9300
F6—C6 1.325 (6) C9—C10 1.500 (6)
F7—C11 1.315 (5) C10—H10A 0.9600
F8—C11 1.322 (4) C10—H10B 0.9600
F9—C11 1.295 (5) C10—H10C 0.9600
F10—C16 1.298 (5) C11—C12 1.487 (5)
F11—C16 1.324 (5) C12—C13 1.373 (5)
F12—C16 1.317 (5) C13—C14 1.363 (6)
F13—C21 1.321 (5) C13—H13 0.9300
F14—C21 1.331 (5) C14—C15 1.490 (6)
F15—C21 1.303 (5) C15—H15A 0.9600
N1—C2 1.337 (4) C15—H15B 0.9600
N1—N2 1.364 (4) C15—H15C 0.9600
N2—C4 1.358 (4) C16—C17 1.480 (5)
N2—B1 1.538 (5) C17—C18 1.375 (5)
N3—C7 1.337 (4) C18—C19 1.368 (5)
N3—N4 1.360 (4) C18—H18 0.9300
N4—C9 1.350 (4) C19—C20 1.488 (5)
N4—B1 1.538 (5) C20—H20A 0.9600
N5—C12 1.335 (4) C20—H20B 0.9600
N5—N6 1.370 (4) C20—H20C 0.9600
N6—C14 1.354 (4) C21—C22 1.480 (5)
N6—B1 1.547 (5) C22—C23 1.381 (5)
N7—C17 1.343 (4) C23—C24 1.373 (5)
N7—N8 1.359 (3) C23—H23 0.9300
N8—C19 1.350 (4) C24—C25 1.483 (5)
N8—B2 1.551 (5) C25—H25A 0.9600
N9—C22 1.338 (4) C25—H25B 0.9600
N9—N10 1.358 (3) C25—H25C 0.9600
N10—C24 1.347 (4) B1—H1B 1.11 (3)
N10—B2 1.546 (5) B2—H21B 1.16 (3)
C1—C2 1.471 (5) B2—H22B 1.08 (4)
N7—Co1—H21B 72.2 (9) C9—C10—H10A 109.5
N7—Co1—N9 93.97 (10) C9—C10—H10B 109.5
H21B—Co1—N9 73.4 (9) H10A—C10—H10B 109.5
N7—Co1—N3 99.66 (10) C9—C10—H10C 109.5
H21B—Co1—N3 169.7 (9) H10A—C10—H10C 109.5
N9—Co1—N3 101.63 (10) H10B—C10—H10C 109.5
N7—Co1—N1 166.50 (10) F9—C11—F7 106.3 (4)
H21B—Co1—N1 98.7 (9) F9—C11—F8 106.2 (4)
N9—Co1—N1 92.81 (10) F7—C11—F8 105.0 (4)
N3—Co1—N1 90.37 (10) F9—C11—C12 115.0 (3)
N7—Co1—N5 89.25 (10) F7—C11—C12 112.6 (3)
H21B—Co1—N5 93.9 (9) F8—C11—C12 111.2 (3)
N9—Co1—N5 165.12 (10) N5—C12—C13 111.5 (3)
N3—Co1—N5 92.12 (10) N5—C12—C11 123.5 (3)
N1—Co1—N5 81.32 (10) C13—C12—C11 125.0 (3)
C2—N1—N2 105.2 (3) C14—C13—C12 105.9 (3)
C2—N1—Co1 140.2 (2) C14—C13—H13 127.1
N2—N1—Co1 114.44 (18) C12—C13—H13 127.1
C4—N2—N1 110.6 (3) N6—C14—C13 107.4 (3)
C4—N2—B1 128.4 (3) N6—C14—C15 123.2 (4)
N1—N2—B1 120.8 (2) C13—C14—C15 129.4 (4)
C7—N3—N4 104.9 (3) C14—C15—H15A 109.5
C7—N3—Co1 139.2 (2) C14—C15—H15B 109.5
N4—N3—Co1 115.93 (19) H15A—C15—H15B 109.5
C9—N4—N3 110.8 (3) C14—C15—H15C 109.5
C9—N4—B1 129.0 (3) H15A—C15—H15C 109.5
N3—N4—B1 120.0 (2) H15B—C15—H15C 109.5
C12—N5—N6 104.9 (3) F10—C16—F12 107.6 (4)
C12—N5—Co1 139.6 (2) F10—C16—F11 107.4 (4)
N6—N5—Co1 113.09 (19) F12—C16—F11 103.1 (3)
C14—N6—N5 110.3 (3) F10—C16—C17 114.9 (3)
C14—N6—B1 129.7 (3) F12—C16—C17 112.0 (3)
N5—N6—B1 119.7 (2) F11—C16—C17 111.0 (4)
C17—N7—N8 105.5 (2) N7—C17—C18 110.9 (3)
C17—N7—Co1 146.1 (2) N7—C17—C16 122.6 (3)
N8—N7—Co1 108.39 (18) C18—C17—C16 126.2 (3)
C19—N8—N7 110.2 (3) C19—C18—C17 105.5 (3)
C19—N8—B2 134.5 (3) C19—C18—H18 127.2
N7—N8—B2 114.9 (2) C17—C18—H18 127.2
C22—N9—N10 105.5 (2) N8—C19—C18 107.9 (3)
C22—N9—Co1 146.2 (2) N8—C19—C20 122.8 (3)
N10—N9—Co1 108.18 (18) C18—C19—C20 129.3 (3)
C24—N10—N9 111.0 (3) C19—C20—H20A 109.5
