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Crystallographic characterization of rare-earth cyano­tri­phenyl­borate complexes and the cyano­borates [NCBPh3]1−, [NCBPh2Me]1−, and [NCBPh2(μ-O)BPh2]1−

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aDepartment of Chemistry, University of California, Irvine, CA 92697-2025, USA
*Correspondence e-mail: wevans@uci.edu

Edited by S. Parkin, University of Kentucky, USA (Received 19 May 2021; accepted 3 July 2021; online 13 July 2021)

The investigation of the coordination chemistry of rare-earth metal complexes with cyanide ligands led to the isolation and crystallographic characterization of the LnIII cyano­tri­phenyl­borate complexes di­chlorido­(cyano­tri­phenyl­borato-κN)tetra­kis­(tetra­hydro­furan-κO)lanthanide(III), [LnCl2(C19H15BN)(C4H8O)4] [lanthanide (Ln) = dysprosium (Dy) and yttrium Y)] from reactions of LnCl3, KCN, and NaBPh4. Attempts to independently synthesize the tetra­ethyl­ammonium salt of (NCBPh3) from BPh3 and [NEt4][CN] in THF yielded crystals of the phenyl-substituted cyclic borate, tetra­ethyl­aza­nium 2,2,4,6-tetra­phenyl-1,3,5,2λ4,4,6-trioxatriborinan-2-ide, C8H20N+·C24H20B3O3 or [NEt4][B3(μ-O)3(C6H5)4]. The mechanochemical reaction of BPh3 and [NEt4][CN] without solvent produced crystals of tetra­ethyl­aza­nium cyano­diphenyl-λ4-boranyl di­phenyl­borinate, C8H20N+·C25H20B2NO or [NEt4][NCBPh2(μ-O)BPh2]. Reaction of BPh3 and KCN in THF in the presence of 2.2.2-cryptand (crypt) led to a crystal of bis­[(2.2.2-cryptand)potassium] 2,2,4,6-tetra­phenyl-1,3,5,2λ4,4,6-trioxatriborinan-2-ide cyano­methyl­diphenyl­borate tetra­hydro­furan disolvate, 2C18H36KN2O6+·C24H20B3O3·C14H13BN·2C4H8O or [K(crypt)]2[B3(μ-O)3(C6H5)4][NCBPh2Me]·2THF. The [NCBPh2(μ-O)BPh2]1− and (NCBPh2Me)1− anions have not been structurally characterized previously. The structure of 1-Y was refined as a two-component twin with occupancy factors 0.513 (1) and 0.487 (1). In 4, one solvent mol­ecule was disordered and included using multiple components with partial site-occupancy factors.

1. Chemical context

Attempts to make cationic rare-earth metal cyanide complexes of the type [Ln(CN)2(THF)x][BPh4] by combining LnCl3 with sodium tetra­phenyl­borate and potassium cyanide led to the isolation of the cyano­tri­phenyl­borate complexes LnCl2(THF)4(NCBPh3), 1-Ln (Ln = Dy, Y). Previously, transition-metal complexes of (NCBPh3)1− have been known to form from RhCl(PPh3)3, KCN, and BPh3 (Pankowski et al., 1996[Pankowski, M., Cabestaing, C. & Jaouen, G. (1996). J. Organomet. Chem. 516, 11-16.]; Carlton et al., 1998[Carlton, L., Weber, R. & Levendis, D. C. (1998). Inorg. Chem. 37, 1264-1271.]; Fernandes et al., 2002[Fernandes, M. A., Cîrcu, V., Weber, R., Varnali, T. & Carlton, L. (2002). J. Chem. Crystallogr. 32, 273-278.]) and from [Et4N][Cr(CN)6] and BPh3 (Schelter et al., 2005[Schelter, E. J., Shatruk, M., Heintz, R. A., Galán-Mascarós, J. R. & Dunbar, K. R. (2005). Chem. Commun. pp. 1417-1419.]).

Efforts to independently synthesize the tetra­ethyl­ammonium salt of the (NCBPh3)1− ligand generated a borate anion and two new cyano­phenyl­borate anions that, to our knowledge, have not been structurally characterized. Specifically, the reaction of BPh3 and [NEt4][CN] in THF led to crystals of the cyclic borate, [NEt4][B3(μ-O)3(C6H5)4], 2. When the analogous reaction was tried mechanochemically without solvent, the cyano­borate, [NEt4][NCBPh2(μ-O)BPh2], 3, was obtained. Reaction of BPh3 with KCN in the presence of 2.2.2-cryptand (crypt) gave crystals of the double salt [K(crypt)]2[B3(μ-O)3Ph4][NCBPh2Me], 4. The cyano­borate anions in 3 and 4 have not been previously characterized by X-ray crystallography. The ChemDraw representations of 1-Ln (Ln = Dy, Y), 2, 3, and 4 are depicted in the scheme below.

[Scheme 1]

2. Structural commentary

The displacement ellipsoid plot of LnCl2(THF)4(NCBPh3) 1-Ln (Ln = Dy, Y) is depicted in Fig. 1[link] and the structural parameters are tabulated in Table 1[link]. 1-Dy and 1-Y crystallize in the P[\overline{1}] space group and are isomorphous. The geometry around the LnIII ions is distorted penta­gonal bipyramidal. The C1—N1 bond distances are 1.141 (3) and 1.144 (4) Å in 1-Dy and 1-Y, respectively. These distances are consistent with a C≡N triple bond (Allen et al., 1987[Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, 2, S1-S19.]). The 178.7 (3) and 178.4 (3)° N1—C1—B1 bond angles in 1-Dy and 1-Y, respectively, are also consistent with a C≡N triple bond. The C1—N1—Ln1 angles are 163.92 (19) and 164.6 (3)° in 1-Dy and 1-Y, respectively. In comparison, the titanium complex, [(η5-C5H5)2Ti(η2-COR)(NCBPh3)], has a C—N distance of 1.14 (2) Å, an N—C—B angle of 176.8 (16)°, and a C—N—Ti angle of 169.1 (13)° (Pankowski et al., 1996[Pankowski, M., Cabestaing, C. & Jaouen, G. (1996). J. Organomet. Chem. 516, 11-16.]). The chromium complex [Et4N]3[Cr(NCBPh3)6] has C—N distances of 1.127 (5), 1.100 (5), and 1.150 (5) Å, N—C—B angles of 178.9 (4), 176.8 (4), and 179.8 (5)°, and Cr—N—C angles of 174.8 (3), 175.4 (3), and 173.5 (3)° (Schelter et al., 2005[Schelter, E. J., Shatruk, M., Heintz, R. A., Galán-Mascarós, J. R. & Dunbar, K. R. (2005). Chem. Commun. pp. 1417-1419.]). The B—C(CN) and B—C(phen­yl) distances in 1-Dy and 1-Y, respectively, are similar to those reported in transition-metal complexes with [NCBPh3]1− ligands (Pankowski et al., 1996[Pankowski, M., Cabestaing, C. & Jaouen, G. (1996). J. Organomet. Chem. 516, 11-16.]; Fernandes et al., 2002[Fernandes, M. A., Cîrcu, V., Weber, R., Varnali, T. & Carlton, L. (2002). J. Chem. Crystallogr. 32, 273-278.]).

Table 1
Selected bond lengths and angles (Å, °) for 1-Dy and 1-Y

  1-Dy 1-Y
Ln1—O1 2.3790 (18) 2.369 (2)
Ln1—O2 2.3838 (17) 2.370 (2)
Ln1—O3 2.4022 (16) 2.390 (2)
Ln1—O4 2.3932 (17) 2.382 (2)
Ln1—N1 2.431 (2) 2.420 (3)
Ln1—Cl1 2.5888 (6) 2.5803 (9)
Ln1—Cl2 2.5835 (6) 2.5730 (8)
N1—C1 1.141 (3) 1.144 (4)
B1—C1 1.621 (3) 1.629 (4)
B1—C18 1.625 (3) 1.630 (5)
B1—C24 1.632 (4) 1.626 (5)
B1—C30 1.641 (3) 1.642 (5)
     
C1—N1—Ln1 163.92 (19) 164.6 (3)
N1—C1—B1 178.7 (3) 178.4 (3)
[Figure 1]
Figure 1
Displacement ellipsoid plot of DyCl2(THF)4(NCBPh3), 1-Dy, drawn at the 30% probability level.

The displacement ellipsoid plots of [NEt4][B3(μ-O)3(C6H5)4], 2, [NEt4][NCBPh2(μ-O)BPh2], 3, and [K(crypt)]2[B3(μ-O)3(C6H5)4][NCBPh2Me], 4, are shown below in Figs. 2[link], 3[link] and 4[link], respectively, and the structural parameters are tabulated in Table 1[link]. Both 2 and 4 contain a non-planar anionic tetra­phenyl­boroxinate ring as reported previously in the tetra­methyl­ammonium salt, [NMe4][B3(μ-O)3(C6H5)4] (Kliegel et al., 1986[Kliegel, W., Motzkus, H.-W., Rettig, S. J. & Trotter, J. (1986). Can. J. Chem. 64, 507-513.]). While complex 2 is a tetra­ethyl­ammonium salt of the tetra­phenyl­boroxinate anion, complex 4 is a double salt with the second anion being [NCBPh2Me]1−. There are no crystallographically characterized examples of this anion in the literature to our knowledge. Complex 3 contains a [Ph2B(μ-O)BPh2CN]1− anion, differing both from the cyclic B3O3 phenyl­boroxinate anions found in 2 and 4 and from the [NCBPh2Me]1− anion in 4. We found no crystallographically characterized examples of this anion in the literature.

[Figure 2]
Figure 2
Displacement ellipsoid plot of 2, [NEt4][B3(μ-O)3(C6H5)4], drawn at the 30% probability level. The disorder in the [NEt4]+ cation is omitted for clarity.
[Figure 3]
Figure 3
Displacement ellipsoid plot of 3, [NEt4][NCBPh2(μ-O)BPh2], drawn at the 50% probability level.
[Figure 4]
Figure 4
Displacement ellipsoid plot of 4, [K(crypt)]2[B3(μ-O)3(C6H5)4][NCBPh2Me], drawn at the 50% probability level.

The O—B—O and B—O—B angles range from 110.4 (1) to 122.5 (2)° for 2 and range from 109.9 (5) to 123.3 (5)° for 4, both ranges are similar to those in [NMe4][B3(μ-O)3(C6H5)4]. The 1.497 (2) and 1.504 (2) Å B—O bonds involving four-coordinate B1 in 2 are longer than the other four B—O bond distances involving three-coordinate boron, which range from 1.333 (2) Å to 1.399 (2) Å for 2. Similar distances are found in 4.

Inter­estingly, though the B–C(CN) and B–C(phen­yl) distances for 4 are similar to those of the [NCBPh3] anion in 1-Ln, the N—C—B angle of 171.6 (9)° in 4 is less linear than the N—C—B angles in 1-Ln and in 3, 178 and 177.10 (13)°, respectively.

Both the C—N and B—C(CN) lengths in 3 and 4 are similar to those in 1-Ln. The 1.488 (10) Å B4—C(Me) distance in 4 is much shorter than the reported B—C(Me) distances in [BMe4] [1.639 (2) to 1.648 (2) Å] (Zhu & Kochi, 1999[Zhu, D. & Kochi, J. K. (1999). Organometallics, 18, 161-172.]), [BPh3Me] [1.653 (2) Å] (Zhu & Kochi, 1999[Zhu, D. & Kochi, J. K. (1999). Organometallics, 18, 161-172.]), and [FcB(MesF)(Me)(CN)] [1.628 (5) Å] (Broomsgrove et al., 2010[Broomsgrove, A. E. J., Addy, D. A., Di Paolo, A., Morgan, I. R., Bresner, C., Chislett, V., Fallis, I. A., Thompson, A. L., Vidovic, D. & Aldridge, S. (2010). Inorg. Chem. 49, 157-173.]). The B4—C(Me) distance is also shorter than the 1.636 (2) and 1.614 (10) Å B—C(CN) distances in 3 and 4, respectively. The 1.633 (11) and 1.648 (11) Å B4—C(phen­yl) distances are similar to the other B—C(phen­yl) distances in the structures reported here.

3. Supra­molecular features

There are no notable supra­molecular features in 1-Ln, 2, 3, or 4.

4. Database survey

The Cambridge Structural Database contains 14 known structures of transition metal complexes with the [NCBPh3]1− ligand found in 1-Ln or related [NCB(C6F5)3]1− ligands, including titanium (Pankowski et al., 1996[Pankowski, M., Cabestaing, C. & Jaouen, G. (1996). J. Organomet. Chem. 516, 11-16.], CSD refcode: TEXLEN), chromium (Schelter et al., 2005[Schelter, E. J., Shatruk, M., Heintz, R. A., Galán-Mascarós, J. R. & Dunbar, K. R. (2005). Chem. Commun. pp. 1417-1419.], CSD Refcode: XAKCUI), iron (Vei et al., 2003[Vei, I. C., Pascu, S. I., Green, M. L. H., Green, J. C., Schilling, R. E., Anderson, G. D. W. & Rees, L. H. (2003). Dalton Trans. pp. 2550-2557.], CSD Refcode: TAGKUI), nickel (Brunkan et al., 2004[Brunkan, N. M., Brestensky, D. M. & Jones, W. D. (2004). J. Am. Chem. Soc. 126, 3627-3641.], CSD Refcode: AVOKAX), copper (Naza­renko et al., 1996[Nazarenko, A. Y., Belsky, V. K. & Streltsova, N. R. (1996). Zh. Neorg. Khim. 41, 1119-1123.], CSD Refcode: REYHEI) zirconium (Zhou et al., 2001[Zhou, J., Lancaster, S. J., Walker, D. A., Beck, S., Thornton-Pett, M. & Bochmann, M. (2001). J. Am. Chem. Soc. 123, 223-237.], CSD Refcode: YEQZEZ), and rhodium (Fernandes et al., 2002[Fernandes, M. A., Cîrcu, V., Weber, R., Varnali, T. & Carlton, L. (2002). J. Chem. Crystallogr. 32, 273-278.], CSD Refcode: XUTDIZ; Cornock et al., 1977[Cornock, M. C., Robertson, D. R., Stephenson, T. A., Jones, C. L., Milburn, G. H. W. & Sawyer, L. (1977). J. Organomet. Chem. 135, C50-C52.], CSD Refcode: CBORRH). There is also a crystallographically-characterized cerium cyano­tri­phenyl­borate complex, [Ce(LOEt)2(NCBPh3)2] (LOEt = [Co(η5-C5H5){P(O)(OEt)2}3]) (Au-Yeung et al., 2016[Au-Yeung, K. C., So, Y. M., Sung, H. H. Y., Williams, I. D. & Leung, W. H. (2016). Dalton Trans. 45, 18163-18170.], CSD Refcode: EYAZOV).

Other crystallographically characterized tetra­phenyl­boroxinates of the type found in 2 that are reported in the Cambridge Structural Database include [Me3NCH2CH2OH][B3(μ-O)3(C6H5)4] (Beckett et al., 2006[Beckett, M. A., Coles, S. J., Light, M. E., Fischer, L., Stiefvater-Thomas, B. M. & Varma, K. S. (2006). Polyhedron, 25, 1011-1016.], CSD Refcode: ICUWAF), [NEt3H][B3(μ-O)3(C6H5)4] (Kratzert & Krossing, 2018[Kratzert, D. & Krossing, I. (2018). J. Appl. Cryst. 51, 928-934.], CSD Refcode: HERJUM01), [(tBu3PAu)4P][B3(μ-O)3(C6H5)4] (Zeller et al., 1993[Zeller, E., Beruda, H. & Schmidbaur, H. (1993). Chem. Ber. 126, 2033-2036.], CSD Refcode: PEVZOF), [C6H11NMe3][B3(μ-O)3(C6H5)4] (Beckett et al., 2018[Beckett, M. A., Coles, S. J., Horton, P. N., Jones, C. L., Marshall, E. V. & Perry, T. (2018). J. Organomet. Chem. 865, 72-79.], CSD Refcode: VEKVIT), [Ph2B{OCH2CH2N(Me)(CH2)n}2][B3(μ-O)3(C6H5)4] (n = 4, 5) (Beckett et al., 2010[Beckett, M. A., Bennett, E. L., Horton, P. N. & Hursthouse, M. B. (2010). J. Organomet. Chem. 695, 1080-1083.], CSD Refcode: VUTGUN), and [(η5-C5H5)Ni(η6-C6H6)Ni(η5-C5H5)][B3(μ-O)3(C6F5)5] (Priego et al., 2000[Priego, J. L., Doerrer, L. H., Rees, L. H. & Green, M. L. H. (2000). Chem. Commun. pp. 779-780.], CSD Refcode: MEKLAP).

There are no crystallographically characterized examples of the [Ph2B(μ-O)BPh2CN]1− and [NCBPh2Me]1− anions found in 3 and 4, respectively, in the literature.

5. Synthesis and crystallization

DyCl2(THF)4(NCBPh3), 1-Dy. In an argon-filled glovebox, KCN (42 mg, 0.642 mmol) was added to a stirred slurry of DyCl3 (75 mg, 0.279 mmol) in THF (10 mL). NaBPh4 (96 mg, 0.279 mmol) was added to the stirred slurry. The cloudy white solution was stirred overnight. The volatiles were removed under vacuum. The product was extracted into THF (10 mL) and centrifuged to remove white solids. The clear colorless solution had its volatiles removed under vacuum. The product was isolated as a colorless powder. Colorless crystals of DyCl2(THF)4(NCBPh3), 1-Dy, suitable for X-ray diffraction, were isolated from a vapor diffusion of hexane into a concentrated THF solution at room temperature after 6 d.