C24—N10—B2 133.8 (3) C19—C20—H20B 109.5
N9—N10—B2 115.2 (2) H20A—C20—H20B 109.5
F3—C1—F2 106.9 (4) C19—C20—H20C 109.5
F3—C1—F1 105.5 (4) H20A—C20—H20C 109.5
F2—C1—F1 106.2 (3) H20B—C20—H20C 109.5
F3—C1—C2 114.7 (3) F15—C21—F13 107.5 (4)
F2—C1—C2 110.7 (3) F15—C21—F14 104.3 (4)
F1—C1—C2 112.2 (4) F13—C21—F14 105.2 (4)
N1—C2—C3 110.6 (3) F15—C21—C22 112.3 (4)
N1—C2—C1 123.9 (3) F13—C21—C22 114.2 (3)
C3—C2—C1 125.4 (3) F14—C21—C22 112.6 (4)
C4—C3—C2 106.4 (3) N9—C22—C23 110.6 (3)
C4—C3—H3 126.8 N9—C22—C21 122.9 (3)
C2—C3—H3 126.8 C23—C22—C21 126.4 (3)
C3—C4—N2 107.1 (3) C24—C23—C22 105.8 (3)
C3—C4—C5 129.1 (3) C24—C23—H23 127.1
N2—C4—C5 123.8 (3) C22—C23—H23 127.1
C4—C5—H5A 109.5 N10—C24—C23 107.1 (3)
C4—C5—H5B 109.5 N10—C24—C25 123.0 (3)
H5A—C5—H5B 109.5 C23—C24—C25 129.9 (3)
C4—C5—H5C 109.5 C24—C25—H25A 109.5
H5A—C5—H5C 109.5 C24—C25—H25B 109.5
H5B—C5—H5C 109.5 H25A—C25—H25B 109.5
F4—C6—F5 108.3 (5) C24—C25—H25C 109.5
F4—C6—F6 108.8 (5) H25A—C25—H25C 109.5
F5—C6—F6 102.0 (4) H25B—C25—H25C 109.5
F4—C6—C7 115.3 (4) N4—B1—N2 110.5 (3)
F5—C6—C7 111.9 (5) N4—B1—N6 109.8 (3)
F6—C6—C7 109.6 (5) N2—B1—N6 109.0 (3)
N3—C7—C8 111.4 (3) N4—B1—H1B 108.1 (18)
N3—C7—C6 124.1 (4) N2—B1—H1B 109.6 (18)
C8—C7—C6 124.5 (4) N6—B1—H1B 109.8 (18)
C9—C8—C7 105.6 (3) N10—B2—N8 109.2 (3)
C9—C8—H8 127.2 N10—B2—H21B 104.2 (17)
C7—C8—H8 127.2 N8—B2—H21B 103.6 (17)
N4—C9—C8 107.4 (3) N10—B2—H22B 110.1 (19)
N4—C9—C10 123.0 (4) N8—B2—H22B 110.1 (19)
C8—C9—C10 129.6 (4) H21B—B2—H22B 119 (3)
N7—Co1—N1—C2 −78.5 (5) N4—N3—C7—C8 0.1 (4)
H21B—Co1—N1—C2 −32.0 (10) Co1—N3—C7—C8 179.3 (3)
N9—Co1—N1—C2 41.6 (3) N4—N3—C7—C6 178.6 (4)
N3—Co1—N1—C2 143.3 (3) Co1—N3—C7—C6 −2.2 (7)
N5—Co1—N1—C2 −124.6 (3) F4—C6—C7—N3 8.4 (7)
N7—Co1—N1—N2 97.9 (4) F5—C6—C7—N3 −116.0 (5)
H21B—Co1—N1—N2 144.4 (9) F6—C6—C7—N3 131.6 (5)
N9—Co1—N1—N2 −142.0 (2) F4—C6—C7—C8 −173.3 (5)
N3—Co1—N1—N2 −40.3 (2) F5—C6—C7—C8 62.3 (7)
N5—Co1—N1—N2 51.8 (2) F6—C6—C7—C8 −50.1 (6)
C2—N1—N2—C4 −0.2 (3) N3—C7—C8—C9 −0.4 (5)
Co1—N1—N2—C4 −177.8 (2) C6—C7—C8—C9 −178.8 (4)
C2—N1—N2—B1 175.2 (3) N3—N4—C9—C8 −0.5 (4)
Co1—N1—N2—B1 −2.4 (3) B1—N4—C9—C8 175.0 (3)
N7—Co1—N3—C7 49.1 (4) N3—N4—C9—C10 179.7 (4)
H21B—Co1—N3—C7 13 (5) B1—N4—C9—C10 −4.8 (6)
N9—Co1—N3—C7 −47.0 (4) C7—C8—C9—N4 0.5 (5)
N1—Co1—N3—C7 −140.0 (4) C7—C8—C9—C10 −179.7 (5)
N5—Co1—N3—C7 138.7 (4) N6—N5—C12—C13 −1.3 (4)
N7—Co1—N3—N4 −131.7 (2) Co1—N5—C12—C13 158.4 (3)
H21B—Co1—N3—N4 −168 (5) N6—N5—C12—C11 176.0 (3)
N9—Co1—N3—N4 132.1 (2) Co1—N5—C12—C11 −24.4 (5)
N1—Co1—N3—N4 39.2 (2) F9—C11—C12—N5 86.5 (5)
N5—Co1—N3—N4 −42.1 (2) F7—C11—C12—N5 −35.4 (5)
C7—N3—N4—C9 0.3 (4) F8—C11—C12—N5 −152.9 (3)
Co1—N3—N4—C9 −179.2 (2) F9—C11—C12—C13 −96.6 (5)
C7—N3—N4—B1 −175.7 (3) F7—C11—C12—C13 141.5 (4)
Co1—N3—N4—B1 4.8 (4) F8—C11—C12—C13 24.0 (5)
N7—Co1—N5—C12 −30.5 (3) N5—C12—C13—C14 0.5 (4)