YCl2(THF)4(NCBPh3), 1-Y. In an argon-filled glovebox, KCN (34 mg, 0.522 mmol) was stirred in THF (10 mL) to form a cloudy white slurry. After 4 h, YCl3 (51 mg, 0.260 mmol) was tapped into the stirred white slurry. After 5 min, a solution of NaBPh4 (89 mg, 0.260 mmol) in THF (8 mL) was added to the stirred slurry. The cloudy white slurry was stirred overnight. The white slurry was centrifuged. The clear, colorless supernatant was collected, and the centrifuge pellet was washed with THF (5 mL), and the wash was combined with the supernatant. The colorless solution had its volatiles removed under vacuum. The product was isolated as a colorless solid (107 mg). X-ray quality crystals were isolated from a vapor diffusion of hexane into a concentrated THF solution at room temperature after 10 d.

[NEt4][B3(μ-O)3(C6H5)4], 2. In an argon-filled glovebox, BPh3 (78 mg, 0.320 mmol) was tapped into a stirred slurry of Et4NCN (50 mg, 0.320 mmol) in THF (5 ml). THF (10 mL) was added to the slurry, and the solution was heated lightly on a hot plate to encourage the Et4NCN to dissolve. After the sample was heated lightly for about an hour, most of the white solids had dissolved. The solution was allowed to stir at room temperature overnight. The volatiles were removed under vacuum and the white solids were washed with toluene (2 mL) twice. The thick tacky colorless solids were extracted into THF. Colorless X-ray quality crystals of [NEt4][B3(μ-O)3(C6H5)4], 2, were grown from a slow evaporation of a THF solution at room temperature.

[NEt4][NCBPh2(μ-O)BPh2], 3. In an argon-filled glovebox, BPh3 and NEt4CN were added to a BMT-20-S tube drive along with 40 steel balls (6 mm). The reaction mixture was ball milled together for 40 minutes using an Ultra-Turrax Tube Drive at the maximum speed setting. After this time, the colorless solids were extracted into toluene and THF. The volatiles were removed under vacuum. X-ray quality colorless crystals of [NEt4][NCBPh2(μ-O)BPh2], 3, were grown from a slow evaporation of a concentrated THF solution at 258 K after a few days.

[K(crypt)]2[B3(μ-O)3(C6H5)4][NCBPh2Me], 4. In an argon-filled glovebox, 2.2.2-cryptand (156 mg, 0.413 mmol) and KCN (30 mg, 0.460 mmol) were stirred in THF (10 mL) for 2 h, which allowed most of the white solids to dissolve. A solution of BPh3 (100 mg, 0.413 mmol) in THF (5 mL) was added to this mixture and the combination was allowed to stir for 3 d. The volatiles were removed under vacuum from the clear and colorless solution. The sample was extracted into THF (20 mL) and volatiles were removed under vacuum. The product was isolated as a colorless solid (423 mg). Colorless X-ray quality crystals of [K(crypt)]2[B3(μ-O)3(C6H5)4][NCBPh2Me], 4, were obtained from a vapor diffusion of pentane into a concentrated THF solution at room temperature.

6. Refinement

General Structure Solution and Refinement. The analytical scattering factors (Wilson, 1992[Wilson, A. J. C. (1992). International Tables for Crystallography, Vol. C. Dordrecht: Kluwer Academic Publishers.]) for neutral atoms were used throughout the analysis. Hydrogen atoms were included using a riding model. DyCl2(THF)4(NCBPh3), 1-Dy: Data were collected using a 15 sec/frame scan time. There were no systematic absences nor any diffraction symmetry other than the Friedel condition. Atom C5 was disordered and included using multiple components with partial site-occupancy factors. YCl2(THF)4(NCBPh3), 1-Y: Data were collected using a 30 sec/frame scan time. There were no systematic absences nor any diffraction symmetry other than the Friedel condition. Disordered atoms were included using multiple components with partial site-occupancy-factors. The structure was refined as a two-component twin with occupancy factors 0.513 (1) and 0.487 (1). [NEt4][B3(μ-O)3(C6H5)4], 2: Data were collected using a 20 sec/frame scan time. The tetra­ethyl­ammonium ion was fully disordered. The disordered atoms were included using multiple components with partial site-occupancy factors. [NEt4][NCBPh2(μ-O)BPh2], 3: Data were collected using a 30 sec/frame scan time. [K(crypt)]2[B3(μ-O)3(C6H5)4][NCBPh2Me], 4: Data were collected using a 60 sec/frame scan time. There were two mol­ecules of tetra­hydro­furan solvent present. One solvent mol­ecule was disordered and included using multiple components with partial site-occupancy factors. Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

  1-Dy 1-Y 2 3 4
Crystal data
Chemical formula [DyCl2(C19H15BN)(C4H8O)4] [YCl2(C19H15BN)(C4H8O)4] C8H20N+·C24H20B3O3 C8H20N+·C25H20B2NO 2C18H36KN2O6+·C24H20B3O3·C14H13BN·2C4H8O
Mr 789.94 716.35 519.08 502.29 1570.27
Crystal system, space group Triclinic, P[\overline{1}] Triclinic, P[\overline{1}] Monoclinic, P21/n Monoclinic, P21/n Orthorhombic, Pca21
Temperature (K) 158 173 133 88 88
a, b, c (Å) 12.0043 (17), 12.5261 (17), 13.4913 (19) 12.0404 (9), 12.5428 (9), 13.4654 (10) 9.7245 (7), 18.3021 (13), 16.7716 (12) 11.0269 (8), 13.9387 (11), 18.8488 (14) 27.193 (2), 14.5520 (11), 21.2218 (16)
α, β, γ (°) 114.7161 (13), 101.2230 (16), 94.2256 (16) 114.6967 (8), 101.3142 (9), 94.3882 (9) 90, 101.5456 (9), 90 90, 100.6357 (10), 90 90, 90, 90
V3) 1780.0 (4) 1782.7 (2) 2924.6 (4) 2847.3 (4) 8397.7 (11)
Z 2 2 4 4 4
Radiation type Mo Kα Mo Kα Mo Kα Mo Kα Mo Kα
μ (mm−1) 2.29 1.82 0.07 0.07 0.18
Crystal size (mm) 0.39 × 0.33 × 0.26 0.32 × 0.20 × 0.13 0.37 × 0.33 × 0.23 0.28 × 0.27 × 0.22 0.45 × 0.33 × 0.28
 
Data collection
Diffractometer Bruker SMART APEXII CCD Bruker SMART APEXII CCD Bruker SMART APEXII CCD Bruker SMART APEXII CCD Bruker SMART APEXII CCD
Absorption correction Numerical (SADABS; Krause et al., 2015[Krause, L., Herbst-Irmer, R., Sheldrick, G. M. & Stalke, D. (2015). J. Appl. Cryst. 48, 3-10.]) Multi-scan (TWINABS; Sheldrick, 2012[Sheldrick, G. M. (2012). TWINABS. University of Göttingen, Germany.]) Multi-scan (SADABS; Krause et al., 2015[Krause, L., Herbst-Irmer, R., Sheldrick, G. M. & Stalke, D. (2015). J. Appl. Cryst. 48, 3-10.]) Multi-scan (SADABS; Krause et al., 2015[Krause, L., Herbst-Irmer, R., Sheldrick, G. M. & Stalke, D. (2015). J. Appl. Cryst. 48, 3-10.]) Multi-scan (SADABS; Krause et al., 2015[Krause, L., Herbst-Irmer, R., Sheldrick, G. M. & Stalke, D. (2015). J. Appl. Cryst. 48, 3-10.])
Tmin, Tmax 0.558, 0.696 0.576, 0.746 0.834, 0.862 0.715, 0.746 0.825, 0.862
No. of measured, independent and observed [I > 2σ(I)] reflections 21440, 8460, 7562 7988, 7988, 6188 31741, 5959, 5030 34768, 7242, 5500 85621, 15958, 14236
Rint 0.019 0.029 0.042 0.038
(sin θ/λ)max−1) 0.680 0.650 0.625 0.685 0.610
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.024, 0.061, 1.04 0.047, 0.102, 1.04 0.064, 0.179, 1.02 0.048, 0.119, 1.04 0.074, 0.209, 1.06
No. of reflections 8460 7988 5959 7242 15958
No. of parameters 406 425 442 347 988
No. of restraints 0 0 0 0 1
H-atom treatment H-atom parameters constrained H-atom parameters constrained H-atom parameters constrained H-atom parameters constrained H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 1.34, −0.89 0.64, −0.81 1.06, −0.47 0.41, −0.24 0.78, −0.34
Computer programs: APEX2 (Bruker, 2014[Bruker (2014). APEX2. Bruker AXS, Inc., Madison, Wisconsin, USA.]), SAINT (Bruker, 2013[Bruker (2013). SAINT. Bruker AXS, Inc., Madison, Wisconsin, USA.]), SHELXT2014/4 (Sheldrick, 2015a[Sheldrick, G. M. (2015a). Acta Cryst. A71, 3-8.]), SHELXL2014/7 (Sheldrick, 2015b[Sheldrick, G. M. (2015b). Acta Cryst. C71, 3-8.]), and SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]).

Supporting information


Computing details top

For all structures, data collection: APEX2 (Bruker, 2014); cell refinement: SAINT (Bruker, 2013); data reduction: SAINT (Bruker, 2013); program(s) used to solve structure: SHELXT2014/4 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 201); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Dichlorido(cyanotriphenylborato-κN)tetrakis(tetrahydrofuran-κO)dysprosium(III) (1-Dy) top
Crystal data top
[DyCl2(C19H15BN)(C4H8O)4]Z = 2
Mr = 789.94F(000) = 802
Triclinic, P1Dx = 1.474 Mg m3
a = 12.0043 (17) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.5261 (17) ÅCell parameters from 9908 reflections
c = 13.4913 (19) Åθ = 2.3–28.8°
α = 114.7161 (13)°µ = 2.29 mm1
β = 101.2230 (16)°T = 158 K
γ = 94.2256 (16)°Irregular, colorless
V = 1780.0 (4) Å30.39 × 0.33 × 0.26 mm
Data collection top
Bruker SMART APEXII CCD
diffractometer
7562 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.019
φ and ω scansθmax = 28.9°, θmin = 1.7°
Absorption correction: numerical
(SADABS; Krause et al., 2015)
h = 1616
Tmin = 0.558, Tmax = 0.696k = 1616
21440 measured reflectionsl = 1818
8460 independent reflections
Refinement top
Refinement on F2Primary atom site location: dual space
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.024Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.061H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0251P)2 + 2.2673P]
where P = (Fo2 + 2Fc2)/3
8460 reflections(Δ/σ)max = 0.002
406 parametersΔρmax = 1.34 e Å3
0 restraintsΔρmin = 0.89 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. A colorless crystal of approximate dimensions 0.255 x 0.332 x 0.391 mm was mounted in a cryoloop and transferred to a Bruker SMART APEX II diffractometer. The APEX2 program package was used to determine the unit-cell parameters and for data collection (15 sec/frame scan time for a sphere of diffraction data). The raw frame data was processed using SAINT and SADABS to yield the reflection data file. Subsequent calculations were carried out using the SHELXTL program. There were no systematic absences nor any diffraction symmetry other than the Friedel condition. The centrosymmetric triclinic space group P-1 was assigned and later determined to be correct.

The structure was solved by dual space methods and refined on F2 by full-matrix least-squares techniques. The analytical scattering factors for neutral atoms were used throughout the analysis. Hydrogen atoms were included using a riding model. Atom C(5) was disordered and included using multiple components with partial site-occupancy-factors.