H21B—Co1—N5—C12 41.5 (10) C11—C12—C13—C14 −176.7 (3)
N9—Co1—N5—C12 72.2 (5) N5—N6—C14—C13 −1.3 (4)
N3—Co1—N5—C12 −130.2 (3) B1—N6—C14—C13 172.8 (3)
N1—Co1—N5—C12 139.8 (3) N5—N6—C14—C15 179.5 (4)
N7—Co1—N5—N6 128.0 (2) B1—N6—C14—C15 −6.4 (6)
H21B—Co1—N5—N6 −159.9 (9) C12—C13—C14—N6 0.5 (4)
N9—Co1—N5—N6 −129.3 (4) C12—C13—C14—C15 179.6 (4)
N3—Co1—N5—N6 28.4 (2) N8—N7—C17—C18 0.3 (4)
N1—Co1—N5—N6 −61.7 (2) Co1—N7—C17—C18 −176.5 (3)
C12—N5—N6—C14 1.6 (3) N8—N7—C17—C16 −174.5 (3)
Co1—N5—N6—C14 −164.2 (2) Co1—N7—C17—C16 8.7 (7)
C12—N5—N6—B1 −173.2 (3) F10—C16—C17—N7 −0.7 (6)
Co1—N5—N6—B1 21.0 (3) F12—C16—C17—N7 −123.9 (4)
H21B—Co1—N7—C17 −156.8 (10) F11—C16—C17—N7 121.4 (4)
N9—Co1—N7—C17 132.1 (4) F10—C16—C17—C18 −174.6 (4)
N3—Co1—N7—C17 29.6 (4) F12—C16—C17—C18 62.2 (6)
N1—Co1—N7—C17 −107.9 (5) F11—C16—C17—C18 −52.5 (5)
N5—Co1—N7—C17 −62.4 (4) N7—C17—C18—C19 0.1 (4)
H21B—Co1—N7—N8 26.5 (10) C16—C17—C18—C19 174.6 (4)
N9—Co1—N7—N8 −44.6 (2) N7—N8—C19—C18 0.6 (4)
N3—Co1—N7—N8 −147.1 (2) B2—N8—C19—C18 −171.6 (4)
N1—Co1—N7—N8 75.4 (5) N7—N8—C19—C20 179.7 (4)
N5—Co1—N7—N8 120.8 (2) B2—N8—C19—C20 7.5 (6)
C17—N7—N8—C19 −0.5 (4) C17—C18—C19—N8 −0.4 (4)
Co1—N7—N8—C19 177.6 (2) C17—C18—C19—C20 −179.5 (4)
C17—N7—N8—B2 173.4 (3) N10—N9—C22—C23 −0.1 (4)
Co1—N7—N8—B2 −8.5 (3) Co1—N9—C22—C23 −175.9 (3)
N7—Co1—N9—C22 −134.0 (4) N10—N9—C22—C21 178.1 (3)
H21B—Co1—N9—C22 155.9 (10) Co1—N9—C22—C21 2.3 (6)
N3—Co1—N9—C22 −33.3 (4) F15—C21—C22—N9 −137.6 (4)
N1—Co1—N9—C22 57.6 (4) F13—C21—C22—N9 −14.9 (6)
N5—Co1—N9—C22 123.8 (5) F14—C21—C22—N9 105.1 (4)
N7—Co1—N9—N10 50.21 (19) F15—C21—C22—C23 40.3 (6)
H21B—Co1—N9—N10 −19.8 (10) F13—C21—C22—C23 163.0 (4)
N3—Co1—N9—N10 150.93 (18) F14—C21—C22—C23 −77.1 (5)
N1—Co1—N9—N10 −118.11 (19) N9—C22—C23—C24 0.6 (4)
N5—Co1—N9—N10 −51.9 (5) C21—C22—C23—C24 −177.5 (4)
C22—N9—N10—C24 −0.5 (3) N9—N10—C24—C23 0.8 (4)
Co1—N9—N10—C24 177.1 (2) B2—N10—C24—C23 178.0 (3)
C22—N9—N10—B2 −178.2 (3) N9—N10—C24—C25 −177.5 (3)
Co1—N9—N10—B2 −0.6 (3) B2—N10—C24—C25 −0.3 (6)
N2—N1—C2—C3 −0.1 (4) C22—C23—C24—N10 −0.8 (4)
Co1—N1—C2—C3 176.5 (3) C22—C23—C24—C25 177.3 (4)
N2—N1—C2—C1 178.3 (3) C9—N4—B1—N2 121.5 (4)
Co1—N1—C2—C1 −5.1 (6) N3—N4—B1—N2 −63.3 (4)
F3—C1—C2—N1 34.6 (5) C9—N4—B1—N6 −118.2 (4)
F2—C1—C2—N1 155.7 (4) N3—N4—B1—N6 57.0 (4)
F1—C1—C2—N1 −85.9 (5) C4—N2—B1—N4 −124.1 (3)
F3—C1—C2—C3 −147.2 (4) N1—N2—B1—N4 61.4 (4)
F2—C1—C2—C3 −26.2 (6) C4—N2—B1—N6 115.1 (3)
F1—C1—C2—C3 92.3 (5) N1—N2—B1—N6 −59.4 (4)
N1—C2—C3—C4 0.3 (4) C14—N6—B1—N4 112.3 (4)
C1—C2—C3—C4 −178.1 (4) N5—N6—B1—N4 −74.1 (3)
C2—C3—C4—N2 −0.4 (4) C14—N6—B1—N2 −126.5 (3)
C2—C3—C4—C5 178.7 (4) N5—N6—B1—N2 47.1 (4)
N1—N2—C4—C3 0.3 (4) C24—N10—B2—N8 111.9 (4)
B1—N2—C4—C3 −174.6 (3) N9—N10—B2—N8 −71.0 (3)
N1—N2—C4—C5 −178.7 (4) C19—N8—B2—N10 −109.7 (4)
B1—N2—C4—C5 6.3 (6) N7—N8—B2—N10 78.3 (3)