Least-squares analysis yielded wR2 = 0.0609 and Goof = 1.042 for 406 variables refined against 8460 data (0.74Å), R1 = 0.0239 for those 7562 data with I > 2.0sigma(I).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Dy10.24691 (2)0.24994 (2)0.49865 (2)0.01889 (4)
Cl10.23261 (5)0.07841 (6)0.55751 (5)0.03227 (13)
Cl20.25400 (5)0.40466 (5)0.41894 (5)0.03005 (12)
O10.45097 (15)0.26894 (16)0.55203 (16)0.0342 (4)
O20.30435 (16)0.12131 (15)0.33601 (14)0.0316 (4)
O30.07375 (14)0.14589 (15)0.35225 (14)0.0287 (4)
O40.08323 (15)0.30171 (15)0.57396 (14)0.0288 (4)
N10.31345 (17)0.42077 (18)0.68261 (17)0.0284 (4)
B10.3578 (2)0.6482 (2)0.8573 (2)0.0236 (5)
C10.33280 (19)0.5144 (2)0.75535 (19)0.0247 (5)
C20.5339 (2)0.3715 (3)0.5732 (3)0.0376 (6)
H2A0.50010.44520.59820.045*
H2B0.56010.35960.50470.045*
C30.6319 (3)0.3779 (3)0.6651 (4)0.0676 (12)
H3A0.62080.42950.74020.081*
H3B0.70640.41000.65820.081*
C40.6293 (3)0.2511 (3)0.6487 (3)0.0465 (7)
H4A0.62490.24470.71860.056*0.65
H4B0.69850.22070.62560.056*0.65
H4C0.65210.20060.57930.056*0.35
H4D0.67840.24640.71430.056*0.35
C50.5180 (4)0.1813 (4)0.5532 (5)0.0455 (11)0.65
H5A0.53710.13970.47970.055*0.65
H5B0.47610.12170.56930.055*0.65
C5B0.5075 (7)0.2203 (9)0.6388 (9)0.046 (2)0.35
H5B10.48800.26090.71220.055*0.35
H5B20.48310.13300.60840.055*0.35
C60.2852 (4)0.0100 (3)0.2908 (3)0.0578 (9)
H6A0.20180.04330.26350.069*
H6B0.32000.03420.34930.069*
C70.3429 (3)0.0522 (3)0.1953 (3)0.0465 (7)
H7A0.30310.13180.13560.056*
H7B0.42490.05580.22180.056*
C80.3317 (3)0.0430 (3)0.1538 (3)0.0513 (8)
H8A0.38890.04400.11020.062*
H8B0.25320.03090.10660.062*
C90.3554 (3)0.1549 (3)0.2616 (2)0.0432 (7)
H9A0.43940.18360.29350.052*
H9B0.31950.21850.24950.052*
C100.0179 (2)0.0684 (2)0.3591 (2)0.0378 (6)
H10A0.07910.11270.38660.045*
H10B0.01250.03280.40970.045*
C110.0631 (2)0.0268 (2)0.2381 (2)0.0406 (6)
H11A0.01490.08990.21980.049*
H11B0.14400.06370.22400.049*
C120.0541 (3)0.0436 (3)0.1712 (3)0.0540 (9)
H12A0.03180.00470.10090.065*
H12B0.12880.06780.15150.065*
C130.0369 (3)0.1510 (3)0.2465 (2)0.0454 (7)
H13A0.10280.15040.21220.054*
H13B0.00530.22490.25800.054*
C140.0192 (3)0.3867 (3)0.5532 (3)0.0421 (7)
H14A0.05530.34490.49740.051*
H14B0.06360.43070.52320.051*
C150.0006 (4)0.4690 (5)0.6599 (3)0.0839 (15)
H15A0.07200.50150.64800.101*
H15B0.06520.53590.70310.101*
C160.0113 (4)0.3935 (5)0.7179 (4)0.0923 (17)
H16A0.09260.35530.69920.111*
H16B0.01520.44190.80050.111*
C170.0639 (3)0.2994 (3)0.6771 (3)0.0493 (8)
H17A0.13780.31960.73400.059*
H17B0.02400.21980.66100.059*
C180.3477 (2)0.7417 (2)0.8026 (2)0.0248 (5)
C190.3067 (2)0.7120 (2)0.6885 (2)0.0298 (5)
H19A0.28360.63040.63560.036*
C200.2988 (2)0.7998 (3)0.6504 (2)0.0370 (6)
H20A0.27130.77700.57220.044*
C210.3305 (2)0.9190 (3)0.7249 (3)0.0395 (6)
H21A0.32470.97830.69860.047*
C220.3708 (2)0.9512 (2)0.8386 (3)0.0383 (6)
H22A0.39211.03310.89120.046*
C230.3800 (2)0.8635 (2)0.8755 (2)0.0313 (5)
H23A0.40950.88710.95360.038*
C240.2584 (2)0.6512 (2)0.92518 (19)0.0254 (5)
C250.1699 (2)0.7173 (2)0.9233 (2)0.0337 (5)
H25A0.16870.76330.88230.040*
C260.0836 (2)0.7187 (3)0.9790 (3)0.0412 (6)
H26A0.02510.76500.97560.049*
C270.0830 (3)0.6528 (3)1.0393 (3)0.0425 (7)
H27A0.02470.65371.07800.051*
C280.1687 (3)0.5852 (3)1.0425 (2)0.0398 (6)
H28A0.16900.53921.08350.048*
C290.2542 (2)0.5840 (2)0.9863 (2)0.0318 (5)
H29A0.31170.53640.98910.038*
C300.4912 (2)0.67005 (19)0.9294 (2)0.0267 (5)
C310.5262 (2)0.7043 (2)1.0449 (2)0.0330 (6)
H31A0.46960.71371.08690.040*
C320.6433 (3)0.7251 (2)1.1005 (2)0.0414 (7)
H32A0.66460.74831.17920.050*
C330.7263 (2)0.7123 (2)1.0424 (3)0.0429 (7)
H33A0.80520.72581.08030.051*
C340.6955 (2)0.6797 (3)0.9283 (3)0.0424 (7)
H34A0.75300.67120.88740.051*
C350.5798 (2)0.6594 (2)0.8735 (2)0.0351 (6)
H35A0.55990.63730.79500.042*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Dy10.02183 (6)0.01583 (6)0.01804 (6)0.00100 (4)0.00370 (4)0.00748 (4)
Cl10.0365 (3)0.0313 (3)0.0369 (3)0.0028 (2)0.0059 (2)0.0243 (3)
Cl20.0376 (3)0.0231 (3)0.0322 (3)0.0012 (2)0.0053 (2)0.0169 (2)
O10.0244 (8)0.0269 (9)0.0423 (10)0.0024 (7)0.0038 (7)0.0090 (8)
O20.0381 (10)0.0284 (9)0.0259 (9)0.0075 (7)0.0121 (7)0.0076 (7)
O30.0256 (8)0.0307 (9)0.0256 (8)0.0050 (7)0.0001 (7)0.0128 (7)
O40.0305 (9)0.0291 (9)0.0296 (9)0.0063 (7)0.0119 (7)0.0136 (7)
N10.0272 (10)0.0246 (10)0.0259 (10)0.0018 (8)0.0032 (8)0.0061 (8)
B10.0278 (12)0.0190 (11)0.0197 (12)0.0026 (9)0.0018 (10)0.0064 (10)
C10.0231 (11)0.0264 (12)0.0236 (11)0.0030 (9)0.0035 (9)0.0114 (10)
C20.0244 (12)0.0460 (16)0.0486 (16)0.0008 (11)0.0057 (11)0.0292 (14)
C30.0453 (19)0.0471 (19)0.095 (3)0.0098 (15)0.0298 (19)0.040 (2)
C40.0424 (16)0.0489 (18)0.0525 (18)0.0083 (13)0.0032 (14)0.0301 (15)
C50.030 (2)0.034 (2)0.074 (4)0.0091 (18)0.011 (2)0.026 (2)
C5B0.028 (4)0.062 (6)0.066 (6)0.004 (4)0.000 (4)0.050 (5)
C60.084 (3)0.0343 (16)0.056 (2)0.0188 (16)0.0311 (19)0.0130 (15)
C70.0495 (17)0.0352 (15)0.0406 (16)0.0061 (13)0.0187 (13)0.0005 (13)
C80.059 (2)0.0543 (19)0.0323 (15)0.0081 (16)0.0211 (14)0.0070 (14)
C90.0504 (17)0.0402 (16)0.0393 (15)0.0044 (13)0.0254 (13)0.0123 (13)
C100.0328 (13)0.0355 (14)0.0384 (15)0.0075 (11)0.0026 (11)0.0149 (12)
C110.0354 (14)0.0273 (13)0.0456 (16)0.0037 (11)0.0010 (12)0.0096 (12)
C120.061 (2)0.0490 (18)0.0325 (15)0.0120 (15)0.0106 (14)0.0131 (14)
C130.0461 (17)0.0491 (17)0.0352 (15)0.0084 (13)0.0088 (12)0.0241 (14)
C140.0383 (15)0.0452 (16)0.0558 (18)0.0190 (13)0.0187 (13)0.0296 (15)
C150.090 (3)0.108 (4)0.050 (2)0.071 (3)0.017 (2)0.024 (2)
C160.076 (3)0.173 (5)0.082 (3)0.075 (3)0.059 (3)0.083 (4)
C170.0502 (18)0.070 (2)0.0479 (18)0.0171 (16)0.0252 (15)0.0390 (17)
C180.0245 (11)0.0263 (11)0.0255 (11)0.0049 (9)0.0063 (9)0.0131 (9)
C190.0277 (12)0.0361 (13)0.0260 (12)0.0054 (10)0.0061 (9)0.0145 (10)
C200.0308 (13)0.0594 (18)0.0356 (14)0.0129 (12)0.0094 (11)0.0335 (14)
C210.0312 (13)0.0515 (17)0.0590 (18)0.0146 (12)0.0155 (13)0.0432 (16)
C220.0389 (14)0.0310 (13)0.0511 (17)0.0080 (11)0.0114 (13)0.0236 (13)
C230.0377 (13)0.0269 (12)0.0300 (13)0.0056 (10)0.0068 (10)0.0140 (10)
C240.0320 (12)0.0189 (10)0.0195 (10)0.0008 (9)0.0037 (9)0.0047 (9)
C250.0355 (13)0.0343 (13)0.0364 (14)0.0083 (11)0.0094 (11)0.0198 (12)
C260.0359 (14)0.0423 (16)0.0524 (17)0.0136 (12)0.0165 (13)0.0241 (14)
C270.0428 (16)0.0451 (16)0.0454 (16)0.0057 (13)0.0207 (13)0.0217 (14)
C280.0503 (17)0.0371 (15)0.0388 (15)0.0045 (12)0.0145 (13)0.0224 (13)
C290.0403 (14)0.0238 (12)0.0313 (13)0.0048 (10)0.0096 (11)0.0120 (10)
C300.0327 (12)0.0144 (10)0.0262 (11)0.0002 (9)0.0018 (9)0.0071 (9)
C310.0423 (14)0.0218 (11)0.0271 (12)0.0062 (10)0.0012 (10)0.0074 (10)
C320.0518 (17)0.0247 (12)0.0311 (14)0.0065 (12)0.0122 (12)0.0065 (11)
C330.0317 (14)0.0248 (13)0.0570 (18)0.0016 (10)0.0095 (13)0.0131 (13)
C340.0300 (13)0.0360 (15)0.0563 (18)0.0002 (11)0.0028 (12)0.0201 (14)
C350.0316 (13)0.0351 (14)0.0367 (14)0.0007 (11)0.0016 (11)0.0180 (12)
Geometric parameters (Å, º) top
Dy1—O12.3790 (18)C7—C81.519 (5)
Dy1—O22.3838 (17)C8—C91.495 (4)
Dy1—O42.3932 (17)C10—C111.521 (4)
Dy1—O32.4022 (16)C11—C121.514 (4)
Dy1—N12.431 (2)C12—C131.498 (4)
Dy1—Cl22.5835 (6)C14—C151.456 (5)
Dy1—Cl12.5888 (6)C15—C161.470 (7)
O1—C51.411 (5)C16—C171.522 (5)
O1—C21.455 (3)C18—C191.397 (3)
O1—C5B1.597 (8)C18—C231.398 (3)
O2—C91.454 (3)C19—C201.396 (4)
O2—C61.476 (4)C20—C211.377 (4)
O3—C131.439 (3)C21—C221.384 (4)
O3—C101.455 (3)C22—C231.386 (4)
O4—C141.445 (3)C24—C251.397 (3)
O4—C171.465 (3)C24—C291.407 (3)
N1—C11.141 (3)C25—C261.390 (4)
B1—C11.621 (3)C26—C271.382 (4)
B1—C181.625 (3)C27—C281.385 (4)
B1—C241.632 (4)C28—C291.387 (4)
B1—C301.641 (3)C30—C311.396 (3)
C2—C31.505 (4)C30—C351.402 (4)
C3—C41.507 (4)C31—C321.407 (4)
C4—C5B1.450 (9)C32—C331.363 (5)
C4—C51.557 (6)C33—C341.380 (4)
C6—C71.499 (4)C34—C351.390 (4)
O1—Dy1—O273.01 (6)O1—C2—C3104.0 (2)
O1—Dy1—O4142.46 (6)C2—C3—C4105.0 (3)
O2—Dy1—O4143.59 (6)C5B—C4—C398.6 (4)
O1—Dy1—O3145.88 (6)C3—C4—C5103.7 (3)
O2—Dy1—O373.03 (6)O1—C5—C4105.1 (3)
O4—Dy1—O370.83 (6)C4—C5B—O1101.3 (5)
O1—Dy1—N173.26 (7)O2—C6—C7105.1 (3)
O2—Dy1—N1144.41 (7)C6—C7—C8102.4 (2)
O4—Dy1—N171.76 (6)C9—C8—C7102.1 (3)
O3—Dy1—N1140.64 (6)O2—C9—C8104.8 (2)
O1—Dy1—Cl294.03 (5)O3—C10—C11103.4 (2)
O2—Dy1—Cl285.89 (5)C12—C11—C10102.5 (2)
O4—Dy1—Cl296.37 (4)C13—C12—C11105.6 (2)
O3—Dy1—Cl286.87 (4)O3—C13—C12107.3 (2)
N1—Dy1—Cl285.47 (5)O4—C14—C15107.6 (3)
O1—Dy1—Cl187.73 (5)C14—C15—C16102.9 (4)
O2—Dy1—Cl189.32 (5)C15—C16—C17106.5 (3)
O4—Dy1—Cl185.53 (4)O4—C17—C16104.3 (3)
O3—Dy1—Cl188.55 (4)C19—C18—C23116.1 (2)
N1—Dy1—Cl1100.36 (5)C19—C18—B1126.0 (2)
Cl2—Dy1—Cl1174.169 (19)C23—C18—B1117.9 (2)
C5—O1—C2104.8 (2)C20—C19—C18121.4 (2)
C2—O1—C5B105.3 (3)C21—C20—C19120.8 (2)
C5—O1—Dy1129.0 (2)C20—C21—C22119.2 (2)
C2—O1—Dy1125.50 (15)C21—C22—C23119.7 (3)
C5B—O1—Dy1119.5 (3)C22—C23—C18122.8 (2)
C9—O2—C6108.8 (2)C25—C24—C29115.6 (2)
C9—O2—Dy1127.40 (16)C25—C24—B1122.3 (2)
C6—O2—Dy1123.67 (17)C29—C24—B1122.1 (2)
C13—O3—C10107.00 (19)C26—C25—C24122.8 (2)
C13—O3—Dy1128.45 (15)C27—C26—C25120.0 (3)
C10—O3—Dy1124.48 (15)C26—C27—C28119.1 (3)
C14—O4—C17107.9 (2)C27—C28—C29120.5 (3)
C14—O4—Dy1120.89 (15)C28—C29—C24122.1 (2)
C17—O4—Dy1126.17 (16)C31—C30—C35115.8 (2)
C1—N1—Dy1163.92 (19)C31—C30—B1125.4 (2)
C1—B1—C18108.07 (19)C35—C30—B1118.6 (2)
C1—B1—C24105.67 (19)C30—C31—C32121.6 (3)
C18—B1—C24111.50 (19)C33—C32—C31120.5 (3)
C1—B1—C30106.34 (19)C32—C33—C34119.8 (3)
C18—B1—C30108.93 (19)C33—C34—C35119.6 (3)
C24—B1—C30115.9 (2)C34—C35—C30122.7 (3)
N1—C1—B1178.7 (3)
Dichlorido(cyanotriphenylborato-κN)tetrakis(tetrahydrofuran-κO)ytterbium(III) (1-Y) top
Crystal data top
[YCl2(C19H15BN)(C4H8O)4]Z = 2
Mr = 716.35F(000) = 748
Triclinic, P1Dx = 1.334 Mg m3
a = 12.0404 (9) ÅMo Kα radiation, λ = 0.71073 Å
b = 12.5428 (9) ÅCell parameters from 9606 reflections
c = 13.4654 (10) Åθ = 2.3–27.1°
α = 114.6967 (8)°µ = 1.82 mm1
β = 101.3142 (9)°T = 173 K
γ = 94.3882 (9)°Prism, colorless
V = 1782.7 (2) Å30.32 × 0.20 × 0.13 mm
Data collection top
Bruker SMART APEXII CCD
diffractometer
7988 independent reflections
Radiation source: fine-focus sealed tube6188 reflections with I > 2σ(I)
φ and ω scansθmax = 27.5°, θmin = 1.7°
Absorption correction: multi-scan
(TWINABS; Sheldrick, 2012)
h = 1515
Tmin = 0.576, Tmax = 0.746k = 1614
7988 measured reflectionsl = 017
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.102H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0438P)2 + 0.9643P]
where P = (Fo2 + 2Fc2)/3
7988 reflections(Δ/σ)max < 0.001
425 parametersΔρmax = 0.64 e Å3
0 restraintsΔρmin = 0.80 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. A colorless crystal of approximate dimensions 0.126 x 0.198 x 0.324 mm was mounted on a glass fiber and transferred to a Bruker SMART APEX II diffractometer system. The APEX2 program package and the CELL_NOW were used to determine the unit-cell parameters. Data was collected using a 30 sec/frame scan time. The raw frame data was processed using SAINT3 and TWINABS to yield the reflection data file (HKLF5 format). Subsequent calculations were carried out using the SHELXTL program package. There were no systematic absences nor any diffraction symmetry other than the Friedel condition The centrosymmetric triclinic space group P-1 was assigned and later determined to be correct.

The structure was solved by direct methods and refined on F2 by full-matrix least-squares techniques. The analytical scattering factors for neutral atoms were used throughout the analysis. Hydrogen atoms were included using a riding model. Disordered atoms were included using multiple components with partial site-occupancy-factors.

Least-squares analysis yielded wR2 = 0.1023 and Goof = 1.037 for 425 variables refined against 7988 data (0.77 ), R1 = 0.0470 for those 6188 with I > 2.0sigma(I). The structure was refined as a two-component twin, BASF = 0.4868.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Y10.24658 (3)0.24946 (3)0.49747 (3)0.01941 (8)
Cl10.23233 (7)0.07981 (7)0.55775 (7)0.0330 (2)
Cl20.25375 (7)0.40279 (7)0.41725 (7)0.03054 (19)
O10.44949 (18)0.2696 (2)0.5508 (2)0.0338 (6)
O20.30323 (19)0.1206 (2)0.33612 (18)0.0304 (5)
O30.07439 (18)0.1455 (2)0.35125 (18)0.0291 (5)
O40.08446 (18)0.3011 (2)0.57256 (18)0.0291 (5)
N10.3129 (2)0.4202 (2)0.6805 (2)0.0273 (6)
B10.3570 (3)0.6480 (3)0.8568 (3)0.0242 (7)
C10.3324 (3)0.5138 (3)0.7540 (3)0.0249 (7)
C20.5324 (3)0.3724 (3)0.5732 (3)0.0368 (8)
H2A0.49860.44590.59800.044*
H2B0.55940.36110.50520.044*
C30.6292 (4)0.3788 (4)0.6661 (4)0.0612 (14)
H3A0.61730.42960.74110.073*
H3B0.70390.41170.66050.073*
C40.6265 (3)0.2520 (4)0.6489 (4)0.0481 (10)
H4A0.62160.24490.71850.058*0.65
H4B0.69580.22230.62630.058*0.65
H4C0.65160.20280.58060.058*0.35
H4D0.67400.24740.71540.058*0.35
C50.5161 (5)0.1826 (5)0.5525 (6)0.0425 (15)0.65
H5A0.53580.14140.47930.051*0.65
H5B0.47390.12270.56790.051*0.65
C5B0.5064 (10)0.2189 (15)0.6354 (15)0.065 (4)0.35
H5B10.48530.25620.70830.078*0.35
H5B20.48320.13120.60230.078*0.35
C60.2840 (4)0.0103 (3)0.2910 (4)0.0563 (12)
H6A0.20060.04360.26360.068*
H6B0.31850.03420.35000.068*
C70.3416 (3)0.0537 (3)0.1950 (3)0.0466 (10)
H7A0.30080.13280.13500.056*
H7B0.42300.05820.22160.056*
C80.3321 (4)0.0423 (4)0.1539 (3)0.0509 (11)
H8A0.39000.04350.11130.061*
H8B0.25430.03050.10580.061*
C90.3553 (3)0.1534 (3)0.2621 (3)0.0435 (10)
H9A0.43920.18190.29490.052*
H9B0.32040.21710.24970.052*
C100.0181 (3)0.0683 (3)0.3584 (3)0.0392 (9)
H10A0.07870.11310.38590.047*
H10B0.01200.03290.40930.047*
C110.0638 (3)0.0268 (3)0.2377 (3)0.0417 (9)
H11A0.14480.06300.22370.050*
H11B0.01650.09040.21960.050*
C120.0539 (4)0.0431 (4)0.1702 (3)0.0558 (12)
H12A0.03260.00590.09960.067*
H12B0.12780.06820.15070.067*
C130.0381 (3)0.1494 (4)0.2447 (3)0.0469 (10)
H13A0.10390.14720.21020.056*
H13B0.00800.22360.25550.056*
C140.0212 (3)0.3876 (3)0.5531 (3)0.0429 (9)
H14A0.06480.42920.52050.052*0.65
H14B0.05420.34620.49860.052*0.65
H14C0.03320.35220.47740.052*0.35
H14D0.07310.45850.56330.052*0.35
C150.0041 (7)0.4723 (7)0.6573 (6)0.0430 (17)0.65
H15A0.06640.50550.64460.052*0.65
H15B0.07080.53840.69860.052*0.65
C160.0078 (6)0.3991 (8)0.7203 (6)0.0461 (17)0.65
H16A0.08950.36490.70550.055*0.65
H16B0.02310.44850.80260.055*0.65
C15B0.0431 (15)0.4171 (17)0.6509 (18)0.071 (5)0.35
H15C0.00020.48980.71880.085*0.35
H15D0.12150.43090.62620.085*0.35
C16B0.0492 (13)0.3163 (16)0.6758 (13)0.061 (4)0.35
H16C0.06460.33640.75050.073*0.35
H16D0.10710.24750.61670.073*0.35
C170.0642 (4)0.2970 (4)0.6745 (3)0.0507 (11)
H17A0.13780.31260.73040.061*0.65
H17B0.02030.21850.65650.061*0.65
H17C0.07320.21840.67260.061*0.35
H17D0.11950.35980.74250.061*0.35
C180.3475 (3)0.7411 (3)0.8012 (2)0.0234 (6)
C190.3062 (3)0.7111 (3)0.6868 (3)0.0300 (7)
H19A0.28290.62950.63380.036*
C200.2984 (3)0.7984 (4)0.6489 (3)0.0373 (8)
H20A0.27060.77540.57050.045*
C210.3304 (3)0.9175 (4)0.7232 (3)0.0402 (9)
H21A0.32500.97640.69640.048*
C220.3703 (3)0.9503 (3)0.8368 (3)0.0377 (8)
H22A0.39141.03230.88930.045*
C230.3795 (3)0.8627 (3)0.8743 (3)0.0303 (7)
H23A0.40870.88650.95270.036*
C240.2577 (3)0.6505 (3)0.9236 (3)0.0258 (7)
C250.1695 (3)0.7157 (3)0.9213 (3)0.0336 (8)
H25A0.16850.76150.88010.040*
C260.0831 (3)0.7171 (4)0.9762 (3)0.0437 (9)
H26A0.02430.76260.97200.052*
C270.0831 (3)0.6515 (3)1.0372 (3)0.0435 (9)
H27A0.02500.65251.07610.052*
C280.1685 (3)0.5845 (3)1.0411 (3)0.0395 (9)
H28A0.16890.53901.08250.047*
C290.2534 (3)0.5837 (3)0.9850 (3)0.0314 (8)
H29A0.31080.53650.98810.038*
C300.4906 (3)0.6702 (3)0.9288 (3)0.0264 (7)
C310.5250 (3)0.7033 (3)1.0442 (3)0.0345 (8)
H31A0.46830.71131.08580.041*
C320.6417 (3)0.7251 (3)1.1004 (3)0.0446 (10)
H32A0.66290.74911.17950.053*
C330.7251 (3)0.7120 (3)1.0424 (4)0.0441 (10)
H33A0.80370.72451.08040.053*
C340.6941 (3)0.6806 (3)0.9286 (4)0.0426 (10)
H34A0.75110.67240.88740.051*
C350.5787 (3)0.6610 (3)0.8744 (3)0.0355 (8)
H35A0.55880.64010.79590.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Y10.02100 (14)0.01684 (13)0.01973 (13)0.00180 (10)0.00476 (10)0.00791 (10)
Cl10.0363 (5)0.0321 (4)0.0387 (5)0.0042 (4)0.0077 (4)0.0244 (4)
Cl20.0377 (5)0.0236 (4)0.0332 (4)0.0024 (3)0.0066 (4)0.0168 (3)
O10.0216 (12)0.0270 (12)0.0441 (14)0.0039 (10)0.0048 (10)0.0092 (11)
O20.0347 (13)0.0268 (13)0.0268 (12)0.0075 (10)0.0124 (10)0.0068 (10)
O30.0243 (12)0.0325 (13)0.0268 (12)0.0043 (10)0.0019 (9)0.0131 (10)
O40.0300 (12)0.0300 (13)0.0299 (12)0.0062 (10)0.0125 (10)0.0133 (10)
N10.0262 (14)0.0236 (14)0.0257 (14)0.0023 (11)0.0047 (11)0.0059 (12)
B10.0294 (19)0.0165 (16)0.0219 (17)0.0023 (15)0.0024 (15)0.0062 (13)
C10.0224 (16)0.0287 (17)0.0249 (16)0.0055 (13)0.0052 (13)0.0134 (14)
C20.0264 (18)0.042 (2)0.047 (2)0.0009 (16)0.0076 (16)0.0252 (18)
C30.043 (2)0.043 (3)0.084 (3)0.0033 (19)0.019 (2)0.032 (2)
C40.041 (2)0.054 (3)0.054 (3)0.0083 (19)0.0030 (19)0.033 (2)
C50.026 (3)0.036 (3)0.065 (4)0.009 (2)0.009 (3)0.024 (3)
C5B0.023 (6)0.099 (12)0.108 (12)0.001 (7)0.002 (7)0.086 (11)
C60.082 (3)0.029 (2)0.055 (3)0.017 (2)0.028 (2)0.010 (2)
C70.047 (2)0.036 (2)0.044 (2)0.0079 (18)0.0209 (19)0.0007 (18)
C80.058 (3)0.053 (3)0.032 (2)0.008 (2)0.0207 (19)0.0056 (19)
C90.049 (2)0.040 (2)0.043 (2)0.0062 (18)0.0268 (19)0.0123 (18)
C100.0304 (19)0.039 (2)0.043 (2)0.0083 (16)0.0030 (16)0.0193 (17)
C110.0314 (19)0.0271 (18)0.053 (2)0.0030 (16)0.0018 (17)0.0111 (17)
C120.060 (3)0.056 (3)0.036 (2)0.009 (2)0.009 (2)0.018 (2)
C130.048 (2)0.051 (3)0.037 (2)0.0078 (19)0.0073 (18)0.025 (2)
C140.037 (2)0.045 (2)0.061 (3)0.0201 (18)0.0213 (19)0.031 (2)
C150.039 (4)0.055 (5)0.039 (3)0.022 (3)0.013 (3)0.020 (3)
C160.044 (4)0.065 (5)0.040 (4)0.026 (4)0.022 (3)0.026 (4)
C15B0.049 (10)0.082 (14)0.110 (15)0.039 (9)0.059 (11)0.048 (13)
C16B0.056 (9)0.093 (12)0.053 (9)0.027 (9)0.037 (7)0.038 (9)
C170.051 (3)0.076 (3)0.049 (2)0.020 (2)0.029 (2)0.041 (2)
C180.0194 (15)0.0272 (16)0.0249 (15)0.0058 (13)0.0066 (13)0.0121 (13)
C190.0272 (18)0.0378 (19)0.0295 (17)0.0084 (15)0.0098 (14)0.0175 (15)
C200.0279 (19)0.063 (3)0.0351 (18)0.0153 (18)0.0099 (16)0.0333 (19)
C210.031 (2)0.052 (2)0.064 (3)0.0170 (17)0.0179 (18)0.047 (2)
C220.035 (2)0.0295 (19)0.053 (2)0.0081 (15)0.0103 (17)0.0228 (17)
C230.0336 (18)0.0278 (17)0.0301 (17)0.0058 (15)0.0062 (15)0.0143 (14)
C240.0309 (17)0.0204 (16)0.0219 (16)0.0030 (13)0.0045 (13)0.0065 (13)
C250.035 (2)0.034 (2)0.0369 (19)0.0062 (16)0.0082 (16)0.0209 (16)
C260.038 (2)0.046 (2)0.056 (2)0.0147 (18)0.0178 (19)0.0264 (19)
C270.043 (2)0.048 (2)0.046 (2)0.0050 (19)0.0234 (19)0.0219 (19)
C280.050 (2)0.036 (2)0.039 (2)0.0043 (18)0.0143 (18)0.0217 (17)
C290.038 (2)0.0248 (18)0.0322 (18)0.0053 (15)0.0121 (15)0.0123 (15)
C300.0324 (18)0.0124 (15)0.0272 (17)0.0005 (13)0.0014 (14)0.0065 (13)
C310.044 (2)0.0237 (18)0.0276 (18)0.0065 (15)0.0010 (15)0.0077 (15)
C320.057 (3)0.0235 (18)0.0333 (19)0.0053 (17)0.0145 (18)0.0056 (15)
C330.033 (2)0.0239 (19)0.058 (3)0.0026 (15)0.0088 (19)0.0116 (18)
C340.033 (2)0.033 (2)0.058 (3)0.0006 (16)0.0059 (18)0.0201 (19)
C350.0307 (19)0.0341 (19)0.040 (2)0.0002 (15)0.0047 (16)0.0176 (16)
Geometric parameters (Å, º) top
Y1—O12.369 (2)C10—C111.515 (5)
Y1—O22.370 (2)C11—C121.518 (5)
Y1—O42.382 (2)C12—C131.493 (5)
Y1—O32.390 (2)C14—C151.429 (8)
Y1—N12.420 (3)C14—C15B1.583 (16)
Y1—Cl22.5730 (8)C15—C161.503 (11)
Y1—Cl12.5803 (9)C16—C171.578 (8)
O1—C51.408 (6)C15B—C16B1.44 (2)
O1—C21.452 (4)C16B—C171.408 (14)
O1—C5B1.594 (12)C18—C191.396 (4)
O2—C91.451 (4)C18—C231.396 (4)
O2—C61.473 (4)C19—C201.390 (5)
O3—C131.438 (4)C20—C211.376 (5)
O3—C101.463 (4)C21—C221.377 (5)
O4—C141.453 (4)C22—C231.391 (5)
O4—C171.460 (4)C24—C251.392 (5)
N1—C11.144 (4)C24—C291.407 (5)
B1—C241.626 (5)C25—C261.388 (5)
B1—C11.629 (4)C26—C271.384 (5)
B1—C181.630 (5)C27—C281.383 (5)
B1—C301.642 (5)C28—C291.384 (5)
C2—C31.504 (5)C30—C351.388 (5)
C3—C41.505 (6)C30—C311.393 (5)
C4—C5B1.428 (12)C31—C321.404 (5)
C4—C51.552 (7)C32—C331.368 (6)
C6—C71.506 (5)C33—C341.376 (6)
C7—C81.523 (6)C34—C351.387 (5)
C8—C91.492 (5)
O1—Y1—O272.94 (8)C5B—C4—C399.2 (7)
O1—Y1—O4142.45 (8)C3—C4—C5103.6 (4)
O2—Y1—O4143.68 (8)O1—C5—C4105.3 (4)
O1—Y1—O3145.89 (8)C4—C5B—O1102.3 (8)
O2—Y1—O373.07 (8)O2—C6—C7105.5 (3)
O4—Y1—O370.93 (8)C6—C7—C8102.2 (3)
O1—Y1—N173.27 (8)C9—C8—C7102.2 (3)
O2—Y1—N1144.47 (9)O2—C9—C8105.4 (3)
O4—Y1—N171.65 (8)O3—C10—C11103.5 (3)
O3—Y1—N1140.55 (9)C10—C11—C12102.4 (3)
O1—Y1—Cl293.71 (6)C13—C12—C11105.8 (3)
O2—Y1—Cl286.20 (6)O3—C13—C12107.4 (3)
O4—Y1—Cl296.39 (6)C15—C14—O4109.7 (4)
O3—Y1—Cl286.81 (6)O4—C14—C15B98.3 (7)
N1—Y1—Cl285.32 (7)C14—C15—C16102.8 (6)
O1—Y1—Cl188.01 (6)C15—C16—C17105.4 (5)
O2—Y1—Cl189.21 (6)C16B—C15B—C14107.1 (11)
O4—Y1—Cl185.42 (6)C17—C16B—C15B97.5 (11)
O3—Y1—Cl188.77 (6)C16B—C17—O4106.2 (7)
N1—Y1—Cl1100.28 (7)O4—C17—C16103.9 (4)
Cl2—Y1—Cl1174.39 (3)C19—C18—C23116.3 (3)
C5—O1—C2104.8 (3)C19—C18—B1126.0 (3)
C2—O1—C5B105.3 (5)C23—C18—B1117.6 (3)
C5—O1—Y1128.8 (3)C20—C19—C18121.2 (3)
C2—O1—Y1125.9 (2)C21—C20—C19121.0 (3)
C5B—O1—Y1119.6 (4)C20—C21—C22119.3 (3)
C9—O2—C6108.5 (3)C21—C22—C23119.5 (3)
C9—O2—Y1127.3 (2)C22—C23—C18122.6 (3)
C6—O2—Y1124.1 (2)C25—C24—C29115.5 (3)
C13—O3—C10107.0 (2)C25—C24—B1122.6 (3)
C13—O3—Y1128.5 (2)C29—C24—B1121.9 (3)
C10—O3—Y1124.49 (19)C26—C25—C24123.2 (3)
C14—O4—C17107.8 (3)C27—C26—C25119.4 (4)
C14—O4—Y1121.12 (19)C28—C27—C26119.4 (3)
C17—O4—Y1126.3 (2)C27—C28—C29120.2 (3)
C1—N1—Y1164.6 (3)C28—C29—C24122.2 (3)
C24—B1—C1105.7 (3)C35—C30—C31115.7 (3)
C24—B1—C18111.6 (3)C35—C30—B1119.3 (3)
C1—B1—C18107.8 (2)C31—C30—B1125.0 (3)
C24—B1—C30116.6 (3)C30—C31—C32121.4 (4)
C1—B1—C30106.0 (3)C33—C32—C31120.6 (3)
C18—B1—C30108.6 (3)C32—C33—C34119.4 (3)
N1—C1—B1178.4 (3)C33—C34—C35119.4 (4)
O1—C2—C3103.9 (3)C34—C35—C30123.5 (3)
C2—C3—C4105.0 (3)
Tetraethylazanium 2,2,4,6-tetraphenyl-1,3,5,2λ4,4,6-trioxatriborinan-2-ide (2) top
Crystal data top
C8H20N+·C24H20B3O3F(000) = 1112
Mr = 519.08Dx = 1.179 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 9.7245 (7) ÅCell parameters from 9884 reflections
b = 18.3021 (13) Åθ = 2.4–28.3°
c = 16.7716 (12) ŵ = 0.07 mm1
β = 101.5456 (9)°T = 133 K
V = 2924.6 (4) Å3Prism, colorless
Z = 40.37 × 0.33 × 0.23 mm
Data collection top
Bruker SMART APEXII CCD
diffractometer
5030 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.029
φ and ω scansθmax = 26.4°, θmin = 1.7°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1212
Tmin = 0.834, Tmax = 0.862k = 2222
31741 measured reflectionsl = 2020
5959 independent reflections
Refinement top
Refinement on F2Primary atom site location: dual space
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.064Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.179H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0909P)2 + 2.9541P]
where P = (Fo2 + 2Fc2)/3
5959 reflections(Δ/σ)max = 0.001
442 parametersΔρmax = 1.06 e Å3
0 restraintsΔρmin = 0.47 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. A colorless crystal of approximate dimensions 0.228 x 0.331 x 0.367 mm was mounted on a glass fiber and transferred to a Bruker SMART APEX II diffractometer. The APEX2 program package was used to determine the unit-cell parameters and for data collection (20 sec/frame scan time for a sphere of diffraction data). The raw frame data was processed using SAINT and SADABS to yield the reflection data file. Subsequent calculations were carried out using the SHELXTL program. The diffraction symmetry was 2/m and the systematic absences were consistent with the monoclinic space group P21/n that was later determined to be correct.

The structure was solved by dual space methods and refined on F2 by full-matrix least-squares techniques. The analytical scattering factors for neutral atoms were used throughout the analysis. Hydrogen atoms were included using a riding model. The tetraethylammonium ion was fully disordered. The disordered atoms were included using multiple components with partial site-occupancy-factors.