Table 2 Flourine interaction geometry (Å, °)

Cg1, Cg2, Cg3 and Cg4 are the centroids of the N3/N4/C9/C8/C7, N5/N6/C14/C13/C12, N7/N8/C19/C18/C17 and N9/N10/C24/C23/C22 rings, respectively.

C—F···Cg C—F F···Cg C···Cg C—F···Cg
C1—F1···Cg4 1.333 (5) 3.319 (4) 3.798 (5) 100.7 (3)
C1—F2···Cg2i 1.331 (4) 3.341 (3) 4.565 (4) 152.6 (2)
C1—F3···Cg4 1.316 (5) 3.273 (3) 3.798 (5) 103.3 (3)
C11—F9···Cg3 1.295 (5) 3.025 (4) 3.826 (4) 119.1 (3)
C16—F10···Cg1 1.298 (5) 3.252 (4) 4.279 (4) 135.8 (3)
C16—F10···Cg2 1.298 (5) 3.208 (3) 4.061 (4) 122.8 (2)
C16—F11···Cg4ii 1.324 (5) 3.605 (4) 4.467 (4) 123.0 (3)
C21—F13···Cg1 1.321 (5) 3.373 (3) 4.346 (5) 130.3 (3)

Symmetry codes: (i) 1/2-x, 3/2-y, -z; (ii) 1/2-x, 1/2+y, 1/2-z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2601).

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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. DOI: 10.1107/S1600536811021994/rz2601sup1.cif

e-67-0m911-sup1.cif (31.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021994/rz2601Isup2.hkl

e-67-0m911-Isup2.hkl (363.7KB, hkl)

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


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