Least-squares analysis yielded wR2 = 0.1785 and Goof = 1.017 for 442 variables refined against 5959 data (0.80 Å), R1 = 0.0639 for those 5030 data with I > 2.0sigma(I).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
B10.4762 (2)0.56789 (11)0.77924 (12)0.0193 (4)
B20.6190 (2)0.62127 (11)0.68613 (12)0.0177 (4)
B30.6440 (2)0.66930 (11)0.82091 (13)0.0190 (4)
O10.52579 (14)0.57190 (7)0.69997 (7)0.0215 (3)
O20.67303 (14)0.67482 (7)0.74274 (8)0.0226 (3)
O30.56271 (14)0.61696 (7)0.84114 (7)0.0212 (3)
C10.3139 (2)0.59569 (10)0.76601 (11)0.0208 (4)
C20.2638 (2)0.63277 (11)0.82703 (12)0.0257 (4)
H2A0.32570.64100.87770.031*
C30.1269 (2)0.65811 (11)0.81642 (13)0.0295 (5)
H3A0.09680.68320.85950.035*
C40.0340 (2)0.64703 (12)0.74362 (14)0.0310 (5)
H4A0.05980.66440.73610.037*
C50.0796 (2)0.61020 (14)0.68181 (14)0.0384 (5)
H5A0.01700.60210.63140.046*
C60.2174 (2)0.58499 (13)0.69332 (13)0.0318 (5)
H6A0.24670.55960.65020.038*
C70.49230 (18)0.48395 (10)0.81153 (11)0.0191 (4)
C80.5228 (2)0.46709 (11)0.89406 (12)0.0291 (5)
H8A0.53860.50580.93260.035*
C90.5309 (3)0.39533 (13)0.92183 (14)0.0368 (5)
H9A0.55280.38560.97860.044*
C100.5071 (2)0.33809 (11)0.86710 (14)0.0325 (5)
H10A0.51010.28910.88590.039*
C110.4790 (2)0.35292 (11)0.78472 (14)0.0295 (5)
H11A0.46450.31390.74660.035*
C120.4719 (2)0.42482 (11)0.75758 (12)0.0245 (4)
H12A0.45250.43410.70070.029*
C130.67346 (18)0.62034 (10)0.60354 (11)0.0189 (4)
C140.6536 (2)0.55854 (11)0.55359 (12)0.0253 (4)
H14A0.60690.51720.56980.030*
C150.7006 (3)0.55642 (13)0.48118 (13)0.0368 (5)
H15A0.68730.51360.44850.044*
C160.7671 (3)0.61664 (15)0.45617 (14)0.0402 (6)
H16A0.79920.61520.40630.048*
C170.7867 (2)0.67887 (14)0.50387 (13)0.0368 (5)
H17A0.83120.72050.48650.044*
C180.7410 (2)0.68035 (12)0.57715 (12)0.0265 (4)
H18A0.75600.72300.61000.032*
C190.71090 (19)0.72806 (10)0.88572 (11)0.0215 (4)
C200.8255 (2)0.77103 (11)0.87687 (13)0.0275 (4)
H20A0.86460.76540.82970.033*
C210.8835 (2)0.82185 (12)0.93569 (15)0.0358 (5)
H21A0.96330.84950.92930.043*
C220.8252 (2)0.83221 (12)1.00344 (14)0.0336 (5)
H22A0.86390.86741.04330.040*
C230.7105 (2)0.79122 (12)1.01311 (13)0.0335 (5)
H23A0.66950.79851.05940.040*
C240.6552 (2)0.73938 (12)0.95518 (12)0.0289 (4)
H24A0.57730.71090.96300.035*
N40.4859 (11)0.8966 (7)0.6646 (6)0.0247 (17)0.567 (3)
C250.4659 (5)0.9730 (2)0.6325 (4)0.0550 (15)0.567 (3)
H25A0.54930.98790.61110.066*0.567 (3)
H25B0.45691.00650.67750.066*0.567 (3)
C260.3277 (5)0.9795 (3)0.5612 (3)0.0479 (12)0.567 (3)
H26A0.32131.02910.53870.072*0.567 (3)
H26B0.24410.96910.58350.072*0.567 (3)
H26C0.33390.94430.51800.072*0.567 (3)
C270.4859 (6)0.8388 (3)0.5960 (3)0.0553 (13)0.567 (3)
H27A0.52120.79230.62250.066*0.567 (3)
H27D0.38710.83060.56860.066*0.567 (3)
C280.5623 (8)0.8535 (3)0.5362 (3)0.0687 (18)0.567 (3)
H28A0.56100.81060.50110.103*0.567 (3)
H28B0.65950.86510.56180.103*0.567 (3)
H28C0.52040.89520.50340.103*0.567 (3)
C290.6298 (5)0.8933 (3)0.7230 (5)0.082 (3)0.567 (3)
H29A0.64580.84250.74310.098*0.567 (3)
H29D0.70330.90470.69170.098*0.567 (3)
C300.6475 (10)0.9406 (5)0.7909 (5)0.114 (4)0.567 (3)
H30A0.74430.93740.82140.170*0.567 (3)
H30B0.58290.92630.82620.170*0.567 (3)
H30C0.62730.99090.77220.170*0.567 (3)
C310.3724 (4)0.8759 (3)0.7034 (3)0.0452 (12)0.567 (3)
H31A0.28150.89060.66920.054*0.567 (3)
H31B0.38250.90070.75680.054*0.567 (3)
C320.3769 (6)0.7839 (3)0.7165 (4)0.0343 (11)0.567 (3)
H32A0.28090.76490.70760.051*0.567 (3)
H32B0.42570.77230.77200.051*0.567 (3)
H32C0.42680.76150.67740.051*0.567 (3)
N4B0.4989 (18)0.9025 (10)0.6867 (8)0.030 (3)0.433 (3)
C25B0.6237 (6)0.9310 (3)0.6647 (4)0.0357 (12)0.433 (3)
H25C0.63150.91000.61140.043*0.433 (3)
H25D0.70570.91360.70520.043*0.433 (3)
C26B0.6326 (4)1.0148 (2)0.6590 (3)0.0206 (9)0.433 (3)
H26D0.71471.02820.63650.031*0.433 (3)
H26E0.64151.03610.71340.031*0.433 (3)
H26F0.54741.03340.62350.031*0.433 (3)
C27B0.3630 (5)0.9241 (3)0.6138 (3)0.0358 (12)0.433 (3)
H27B0.27760.90140.62650.043*0.433 (3)
H27C0.34990.97780.61390.043*0.433 (3)
C28B0.3771 (8)0.9007 (4)0.5299 (4)0.0544 (17)0.433 (3)
H28D0.29000.91170.49110.082*0.433 (3)
H28E0.39540.84810.52970.082*0.433 (3)
H28F0.45520.92710.51410.082*0.433 (3)
C29B0.4530 (6)0.9384 (3)0.7578 (3)0.0360 (12)0.433 (3)
H29B0.36180.91780.76440.043*0.433 (3)
H29C0.44030.99150.74740.043*0.433 (3)
C30B0.5623 (6)0.9263 (3)0.8356 (3)0.0295 (11)0.433 (3)
H30D0.53330.95180.88090.044*0.433 (3)
H30E0.65320.94530.82840.044*0.433 (3)
H30F0.57070.87380.84760.044*0.433 (3)
C31B0.4989 (5)0.8204 (3)0.6900 (3)0.0312 (11)0.433 (3)
H31C0.59340.80070.71270.037*0.433 (3)
H31D0.46330.79860.63580.037*0.433 (3)
C32B0.3869 (8)0.8069 (5)0.7537 (5)0.050 (2)0.433 (3)
H32D0.34220.75900.74300.075*0.433 (3)
H32E0.31480.84510.74480.075*0.433 (3)
H32F0.43870.80890.81010.075*0.433 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
B10.0231 (10)0.0195 (10)0.0164 (9)0.0042 (8)0.0062 (8)0.0017 (7)
B20.0160 (9)0.0192 (10)0.0177 (9)0.0028 (7)0.0030 (7)0.0022 (7)
B30.0163 (9)0.0193 (10)0.0209 (10)0.0016 (7)0.0023 (8)0.0002 (8)
O10.0255 (7)0.0231 (7)0.0169 (6)0.0053 (5)0.0065 (5)0.0020 (5)
O20.0242 (7)0.0237 (7)0.0217 (7)0.0065 (5)0.0089 (5)0.0046 (5)
O30.0249 (7)0.0210 (7)0.0177 (6)0.0045 (5)0.0047 (5)0.0023 (5)
C10.0258 (9)0.0151 (8)0.0224 (9)0.0025 (7)0.0069 (7)0.0022 (7)
C20.0303 (10)0.0269 (10)0.0198 (9)0.0009 (8)0.0049 (8)0.0004 (7)
C30.0332 (11)0.0280 (10)0.0301 (11)0.0064 (8)0.0132 (9)0.0000 (8)
C40.0254 (10)0.0293 (11)0.0389 (12)0.0042 (8)0.0080 (9)0.0007 (9)
C50.0301 (11)0.0470 (14)0.0342 (12)0.0054 (10)0.0028 (9)0.0108 (10)
C60.0288 (11)0.0397 (12)0.0263 (10)0.0044 (9)0.0037 (8)0.0099 (9)
C70.0152 (8)0.0220 (9)0.0205 (9)0.0023 (7)0.0047 (7)0.0009 (7)
C80.0378 (11)0.0272 (10)0.0217 (10)0.0039 (9)0.0041 (8)0.0009 (8)
C90.0447 (13)0.0349 (12)0.0286 (11)0.0009 (10)0.0022 (10)0.0118 (9)
C100.0288 (11)0.0208 (10)0.0489 (13)0.0039 (8)0.0101 (10)0.0108 (9)
C110.0286 (10)0.0204 (10)0.0429 (12)0.0007 (8)0.0151 (9)0.0064 (8)
C120.0276 (10)0.0233 (9)0.0238 (9)0.0027 (8)0.0080 (8)0.0019 (7)
C130.0143 (8)0.0241 (9)0.0179 (8)0.0021 (7)0.0022 (7)0.0015 (7)
C140.0288 (10)0.0248 (10)0.0229 (9)0.0035 (8)0.0062 (8)0.0000 (7)
C150.0431 (13)0.0420 (13)0.0273 (11)0.0055 (10)0.0118 (10)0.0083 (9)
C160.0364 (12)0.0659 (17)0.0220 (10)0.0008 (11)0.0149 (9)0.0032 (10)
C170.0315 (11)0.0531 (14)0.0275 (11)0.0125 (10)0.0097 (9)0.0066 (10)
C180.0252 (10)0.0309 (10)0.0233 (10)0.0055 (8)0.0046 (8)0.0008 (8)
C190.0201 (9)0.0212 (9)0.0224 (9)0.0005 (7)0.0021 (7)0.0009 (7)
C200.0226 (10)0.0277 (10)0.0332 (11)0.0030 (8)0.0082 (8)0.0070 (8)
C210.0248 (10)0.0324 (12)0.0499 (14)0.0088 (9)0.0071 (10)0.0133 (10)
C220.0323 (11)0.0293 (11)0.0355 (12)0.0028 (9)0.0020 (9)0.0144 (9)
C230.0409 (12)0.0339 (12)0.0257 (10)0.0037 (9)0.0071 (9)0.0090 (9)
C240.0317 (11)0.0297 (11)0.0259 (10)0.0084 (8)0.0071 (8)0.0052 (8)
N40.016 (2)0.026 (3)0.030 (5)0.0004 (19)0.001 (3)0.001 (3)
C250.044 (3)0.020 (2)0.115 (4)0.0086 (17)0.048 (3)0.020 (2)
C260.048 (3)0.048 (3)0.049 (3)0.011 (2)0.013 (2)0.007 (2)
C270.066 (3)0.042 (3)0.057 (3)0.011 (2)0.009 (3)0.010 (2)
C280.115 (5)0.052 (3)0.038 (3)0.022 (3)0.014 (3)0.004 (2)
C290.031 (3)0.030 (3)0.162 (7)0.010 (2)0.032 (3)0.018 (3)
C300.108 (7)0.106 (6)0.093 (6)0.054 (5)0.060 (5)0.043 (5)
C310.0221 (19)0.057 (3)0.058 (3)0.0066 (18)0.0125 (18)0.037 (2)
C320.031 (2)0.026 (2)0.048 (3)0.0033 (18)0.013 (2)0.006 (2)
N4B0.044 (5)0.018 (3)0.027 (6)0.007 (3)0.005 (4)0.002 (4)
C25B0.028 (3)0.026 (3)0.054 (3)0.004 (2)0.011 (2)0.007 (2)
C26B0.0155 (19)0.015 (2)0.033 (2)0.0087 (15)0.0080 (17)0.0005 (16)
C27B0.025 (2)0.036 (3)0.042 (3)0.001 (2)0.001 (2)0.011 (2)
C28B0.061 (4)0.057 (4)0.039 (3)0.017 (3)0.004 (3)0.002 (3)
C29B0.036 (3)0.027 (3)0.045 (3)0.001 (2)0.010 (2)0.006 (2)
C30B0.036 (3)0.029 (2)0.022 (2)0.004 (2)0.002 (2)0.0007 (19)
C31B0.027 (2)0.021 (2)0.045 (3)0.0010 (18)0.005 (2)0.001 (2)
C32B0.043 (4)0.048 (5)0.066 (5)0.021 (4)0.028 (4)0.036 (4)
Geometric parameters (Å, º) top
B1—O31.497 (2)C15—C161.385 (4)
B1—O11.504 (2)C16—C171.383 (4)
B1—C71.626 (3)C17—C181.388 (3)
B1—C11.631 (3)C19—C241.395 (3)
B2—O11.333 (2)C19—C201.396 (3)
B2—O21.392 (2)C20—C211.391 (3)
B2—C131.579 (3)C21—C221.380 (3)
B3—O31.329 (2)C22—C231.380 (3)
B3—O21.399 (2)C23—C241.387 (3)
B3—C191.574 (3)N4—C311.441 (13)
C1—C21.394 (3)N4—C251.497 (14)
C1—C61.395 (3)N4—C291.541 (11)
C2—C31.388 (3)N4—C271.561 (11)
C3—C41.381 (3)C25—C261.615 (8)
C4—C51.382 (3)C27—C281.390 (8)
C5—C61.394 (3)C29—C301.414 (9)
C7—C81.391 (3)C31—C321.697 (7)
C7—C121.399 (3)N4B—C25B1.435 (19)
C8—C91.391 (3)N4B—C31B1.504 (18)
C9—C101.381 (3)N4B—C29B1.506 (15)
C10—C111.381 (3)N4B—C27B1.659 (16)
C11—C121.390 (3)C25B—C26B1.541 (6)
C13—C181.396 (3)C27B—C28B1.504 (9)
C13—C141.398 (3)C29B—C30B1.525 (8)
C14—C151.381 (3)C31B—C32B1.688 (9)
O3—B1—O1110.41 (14)C15—C14—C13121.3 (2)
O3—B1—C7109.43 (15)C14—C15—C16120.0 (2)
O1—B1—C7108.31 (15)C17—C16—C15119.9 (2)
O3—B1—C1107.53 (15)C16—C17—C18119.8 (2)
O1—B1—C1109.70 (15)C17—C18—C13121.3 (2)
C7—B1—C1111.47 (15)C24—C19—C20117.19 (18)
O1—B2—O2122.37 (16)C24—C19—B3120.14 (17)
O1—B2—C13120.31 (17)C20—C19—B3122.67 (17)
O2—B2—C13117.32 (16)C21—C20—C19121.36 (19)
O3—B3—O2122.23 (17)C22—C21—C20120.1 (2)
O3—B3—C19120.06 (17)C23—C22—C21119.76 (19)
O2—B3—C19117.70 (16)C22—C23—C24119.9 (2)
B2—O1—B1122.45 (15)C23—C24—C19121.68 (19)
B2—O2—B3117.97 (15)C31—N4—C25110.6 (8)
B3—O3—B1122.39 (15)C31—N4—C29112.5 (8)
C2—C1—C6115.91 (18)C25—N4—C29107.5 (8)
C2—C1—B1121.51 (17)C31—N4—C27105.6 (8)
C6—C1—B1122.57 (17)C25—N4—C27112.8 (7)
C3—C2—C1122.39 (19)C29—N4—C27107.9 (8)
C4—C3—C2120.37 (19)N4—C25—C26111.4 (5)
C3—C4—C5118.9 (2)C28—C27—N4118.7 (7)
C4—C5—C6120.1 (2)C30—C29—N4115.9 (6)
C5—C6—C1122.3 (2)N4—C31—C32108.4 (6)
C8—C7—C12116.51 (18)C25B—N4B—C31B112.3 (12)
C8—C7—B1121.88 (17)C25B—N4B—C29B116.4 (10)
C12—C7—B1121.58 (16)C31B—N4B—C29B113.9 (11)
C9—C8—C7122.0 (2)C25B—N4B—C27B108.2 (10)
C10—C9—C8120.2 (2)C31B—N4B—C27B105.1 (9)
C11—C10—C9119.29 (19)C29B—N4B—C27B99.2 (11)
C10—C11—C12120.06 (19)N4B—C25B—C26B116.0 (8)
C11—C12—C7121.96 (19)C28B—C27B—N4B114.4 (7)
C18—C13—C14117.63 (17)N4B—C29B—C30B110.3 (7)
C18—C13—B2122.09 (17)N4B—C31B—C32B100.0 (8)
C14—C13—B2120.28 (17)
Tetraethylazanium cyanodiphenyl-λ4-boranyl diphenylborinate (3) top
Crystal data top
C8H20N+·C25H20B2NOF(000) = 1080
Mr = 502.29Dx = 1.172 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 11.0269 (8) ÅCell parameters from 9716 reflections
b = 13.9387 (11) Åθ = 2.2–29.1°
c = 18.8488 (14) ŵ = 0.07 mm1
β = 100.6357 (10)°T = 88 K
V = 2847.3 (4) Å3Irregular, colorless
Z = 40.28 × 0.27 × 0.22 mm
Data collection top
Bruker SMART APEXII CCD
diffractometer
5500 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.042
φ and ω scansθmax = 29.1°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1414
Tmin = 0.715, Tmax = 0.746k = 1818
34768 measured reflectionsl = 2525
7242 independent reflections
Refinement top
Refinement on F2Primary atom site location: dual space
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.048Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.119H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0477P)2 + 1.1994P]
where P = (Fo2 + 2Fc2)/3
7242 reflections(Δ/σ)max < 0.001
347 parametersΔρmax = 0.41 e Å3
0 restraintsΔρmin = 0.24 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. A colorless crystal of approximate dimensions 0.216 x 0.265 x 0.280 mm was mounted in a cryoloop and transferred to a Bruker SMART APEX II diffractometer. The APEX2 program package was used to determine the unit-cell parameters and for data collection (30 sec/frame scan time for a sphere of diffraction data). The raw frame data was processed using SAINT and SADABS to yield the reflection data file. Subsequent calculations were carried out using the SHELXTL program. The diffraction symmetry was 2/m and the systematic absences were consistent with the monoclinic space group P21/n that was later determined to be correct.

The structure was solved by dual space methods and refined on F2 by full-matrix least-squares techniques. The analytical scattering factors for neutral atoms were used throughout the analysis. Hydrogen atoms were included using a riding model.

Least-squares analysis yielded wR2 = 0.1188 and Goof = 1.038 for 347 variables refined against 7242 data (0.73 Å), R1 = 0.0476 for those 5500 data with I > 2.0sigma(I).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.54584 (8)0.23892 (7)0.71613 (5)0.0169 (2)
N10.65451 (11)0.48002 (9)0.69950 (7)0.0223 (3)
B10.57013 (13)0.29746 (11)0.65455 (8)0.0150 (3)
B20.48921 (13)0.24852 (11)0.77251 (8)0.0164 (3)
C10.61696 (12)0.40504 (10)0.68153 (7)0.0164 (3)
C20.68248 (12)0.24787 (9)0.62196 (7)0.0155 (3)
C30.74007 (12)0.29439 (10)0.57114 (7)0.0167 (3)
H30.71320.35690.55550.020*
C40.83524 (13)0.25223 (10)0.54282 (7)0.0193 (3)
H40.87160.28560.50810.023*
C50.87694 (13)0.16128 (10)0.56543 (8)0.0229 (3)
H50.94190.13210.54630.028*
C60.82301 (14)0.11343 (11)0.61610 (9)0.0271 (3)
H60.85160.05150.63220.033*
C70.72688 (13)0.15612 (10)0.64344 (8)0.0229 (3)
H70.69030.12190.67770.028*
C80.44546 (12)0.30775 (9)0.59338 (7)0.0155 (3)
C90.42486 (12)0.38370 (10)0.54401 (7)0.0178 (3)
H90.48820.42990.54400.021*
C100.31446 (13)0.39366 (10)0.49485 (7)0.0210 (3)
H100.30360.44610.46210.025*
C110.22064 (13)0.32728 (11)0.49356 (7)0.0243 (3)
H110.14450.33470.46100.029*
C120.23942 (14)0.24983 (12)0.54039 (8)0.0279 (3)
H120.17650.20300.53920.033*
C130.35024 (13)0.24034 (11)0.58922 (8)0.0234 (3)
H130.36150.18650.62060.028*
C140.42967 (12)0.34557 (10)0.79522 (7)0.0179 (3)
C150.35810 (12)0.40696 (10)0.74516 (7)0.0205 (3)
H150.34430.39090.69530.025*
C160.30703 (13)0.49057 (10)0.76672 (8)0.0234 (3)
H160.25710.52990.73180.028*
C170.32839 (13)0.51700 (10)0.83869 (8)0.0240 (3)
H170.29510.57520.85310.029*
C180.39858 (13)0.45811 (10)0.88957 (8)0.0228 (3)
H180.41350.47570.93910.027*
C190.44713 (13)0.37332 (10)0.86811 (7)0.0195 (3)
H190.49350.33290.90370.023*
C200.48423 (12)0.15502 (9)0.82032 (7)0.0160 (3)
C210.39985 (12)0.14284 (10)0.86704 (7)0.0171 (3)
H210.34520.19390.87250.021*
C220.39383 (13)0.05835 (10)0.90564 (7)0.0199 (3)
H220.33450.05150.93600.024*
C230.47508 (13)0.01578 (10)0.89946 (7)0.0204 (3)
H230.47190.07350.92590.024*
C240.56085 (13)0.00558 (10)0.85476 (7)0.0210 (3)
H240.61710.05610.85100.025*
C250.56500 (13)0.07811 (10)0.81549 (7)0.0187 (3)
H250.62370.08370.78460.022*
N20.51337 (10)0.80126 (8)0.65697 (6)0.0166 (2)
C260.53989 (13)0.69500 (10)0.65074 (8)0.0228 (3)
H26A0.59950.68690.61780.027*
H26B0.57970.67090.69880.027*
C270.42736 (13)0.63381 (11)0.62331 (8)0.0253 (3)
H27A0.39100.65330.57400.038*
H27B0.36660.64240.65470.038*
H27C0.45170.56620.62350.038*
C280.42039 (13)0.81887 (10)0.70616 (7)0.0206 (3)
H28A0.41780.88860.71590.025*
H28B0.33760.79980.68010.025*
C290.44632 (14)0.76619 (11)0.77769 (8)0.0252 (3)
H29A0.43970.69690.76900.038*
H29B0.38620.78590.80720.038*
H29C0.52980.78170.80310.038*
C300.63326 (12)0.85169 (10)0.68896 (7)0.0200 (3)
H30A0.61450.91940.69860.024*
H30B0.66760.82140.73590.024*
C310.73123 (13)0.84982 (12)0.64196 (8)0.0256 (3)
H31A0.69860.87980.59530.038*
H31B0.75410.78320.63430.038*
H31C0.80410.88520.66600.038*
C320.46006 (14)0.84029 (11)0.58214 (8)0.0258 (3)
H32A0.51540.82170.54870.031*
H32B0.37920.80930.56490.031*
C330.44268 (16)0.94792 (13)0.57844 (9)0.0359 (4)
H33A0.40170.96620.52970.054*
H33B0.52330.97950.58990.054*
H33C0.39180.96780.61330.054*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0185 (5)0.0189 (5)0.0140 (4)0.0017 (4)0.0045 (4)0.0036 (4)
N10.0202 (6)0.0224 (6)0.0246 (6)0.0005 (5)0.0043 (5)0.0017 (5)
B10.0171 (7)0.0156 (7)0.0127 (6)0.0001 (5)0.0034 (5)0.0017 (5)
B20.0143 (7)0.0180 (7)0.0163 (7)0.0005 (5)0.0008 (5)0.0015 (6)
C10.0137 (6)0.0214 (7)0.0141 (6)0.0027 (5)0.0028 (5)0.0022 (5)
C20.0160 (6)0.0164 (6)0.0137 (6)0.0023 (5)0.0018 (5)0.0023 (5)
C30.0200 (6)0.0169 (6)0.0129 (6)0.0007 (5)0.0019 (5)0.0006 (5)
C40.0211 (7)0.0241 (7)0.0136 (6)0.0030 (5)0.0055 (5)0.0008 (5)
C50.0235 (7)0.0225 (7)0.0249 (7)0.0005 (6)0.0100 (6)0.0067 (6)
C60.0317 (8)0.0158 (7)0.0369 (9)0.0025 (6)0.0147 (7)0.0002 (6)
C70.0264 (7)0.0179 (7)0.0275 (7)0.0012 (6)0.0127 (6)0.0033 (6)
C80.0168 (6)0.0175 (6)0.0131 (6)0.0010 (5)0.0051 (5)0.0010 (5)
C90.0193 (6)0.0178 (6)0.0166 (6)0.0001 (5)0.0043 (5)0.0008 (5)
C100.0251 (7)0.0209 (7)0.0166 (6)0.0060 (6)0.0028 (5)0.0007 (5)
C110.0184 (7)0.0359 (8)0.0174 (7)0.0031 (6)0.0001 (5)0.0033 (6)
C120.0222 (7)0.0361 (9)0.0241 (7)0.0107 (6)0.0011 (6)0.0019 (6)
C130.0248 (7)0.0258 (8)0.0188 (7)0.0057 (6)0.0015 (6)0.0054 (6)
C140.0168 (6)0.0178 (6)0.0199 (7)0.0023 (5)0.0057 (5)0.0027 (5)
C150.0199 (7)0.0241 (7)0.0187 (7)0.0003 (5)0.0070 (5)0.0022 (6)
C160.0223 (7)0.0220 (7)0.0268 (7)0.0031 (6)0.0068 (6)0.0099 (6)
C170.0253 (7)0.0163 (7)0.0336 (8)0.0010 (6)0.0135 (6)0.0009 (6)
C180.0263 (7)0.0227 (7)0.0199 (7)0.0033 (6)0.0058 (6)0.0024 (6)
C190.0213 (7)0.0183 (7)0.0190 (7)0.0014 (5)0.0038 (5)0.0011 (5)
C200.0173 (6)0.0165 (6)0.0134 (6)0.0008 (5)0.0007 (5)0.0013 (5)
C210.0162 (6)0.0171 (6)0.0171 (6)0.0019 (5)0.0004 (5)0.0009 (5)
C220.0204 (7)0.0241 (7)0.0156 (6)0.0021 (5)0.0041 (5)0.0007 (5)
C230.0274 (7)0.0159 (7)0.0171 (6)0.0011 (5)0.0018 (5)0.0023 (5)
C240.0269 (7)0.0167 (7)0.0191 (7)0.0041 (5)0.0035 (6)0.0008 (5)
C250.0221 (7)0.0205 (7)0.0139 (6)0.0025 (5)0.0046 (5)0.0000 (5)
N20.0149 (5)0.0198 (6)0.0150 (5)0.0009 (4)0.0027 (4)0.0014 (4)
C260.0193 (7)0.0205 (7)0.0289 (8)0.0013 (5)0.0050 (6)0.0069 (6)
C270.0234 (7)0.0226 (7)0.0292 (8)0.0040 (6)0.0031 (6)0.0065 (6)
C280.0192 (7)0.0221 (7)0.0220 (7)0.0015 (5)0.0081 (5)0.0015 (6)
C290.0309 (8)0.0265 (8)0.0197 (7)0.0026 (6)0.0089 (6)0.0002 (6)
C300.0180 (6)0.0224 (7)0.0189 (7)0.0031 (5)0.0020 (5)0.0033 (5)
C310.0185 (7)0.0330 (8)0.0259 (7)0.0043 (6)0.0056 (6)0.0045 (6)
C320.0216 (7)0.0379 (9)0.0171 (7)0.0031 (6)0.0014 (5)0.0040 (6)
C330.0328 (9)0.0409 (10)0.0355 (9)0.0058 (7)0.0102 (7)0.0193 (8)
Geometric parameters (Å, º) top
O1—B21.3350 (17)C14—C151.4036 (19)
O1—B11.4831 (16)C14—C191.4059 (19)
N1—C11.1518 (18)C15—C161.387 (2)
B1—C81.6293 (19)C16—C171.383 (2)
B1—C21.6343 (19)C17—C181.385 (2)
B1—C11.636 (2)C18—C191.388 (2)
B2—C201.591 (2)C20—C211.4045 (18)
B2—C141.596 (2)C20—C251.4074 (18)
C2—C31.4019 (18)C21—C221.3923 (19)
C2—C71.4021 (19)C22—C231.386 (2)
C3—C41.3923 (19)C23—C241.385 (2)
C4—C51.389 (2)C24—C251.3869 (19)
C5—C61.386 (2)N2—C261.5184 (18)
C6—C71.395 (2)N2—C301.5202 (17)
C8—C131.4004 (19)N2—C281.5239 (17)
C8—C91.4001 (18)N2—C321.5249 (18)
C9—C101.3940 (19)C26—C271.5158 (19)
C10—C111.385 (2)C28—C291.515 (2)
C11—C121.386 (2)C30—C311.5185 (19)
C12—C131.394 (2)C32—C331.512 (2)
B2—O1—B1138.29 (11)C15—C14—C19116.60 (13)
O1—B1—C8110.58 (11)C15—C14—B2122.99 (12)
O1—B1—C2108.69 (10)C19—C14—B2120.41 (12)
C8—B1—C2111.74 (10)C16—C15—C14121.56 (13)
O1—B1—C1110.69 (10)C17—C16—C15120.41 (13)
C8—B1—C1108.42 (10)C16—C17—C18119.56 (13)
C2—B1—C1106.67 (10)C17—C18—C19119.93 (13)
O1—B2—C20116.03 (12)C18—C19—C14121.90 (13)
O1—B2—C14125.05 (12)C21—C20—C25116.67 (12)
C20—B2—C14118.91 (11)C21—C20—B2123.39 (12)
C3—C2—C7116.17 (12)C25—C20—B2119.92 (12)
C3—C2—B1122.11 (11)C22—C21—C20122.06 (12)
C7—C2—B1121.72 (12)C23—C22—C21119.52 (13)
C4—C3—C2122.36 (12)C24—C23—C22119.93 (13)
C5—C4—C3119.86 (13)C23—C24—C25120.30 (13)
C6—C5—C4119.42 (13)C24—C25—C20121.50 (13)
C5—C6—C7120.09 (14)C26—N2—C30108.41 (10)
N1—C1—B1177.10 (13)C26—N2—C28111.41 (10)
C6—C7—C2122.08 (13)C30—N2—C28108.52 (10)
C13—C8—C9116.23 (12)C26—N2—C32108.87 (11)
C13—C8—B1120.44 (12)C30—N2—C32111.12 (10)
C9—C8—B1123.31 (12)C28—N2—C32108.52 (10)
C10—C9—C8122.12 (13)C27—C26—N2114.71 (11)
C11—C10—C9120.21 (13)C29—C28—N2115.19 (11)
C10—C11—C12119.08 (13)C31—C30—N2114.89 (11)
C11—C12—C13120.29 (14)C33—C32—N2114.87 (13)
C12—C13—C8122.02 (13)
Bis[(2.2.2-cryptand)potassium] 2,2,4,6-tetraphenyl-1,3,5,2λ4,4,6-trioxatriborinan-2-ide cyanomethyldiphenylborate tetrahydrofuran disolvate (4) top
Crystal data top
2C18H36KN2O6+·C24H20B3O3·C14H13BN·2C4H8ODx = 1.242 Mg m3
Mr = 1570.27Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pca21Cell parameters from 9334 reflections
a = 27.193 (2) Åθ = 2.3–25.3°
b = 14.5520 (11) ŵ = 0.18 mm1
c = 21.2218 (16) ÅT = 88 K
V = 8397.7 (11) Å3Irregular, colorless
Z = 40.45 × 0.33 × 0.28 mm
F(000) = 3368
Data collection top
Bruker SMART APEXII CCD
diffractometer
14236 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.038
φ and ω scansθmax = 25.7°, θmin = 1.6°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 3333
Tmin = 0.825, Tmax = 0.862k = 1717
85621 measured reflectionsl = 2525
15958 independent reflections
Refinement top
Refinement on F2Primary atom site location: dual space
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.074Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.209H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.1366P)2 + 5.6525P]
where P = (Fo2 + 2Fc2)/3
15958 reflections(Δ/σ)max = 0.001
988 parametersΔρmax = 0.78 e Å3
1 restraintΔρmin = 0.34 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Refinement. A colorless crystal of approximate dimensions 0.280 x 0.325 x 0.454 mm was mounted in a cryoloop and transferred to a Bruker SMART APEX II diffractometer. The APEX2 program package was used to determine the unit-cell parameters and for data collection (60 sec/frame scan time for a sphere of diffraction data). The raw frame data was processed using SAINT and SADABS to yield the reflection data file. Subsequent calculations were carried out using the SHELXTL program. The diffraction symmetry was mmm and the systematic absences were consistent with the orthorhombic space groups Pbcm and Pca21. It was later determined that space group Pca21 was correct.

The structure was solved by dual space methods and refined on F2 by full-matrix least-squares techniques. The analytical scattering factors for neutral atoms were used throughout the analysis. Hydrogen atoms were included using a riding model. There were two molecules of tetrahydrofuran solvent present. One solvent molecule was disordered and included using multiple components with partial site-occupancy-factors.

Least-squares analysis yielded wR2 = 0.2089 and Goof = 1.064 for 988 variables refined against 15958 data (0.82 Å), R1 = 0.0742 for those 14236 data with I > 2.0sigma(I). The structure was refined as a two component inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
B10.8783 (3)0.5804 (5)0.3189 (4)0.0416 (15)
B20.7983 (2)0.5517 (5)0.3727 (3)0.0363 (14)
B30.8194 (2)0.7051 (5)0.3472 (3)0.0357 (14)
O10.84187 (16)0.5214 (3)0.3531 (2)0.0438 (10)
O20.78518 (15)0.6428 (3)0.3691 (2)0.0409 (10)
O30.86284 (16)0.6798 (3)0.3227 (2)0.0439 (10)
C10.9323 (2)0.5724 (4)0.3521 (3)0.0373 (13)
C20.9683 (2)0.6407 (4)0.3493 (3)0.0358 (13)
H2A0.96170.69440.32540.043*
C31.0129 (2)0.6337 (4)0.3795 (3)0.0371 (13)
H3A1.03630.68190.37650.044*
C41.0229 (3)0.5565 (6)0.4139 (4)0.059 (2)
H4A1.05360.55030.43480.071*
C50.9875 (3)0.4864 (6)0.4181 (4)0.069 (2)
H5A0.99380.43310.44270.083*
C60.9438 (3)0.4954 (5)0.3866 (4)0.0526 (17)
H6A0.92050.44670.38870.063*
C70.8806 (2)0.5476 (4)0.2443 (3)0.0407 (14)
C80.8981 (2)0.6029 (6)0.1968 (4)0.0556 (19)
H8A0.91010.66250.20670.067*
C90.8986 (3)0.5735 (7)0.1358 (4)0.071 (2)
H9A0.91060.61340.10390.085*
C100.8822 (3)0.4880 (7)0.1195 (3)0.067 (2)
H10A0.88330.46850.07680.081*
C110.8641 (3)0.4304 (6)0.1651 (4)0.060 (2)
H11A0.85210.37120.15410.072*
C120.8633 (2)0.4599 (5)0.2283 (4)0.0454 (16)
H12A0.85110.42020.26010.054*
C130.7585 (2)0.4816 (5)0.3991 (3)0.0424 (14)
C140.7634 (3)0.3885 (5)0.3920 (3)0.0503 (16)
H14A0.79180.36400.37200.060*
C150.7271 (3)0.3302 (5)0.4140 (4)0.0558 (19)
H15A0.73210.26580.41040.067*
C160.6842 (3)0.3609 (7)0.4406 (4)0.068 (2)
H16A0.65940.31870.45330.082*
C170.6773 (3)0.4565 (5)0.4489 (4)0.0547 (18)
H17A0.64820.48090.46710.066*
C180.7150 (2)0.5120 (5)0.4290 (3)0.0455 (15)
H18A0.71170.57620.43590.055*
C190.8057 (2)0.8116 (5)0.3545 (3)0.0435 (14)
C200.7603 (3)0.8361 (4)0.3792 (3)0.0457 (15)
H20A0.73840.78920.39280.055*
C210.7462 (3)0.9267 (5)0.3846 (4)0.0552 (17)
H21A0.71460.94160.40080.066*
C220.7791 (2)0.9987 (5)0.3657 (3)0.0451 (15)
H22A0.77071.06170.37020.054*
C230.8234 (3)0.9716 (4)0.3409 (3)0.0442 (15)
H23A0.84551.01740.32640.053*
C240.8372 (2)0.8797 (4)0.3362 (3)0.0411 (14)
H24A0.86880.86420.32010.049*
B40.6001 (3)0.1179 (6)0.5064 (5)0.054 (2)
N10.6889 (3)0.1126 (5)0.4428 (3)0.0676 (19)
C250.6501 (2)0.1121 (5)0.4657 (4)0.0526 (19)
C260.5909 (2)0.2136 (4)0.5281 (3)0.0405 (14)
H26A0.60050.21950.57240.061*
H26B0.55580.22790.52370.061*
H26C0.61020.25640.50250.061*
C270.6088 (2)0.0457 (5)0.5642 (3)0.0436 (15)
C280.5940 (2)0.0708 (6)0.6250 (4)0.062 (2)
H28A0.57780.12790.63150.074*
C290.6028 (3)0.0116 (8)0.6771 (4)0.074 (3)
H29A0.59390.03020.71850.089*
C300.6238 (3)0.0709 (8)0.6675 (5)0.070 (3)
H30A0.62910.11100.70220.084*
C310.6373 (3)0.0972 (6)0.6097 (4)0.062 (2)
H31A0.65210.15570.60360.074*
C320.6300 (2)0.0405 (5)0.5593 (4)0.0457 (16)
H32A0.64000.06120.51880.055*
C330.5551 (2)0.0858 (4)0.4593 (3)0.0444 (15)
C340.5151 (2)0.1423 (4)0.4492 (3)0.0413 (14)
H34A0.51470.20130.46830.050*
C350.4758 (2)0.1170 (5)0.4127 (3)0.0423 (15)
H35A0.44930.15870.40740.051*
C360.4739 (2)0.0349 (5)0.3842 (4)0.0493 (16)
H36A0.44620.01790.35950.059*
C370.5126 (3)0.0236 (6)0.3918 (5)0.074 (3)
H37A0.51170.08270.37280.089*
C380.5538 (3)0.0023 (6)0.4272 (5)0.067 (2)
H38A0.58130.03780.42950.081*
K10.63521 (4)0.17698 (7)0.13192 (5)0.0225 (2)
O40.6908 (2)0.1969 (3)0.2438 (2)0.0539 (13)
O50.59021 (16)0.1512 (3)0.2501 (2)0.0440 (10)
O60.68052 (14)0.3229 (2)0.0665 (2)0.0321 (9)
O70.57967 (15)0.3352 (3)0.0934 (2)0.0370 (9)
O80.68719 (13)0.0226 (3)0.0800 (2)0.0323 (9)
O90.58499 (13)0.0382 (3)0.06660 (19)0.0316 (8)
N20.74407 (17)0.1841 (3)0.1252 (3)0.0399 (12)
N30.52603 (17)0.1712 (3)0.1390 (3)0.0367 (11)
C390.7649 (3)0.2152 (5)0.1857 (4)0.0568 (19)
H39A0.76120.28270.18860.068*
H39B0.80060.20130.18600.068*
C400.7421 (3)0.1730 (5)0.2421 (4)0.065 (2)
H40A0.74590.10530.24040.077*
H40B0.75870.19550.28060.077*
C410.6699 (3)0.1606 (5)0.2991 (3)0.0543 (19)
H41A0.68820.18310.33640.065*
H41B0.67190.09270.29840.065*
C420.6184 (3)0.1899 (5)0.3028 (3)0.0520 (18)
H42A0.61660.25780.30140.062*
H42B0.60400.16900.34310.062*
C430.5393 (3)0.1761 (5)0.2556 (3)0.0495 (17)
H43A0.53580.24380.25490.059*
H43B0.52580.15310.29600.059*
C440.5117 (2)0.1341 (5)0.2009 (3)0.0485 (16)
H44A0.51730.06690.20090.058*
H44B0.47600.14450.20710.058*
C450.7583 (2)0.2471 (4)0.0750 (3)0.0430 (15)
H45A0.75180.21730.03390.052*
H45B0.79410.25850.07790.052*
C460.7319 (2)0.3381 (4)0.0766 (3)0.0406 (15)
H46A0.73710.36820.11790.049*
H46B0.74510.37900.04340.049*
C470.6549 (2)0.4078 (4)0.0635 (3)0.0367 (13)
H47A0.67040.44810.03160.044*
H47B0.65660.43910.10480.044*
C480.6024 (2)0.3903 (4)0.0461 (3)0.0404 (14)
H48A0.58470.44940.04220.049*
H48B0.60080.35830.00500.049*
C490.5290 (2)0.3193 (5)0.0787 (4)0.0483 (16)
H49A0.52630.28530.03840.058*
H49B0.51170.37870.07400.058*
C500.5058 (2)0.2641 (5)0.1312 (4)0.0495 (16)
H50A0.51000.29800.17120.059*
H50B0.47010.25900.12290.059*
C510.7628 (2)0.0919 (4)0.1118 (4)0.0478 (17)
H51A0.76100.05490.15080.057*
H51B0.79790.09690.09980.057*
C520.7361 (2)0.0415 (4)0.0605 (4)0.0450 (16)
H52A0.73560.07940.02180.054*
H52B0.75340.01670.05100.054*
C530.6610 (2)0.0244 (4)0.0311 (3)0.0382 (13)
H53A0.67830.08210.02010.046*
H53B0.65960.01460.00710.046*
C540.6099 (2)0.0454 (4)0.0535 (3)0.0356 (13)
H54A0.59190.08020.02070.043*
H54B0.61140.08370.09200.043*
C550.5348 (2)0.0197 (4)0.0827 (3)0.0399 (14)
H55A0.53320.01460.12300.048*
H55B0.51920.01820.04950.048*
C560.5077 (2)0.1108 (4)0.0891 (3)0.0388 (13)
H56A0.50980.14390.04850.047*
H56B0.47250.09780.09720.047*
K20.37144 (4)0.32115 (7)0.67152 (5)0.0278 (3)
O100.4324 (2)0.3508 (4)0.5644 (2)0.0635 (15)
O110.33319 (18)0.2979 (4)0.5500 (2)0.0503 (12)
O120.42078 (19)0.1605 (3)0.7159 (3)0.0540 (12)
O130.31818 (18)0.1755 (3)0.7270 (2)0.0441 (11)
O140.41652 (16)0.4584 (3)0.7459 (2)0.0422 (10)
O150.31684 (15)0.4755 (3)0.7123 (2)0.0370 (9)
N40.4804 (2)0.3234 (4)0.6868 (4)0.0608 (19)
N50.26389 (19)0.3164 (3)0.6549 (3)0.0411 (13)
C570.5027 (3)0.3645 (8)0.6302 (5)0.088 (3)
H57A0.53860.35310.63110.106*
H57B0.49760.43180.63130.106*
C580.4825 (4)0.3279 (10)0.5704 (5)0.099 (4)
H58A0.50110.35380.53440.119*
H58B0.48630.26030.56950.119*
C590.4153 (3)0.3079 (5)0.5103 (3)0.059 (2)
H59A0.41700.24040.51530.071*
H59B0.43580.32560.47370.071*
C600.3647 (3)0.3362 (5)0.4999 (3)0.057 (2)
H60A0.35340.31390.45830.068*
H60B0.36260.40410.50010.068*
C610.2829 (3)0.3242 (5)0.5402 (4)0.0575 (19)
H61A0.27150.30150.49870.069*
H61B0.28010.39200.54030.069*
C620.2513 (3)0.2849 (5)0.5910 (4)0.0525 (17)
H62A0.21660.30110.58230.063*
H62B0.25390.21700.58970.063*
C630.4985 (3)0.2297 (6)0.6946 (5)0.068 (2)
H63A0.53300.23240.70970.081*
H63B0.49870.19910.65300.081*
C640.4697 (3)0.1739 (6)0.7386 (5)0.073 (3)
H64A0.48590.11350.74410.088*
H64B0.46860.20470.78010.088*
C650.3931 (3)0.1040 (5)0.7584 (4)0.062 (2)
H65A0.39110.13390.80020.074*
H65B0.40950.04380.76350.074*
C660.3428 (3)0.0905 (4)0.7324 (4)0.0543 (19)
H66A0.34510.06100.69050.065*
H66B0.32400.04920.76050.065*
C670.2685 (3)0.1627 (4)0.7081 (4)0.0492 (18)
H67A0.25130.12330.73910.059*
H67B0.26750.13170.66660.059*
C680.2434 (3)0.2546 (4)0.7039 (4)0.0523 (18)
H68A0.20800.24460.69500.063*
H68B0.24590.28560.74530.063*
C690.4936 (3)0.3785 (5)0.7419 (5)0.065 (2)
H69A0.52960.38870.74200.078*
H69B0.48500.34400.78060.078*
C700.4678 (3)0.4699 (5)0.7429 (5)0.071 (3)
H70A0.47910.50570.77990.085*
H70B0.47640.50490.70450.085*
C710.3906 (2)0.5435 (4)0.7514 (3)0.0429 (15)
H71A0.39400.57900.71190.051*
H71B0.40470.58030.78620.051*
C720.3381 (2)0.5254 (4)0.7641 (3)0.0410 (14)
H72A0.33470.48920.80330.049*
H72B0.32050.58430.76980.049*
C730.2657 (2)0.4600 (4)0.7209 (4)0.0483 (17)
H73A0.24870.51940.72700.058*
H73B0.26040.42210.75910.058*
C740.2446 (2)0.4112 (4)0.6642 (4)0.0506 (17)
H74A0.20840.40820.66870.061*
H74B0.25190.44800.62610.061*
O160.8367 (2)0.2092 (4)0.3526 (3)0.0673 (15)
C750.8791 (4)0.2395 (8)0.3223 (6)0.091 (3)
H75A0.87810.30720.31760.110*
H75B0.88120.21190.27970.110*
C760.9223 (3)0.2129 (9)0.3595 (7)0.103 (4)
H76A0.94430.26620.36640.123*
H76B0.94100.16370.33810.123*
C770.9007 (4)0.1783 (6)0.4226 (6)0.080 (3)
H77A0.90380.11070.42630.096*
H77B0.91720.20760.45890.096*
C780.8485 (3)0.2063 (6)0.4185 (4)0.0595 (19)
H78A0.82730.16150.44060.071*
H78B0.84380.26760.43790.071*
O170.4260 (5)0.2513 (10)0.8786 (7)0.075 (4)*0.5
C790.3802 (9)0.3057 (16)0.8880 (10)0.072 (5)*0.5
H79A0.35330.28380.86040.087*0.5
H79B0.38590.37200.88020.087*0.5
C800.3684 (7)0.2852 (15)0.9628 (9)0.068 (5)*0.5
H80A0.34470.32910.98140.081*0.5
H80B0.35780.22110.97080.081*0.5
C810.4237 (13)0.304 (2)0.9836 (18)0.123 (11)*0.5
H81A0.43140.37060.98060.148*0.5
H81B0.42930.28391.02750.148*0.5
C820.4539 (10)0.2522 (19)0.9406 (14)0.103 (7)*0.5
H82A0.45880.18890.95640.123*0.5
H82B0.48640.28180.93530.123*0.5
O17B0.4414 (7)0.2715 (13)0.9034 (10)0.100 (5)*0.5
C79B0.4032 (9)0.3234 (16)0.8637 (13)0.089 (6)*0.5
H79C0.40460.39040.87180.106*0.5
H79D0.40810.31210.81810.106*0.5
C80B0.3583 (8)0.2855 (14)0.8849 (9)0.066 (5)*0.5
H80C0.33260.33360.88380.079*0.5
H80D0.34820.23590.85570.079*0.5
C81B0.3612 (7)0.2500 (15)0.9457 (10)0.070 (5)*0.5
H81C0.35360.18350.94490.084*0.5
H81D0.33650.28070.97290.084*0.5
C82B0.4160 (8)0.2659 (16)0.9746 (11)0.074 (5)*0.5
H82C0.42790.21330.99980.089*0.5
H82D0.41900.32390.99870.089*0.5
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
B10.043 (4)0.041 (4)0.040 (4)0.000 (3)0.008 (3)0.000 (3)
B20.035 (3)0.041 (4)0.034 (3)0.000 (3)0.001 (3)0.000 (3)
B30.036 (3)0.037 (3)0.034 (3)0.001 (3)0.001 (3)0.005 (3)
O10.041 (2)0.038 (2)0.052 (3)0.0030 (18)0.007 (2)0.0022 (19)
O20.039 (2)0.037 (2)0.046 (2)0.0065 (18)0.0003 (19)0.0097 (19)
O30.045 (2)0.038 (2)0.049 (3)0.0006 (18)0.007 (2)0.0067 (19)
C10.040 (3)0.036 (3)0.036 (3)0.005 (2)0.003 (2)0.010 (3)
C20.049 (3)0.031 (3)0.028 (3)0.005 (2)0.010 (2)0.008 (2)
C30.042 (3)0.034 (3)0.035 (3)0.005 (2)0.017 (3)0.010 (2)
C40.037 (4)0.087 (6)0.053 (4)0.006 (4)0.007 (3)0.005 (4)
C50.067 (5)0.061 (5)0.080 (6)0.002 (4)0.009 (4)0.036 (4)
C60.044 (4)0.042 (3)0.072 (5)0.007 (3)0.002 (3)0.015 (3)
C70.031 (3)0.048 (4)0.043 (3)0.005 (3)0.001 (3)0.001 (3)
C80.034 (3)0.079 (5)0.054 (4)0.019 (3)0.005 (3)0.012 (4)
C90.041 (4)0.115 (8)0.056 (5)0.019 (4)0.005 (3)0.021 (5)
C100.045 (4)0.124 (8)0.033 (4)0.009 (5)0.013 (3)0.021 (4)
C110.046 (4)0.066 (5)0.069 (5)0.004 (3)0.017 (4)0.019 (4)
C120.037 (3)0.043 (4)0.055 (4)0.008 (3)0.005 (3)0.001 (3)
C130.045 (3)0.055 (4)0.028 (3)0.003 (3)0.006 (2)0.002 (3)
C140.056 (4)0.045 (4)0.049 (4)0.014 (3)0.008 (3)0.006 (3)
C150.074 (5)0.037 (3)0.057 (4)0.018 (3)0.002 (4)0.009 (3)
C160.056 (5)0.095 (7)0.053 (4)0.030 (4)0.010 (4)0.022 (4)
C170.040 (3)0.063 (5)0.061 (4)0.008 (3)0.007 (3)0.026 (4)
C180.033 (3)0.062 (4)0.041 (3)0.003 (3)0.000 (3)0.003 (3)
C190.043 (3)0.053 (4)0.034 (3)0.001 (3)0.005 (3)0.004 (3)
C200.049 (4)0.039 (3)0.049 (4)0.001 (3)0.010 (3)0.005 (3)
C210.052 (4)0.057 (4)0.056 (4)0.014 (3)0.006 (3)0.013 (4)
C220.048 (4)0.041 (3)0.047 (4)0.005 (3)0.010 (3)0.007 (3)
C230.058 (4)0.034 (3)0.041 (3)0.004 (3)0.011 (3)0.001 (3)
C240.050 (4)0.036 (3)0.037 (3)0.002 (3)0.009 (3)0.001 (3)
B40.041 (4)0.044 (4)0.076 (6)0.004 (3)0.001 (4)0.013 (4)
N10.086 (5)0.062 (4)0.055 (4)0.019 (4)0.008 (4)0.002 (3)
C250.023 (3)0.063 (4)0.071 (5)0.004 (3)0.015 (3)0.032 (4)
C260.039 (3)0.020 (3)0.062 (4)0.001 (2)0.012 (3)0.005 (3)
C270.028 (3)0.049 (4)0.054 (4)0.006 (3)0.003 (3)0.007 (3)
C280.025 (3)0.068 (5)0.092 (6)0.002 (3)0.001 (3)0.032 (5)
C290.039 (4)0.144 (9)0.038 (4)0.019 (5)0.002 (3)0.013 (5)
C300.033 (4)0.105 (7)0.073 (6)0.016 (4)0.014 (4)0.027 (6)
C310.040 (4)0.065 (5)0.080 (6)0.006 (3)0.008 (4)0.030 (4)
C320.036 (3)0.042 (4)0.060 (4)0.006 (3)0.007 (3)0.005 (3)
C330.039 (3)0.041 (3)0.053 (4)0.009 (3)0.008 (3)0.011 (3)
C340.052 (4)0.032 (3)0.040 (3)0.001 (3)0.008 (3)0.010 (3)
C350.042 (3)0.048 (4)0.036 (3)0.008 (3)0.011 (3)0.016 (3)
C360.035 (3)0.048 (4)0.065 (4)0.001 (3)0.002 (3)0.002 (3)
C370.053 (5)0.051 (4)0.118 (8)0.013 (3)0.023 (5)0.037 (5)
C380.033 (4)0.065 (5)0.103 (7)0.012 (3)0.008 (4)0.006 (5)
K10.0211 (5)0.0246 (5)0.0218 (5)0.0034 (4)0.0017 (4)0.0003 (4)
O40.073 (3)0.059 (3)0.031 (2)0.024 (3)0.012 (2)0.008 (2)
O50.044 (2)0.060 (3)0.028 (2)0.008 (2)0.0118 (18)0.0045 (19)
O60.0296 (19)0.0231 (19)0.044 (2)0.0051 (14)0.0056 (17)0.0003 (16)
O70.031 (2)0.034 (2)0.046 (2)0.0045 (16)0.0025 (17)0.0027 (18)
O80.0252 (18)0.0274 (19)0.044 (2)0.0023 (14)0.0005 (16)0.0018 (17)
O90.0266 (18)0.033 (2)0.035 (2)0.0052 (15)0.0020 (15)0.0078 (16)
N20.024 (2)0.037 (3)0.058 (3)0.0057 (19)0.013 (2)0.002 (2)
N30.027 (2)0.037 (2)0.046 (3)0.0024 (18)0.008 (2)0.005 (2)
C390.049 (4)0.052 (4)0.070 (5)0.015 (3)0.025 (4)0.001 (4)
C400.066 (5)0.062 (5)0.066 (5)0.014 (4)0.043 (4)0.015 (4)
C410.090 (6)0.036 (3)0.037 (3)0.008 (3)0.013 (4)0.004 (3)
C420.081 (5)0.055 (4)0.020 (3)0.008 (4)0.003 (3)0.004 (3)
C430.050 (4)0.062 (4)0.037 (3)0.007 (3)0.024 (3)0.005 (3)
C440.041 (3)0.054 (4)0.050 (4)0.018 (3)0.019 (3)0.013 (3)
C450.020 (3)0.044 (3)0.065 (4)0.011 (2)0.006 (3)0.002 (3)
C460.036 (3)0.028 (3)0.058 (4)0.012 (2)0.013 (3)0.001 (3)
C470.045 (3)0.021 (3)0.044 (3)0.000 (2)0.013 (3)0.004 (2)
C480.045 (3)0.030 (3)0.046 (4)0.010 (3)0.002 (3)0.011 (3)
C490.035 (3)0.044 (4)0.067 (5)0.009 (3)0.001 (3)0.001 (3)
C500.027 (3)0.048 (4)0.074 (5)0.006 (2)0.013 (3)0.006 (4)
C510.024 (3)0.038 (3)0.082 (5)0.000 (2)0.010 (3)0.000 (3)
C520.022 (3)0.037 (3)0.076 (5)0.006 (2)0.004 (3)0.001 (3)
C530.039 (3)0.039 (3)0.037 (3)0.004 (3)0.001 (2)0.009 (3)
C540.038 (3)0.030 (3)0.038 (3)0.007 (2)0.006 (2)0.006 (2)
C550.028 (3)0.040 (3)0.051 (3)0.013 (2)0.003 (2)0.009 (3)
C560.021 (2)0.052 (4)0.044 (3)0.004 (2)0.001 (2)0.001 (3)
K20.0351 (6)0.0252 (6)0.0231 (5)0.0068 (4)0.0050 (4)0.0041 (4)
O100.072 (4)0.078 (4)0.041 (3)0.021 (3)0.015 (3)0.002 (3)
O110.055 (3)0.067 (3)0.029 (2)0.001 (2)0.006 (2)0.004 (2)
O120.058 (3)0.045 (3)0.059 (3)0.008 (2)0.000 (2)0.004 (2)
O130.062 (3)0.024 (2)0.046 (3)0.0058 (18)0.020 (2)0.0017 (17)
O140.043 (2)0.031 (2)0.053 (3)0.0010 (18)0.005 (2)0.0147 (19)
O150.033 (2)0.036 (2)0.042 (2)0.0053 (17)0.0069 (17)0.0058 (18)
N40.045 (3)0.056 (4)0.081 (5)0.009 (3)0.013 (3)0.031 (3)
N50.035 (3)0.032 (3)0.056 (3)0.008 (2)0.006 (2)0.006 (2)
C570.055 (5)0.107 (8)0.102 (8)0.039 (5)0.032 (5)0.022 (7)
C580.064 (6)0.156 (11)0.077 (7)0.011 (6)0.046 (6)0.011 (7)
C590.087 (6)0.046 (4)0.043 (4)0.006 (4)0.032 (4)0.006 (3)
C600.089 (6)0.059 (4)0.023 (3)0.009 (4)0.008 (3)0.002 (3)
C610.064 (5)0.051 (4)0.057 (4)0.010 (3)0.018 (4)0.005 (3)
C620.044 (3)0.042 (3)0.072 (5)0.010 (3)0.013 (3)0.014 (3)
C630.041 (4)0.075 (5)0.087 (6)0.011 (4)0.006 (4)0.030 (5)
C640.068 (5)0.059 (5)0.093 (7)0.029 (4)0.016 (5)0.020 (5)
C650.092 (6)0.036 (4)0.059 (5)0.017 (4)0.006 (4)0.005 (3)
C660.077 (5)0.030 (3)0.055 (4)0.001 (3)0.018 (4)0.004 (3)
C670.056 (4)0.036 (3)0.056 (4)0.022 (3)0.031 (3)0.007 (3)
C680.043 (4)0.038 (3)0.076 (5)0.016 (3)0.023 (3)0.005 (3)
C690.047 (4)0.062 (5)0.086 (6)0.007 (3)0.019 (4)0.028 (4)
C700.040 (4)0.052 (4)0.120 (8)0.002 (3)0.022 (4)0.035 (5)
C710.050 (4)0.033 (3)0.046 (4)0.002 (3)0.009 (3)0.014 (3)
C720.050 (4)0.032 (3)0.041 (3)0.003 (3)0.001 (3)0.010 (3)
C730.037 (3)0.030 (3)0.078 (5)0.003 (2)0.018 (3)0.011 (3)
C740.030 (3)0.035 (3)0.086 (5)0.004 (2)0.008 (3)0.004 (3)
O160.069 (4)0.077 (4)0.056 (3)0.006 (3)0.006 (3)0.009 (3)
C750.076 (6)0.094 (7)0.104 (8)0.011 (5)0.020 (6)0.038 (7)
C760.044 (5)0.120 (9)0.144 (11)0.006 (5)0.012 (6)0.041 (8)
C770.088 (7)0.056 (5)0.097 (7)0.016 (4)0.022 (6)0.009 (5)
C780.072 (5)0.057 (4)0.050 (4)0.005 (4)0.005 (4)0.005 (4)
Geometric parameters (Å, º) top
B1—O11.499 (8)O8—C531.433 (7)
B1—O31.508 (8)O9—C541.420 (7)
B1—C11.634 (10)O9—C551.432 (7)
B1—C71.655 (10)N2—C451.457 (9)
B2—O11.331 (8)N2—C511.463 (8)
B2—O21.374 (8)N2—C391.475 (9)
B2—C131.589 (9)N3—C561.464 (8)
B3—O31.342 (8)N3—C501.469 (8)
B3—O21.380 (8)N3—C441.472 (9)
B3—C191.601 (9)C39—C401.481 (12)
C1—C61.374 (9)C41—C421.466 (12)
C1—C21.394 (9)C43—C441.513 (10)
C2—C31.375 (9)C45—C461.507 (9)
C3—C41.368 (11)C47—C481.497 (9)
C4—C51.405 (12)C49—C501.511 (10)
C5—C61.370 (11)C51—C521.499 (10)
C7—C81.375 (10)C53—C541.500 (9)
C7—C121.401 (9)C55—C561.522 (9)
C8—C91.364 (12)K2—O112.802 (4)
C9—C101.366 (14)K2—O132.824 (4)
C10—C111.371 (13)K2—O142.826 (4)
C11—C121.408 (11)K2—O152.828 (4)
C13—C141.368 (10)K2—O102.848 (5)
C13—C181.413 (9)K2—O122.855 (5)
C14—C151.382 (10)K2—N52.947 (5)
C15—C161.372 (12)K2—N42.980 (7)
C16—C171.414 (13)O10—C591.387 (10)
C17—C181.373 (10)O10—C581.407 (12)
C19—C241.367 (9)O11—C611.436 (10)
C19—C201.387 (9)O11—C601.475 (9)
C20—C211.379 (9)O12—C641.429 (11)
C21—C221.435 (11)O12—C651.433 (10)
C22—C231.371 (10)O13—C661.412 (8)
C23—C241.394 (9)O13—C671.421 (9)
B4—C261.488 (10)O14—C701.406 (9)
B4—C251.614 (10)O14—C711.430 (7)
B4—C271.633 (11)O15—C731.421 (7)
B4—C331.648 (11)O15—C721.438 (7)
N1—C251.163 (10)N4—C631.459 (11)
C27—C321.384 (10)N4—C691.462 (10)
C27—C281.399 (11)N4—C571.474 (12)
C28—C291.423 (13)N5—C621.471 (9)
C29—C301.345 (14)N5—C681.483 (9)
C30—C311.336 (14)N5—C741.490 (8)
C31—C321.365 (11)C57—C581.482 (16)
C33—C341.380 (9)C59—C601.452 (12)
C33—C381.394 (11)C61—C621.493 (11)
C34—C351.369 (10)C63—C641.464 (14)
C35—C361.339 (10)C65—C661.486 (12)
C36—C371.365 (10)C67—C681.506 (10)
C37—C381.400 (12)C69—C701.504 (10)
K1—O92.805 (4)C71—C721.475 (9)
K1—O52.815 (4)C73—C741.510 (11)
K1—O62.819 (4)O16—C751.393 (12)
K1—O42.830 (5)O16—C781.435 (9)
K1—O72.872 (4)C75—C761.467 (14)
K1—O82.873 (4)C76—C771.546 (17)
K1—N22.965 (5)C77—C781.478 (13)
K1—N32.974 (5)O17—C791.49 (3)
O4—C411.405 (9)O17—C821.52 (3)
O4—C401.440 (11)C79—C801.65 (3)
O5—C431.435 (8)C80—C811.59 (4)
O5—C421.468 (8)C81—C821.44 (4)
O6—C471.420 (7)O17B—C79B1.54 (3)
O6—C461.431 (7)O17B—C82B1.66 (3)
O7—C481.425 (7)C79B—C80B1.41 (3)
O7—C491.431 (8)C80B—C81B1.39 (3)
O8—C521.420 (7)C81B—C82B1.63 (3)
O1—B1—O3109.9 (5)C45—N2—K1108.8 (3)
O1—B1—C1110.1 (5)C51—N2—K1109.0 (3)
O3—B1—C1107.2 (5)C39—N2—K1110.6 (4)
O1—B1—C7108.8 (5)C56—N3—C50110.1 (5)
O3—B1—C7109.8 (5)C56—N3—C44109.6 (5)
C1—B1—C7111.0 (5)C50—N3—C44109.8 (5)
O1—B2—O2122.2 (6)C56—N3—K1108.7 (3)
O1—B2—C13120.2 (6)C50—N3—K1110.0 (3)
O2—B2—C13117.6 (5)C44—N3—K1108.7 (4)
O3—B3—O2123.0 (6)N2—C39—C40114.6 (6)
O3—B3—C19120.5 (5)O4—C40—C39109.0 (6)
O2—B3—C19116.5 (5)O4—C41—C42108.7 (6)
B2—O1—B1123.3 (5)C41—C42—O5110.3 (5)
B2—O2—B3118.5 (5)O5—C43—C44108.3 (5)
B3—O3—B1121.9 (5)N3—C44—C43113.9 (5)
C6—C1—C2116.4 (6)N2—C45—C46114.2 (5)
C6—C1—B1119.4 (6)O6—C46—C45109.0 (5)
C2—C1—B1124.1 (6)O6—C47—C48109.3 (5)
C3—C2—C1123.1 (6)O7—C48—C47109.6 (5)
C4—C3—C2119.0 (6)O7—C49—C50109.1 (6)
C3—C4—C5119.7 (7)N3—C50—C49114.6 (5)
C6—C5—C4119.6 (7)N2—C51—C52114.9 (5)
C5—C6—C1122.3 (7)O8—C52—C51109.7 (6)
C8—C7—C12118.1 (7)O8—C53—C54109.1 (5)
C8—C7—B1123.0 (6)O9—C54—C53109.3 (5)
C12—C7—B1118.9 (6)O9—C55—C56108.6 (5)
C9—C8—C7121.1 (8)N3—C56—C55115.0 (5)
C8—C9—C10121.5 (8)O11—K2—O1395.89 (15)
C9—C10—C11119.7 (7)O11—K2—O14139.54 (15)
C10—C11—C12119.4 (7)O13—K2—O14121.34 (15)
C7—C12—C11120.3 (7)O11—K2—O15100.52 (14)
C14—C13—C18116.2 (6)O13—K2—O15101.51 (13)
C14—C13—B2122.1 (6)O14—K2—O1559.70 (12)
C18—C13—B2121.7 (6)O11—K2—O1059.95 (16)
C13—C14—C15120.1 (7)O13—K2—O10138.17 (15)
C16—C15—C14123.1 (7)O14—K2—O1094.97 (15)
C15—C16—C17118.9 (7)O15—K2—O10115.46 (16)
C18—C17—C16116.3 (7)O11—K2—O12112.31 (15)
C17—C18—C13125.3 (7)O13—K2—O1259.27 (15)
C24—C19—C20118.6 (6)O14—K2—O12100.96 (14)
C24—C19—B3121.8 (6)O15—K2—O12142.74 (15)
C20—C19—B3119.6 (6)O10—K2—O1296.54 (17)
C21—C20—C19121.7 (6)O11—K2—N561.21 (15)
C20—C21—C22120.0 (7)O13—K2—N561.52 (15)
C23—C22—C21116.5 (6)O14—K2—N5120.95 (13)
C22—C23—C24122.7 (6)O15—K2—N562.25 (13)
C19—C24—C23120.4 (7)O10—K2—N5119.07 (17)
C26—B4—C25110.9 (6)O12—K2—N5119.12 (15)
C26—B4—C27113.2 (7)O11—K2—N4118.08 (18)
C25—B4—C27104.2 (6)O13—K2—N4118.20 (18)
C26—B4—C33109.1 (6)O14—K2—N460.00 (14)
C25—B4—C33106.6 (7)O15—K2—N4118.67 (14)
C27—B4—C33112.5 (6)O10—K2—N460.4 (2)
N1—C25—B4171.6 (9)O12—K2—N460.39 (17)
C32—C27—C28115.2 (7)N5—K2—N4179.04 (16)
C32—C27—B4125.9 (7)C59—O10—C58107.1 (7)
C28—C27—B4118.8 (7)C59—O10—K2113.4 (4)
C27—C28—C29120.6 (7)C58—O10—K2117.1 (5)
C30—C29—C28119.6 (8)C61—O11—C60110.4 (6)
C31—C30—C29120.7 (8)C61—O11—K2117.1 (4)
C30—C31—C32120.4 (9)C60—O11—K2113.7 (4)
C31—C32—C27123.3 (8)C64—O12—C65110.9 (7)
C34—C33—C38115.1 (6)C64—O12—K2115.9 (4)
C34—C33—B4120.8 (6)C65—O12—K2115.5 (4)
C38—C33—B4124.2 (6)C66—O13—C67111.1 (5)
C35—C34—C33122.8 (6)C66—O13—K2116.6 (4)
C36—C35—C34121.7 (6)C67—O13—K2117.9 (4)
C35—C36—C37118.3 (7)C70—O14—C71112.9 (5)
C36—C37—C38120.8 (7)C70—O14—K2119.3 (4)
C33—C38—C37121.1 (7)C71—O14—K2116.3 (3)
O9—K1—O597.61 (12)C73—O15—C72112.0 (5)
O9—K1—O6120.79 (13)C73—O15—K2115.3 (3)
O5—K1—O6136.77 (13)C72—O15—K2115.1 (3)
O9—K1—O4138.46 (13)C63—N4—C69109.8 (7)
O5—K1—O459.89 (14)C63—N4—C57109.4 (7)
O6—K1—O495.88 (13)C69—N4—C57109.2 (7)
O9—K1—O7100.40 (12)C63—N4—K2109.8 (4)
O5—K1—O797.57 (13)C69—N4—K2109.7 (4)
O6—K1—O759.09 (12)C57—N4—K2109.0 (6)
O4—K1—O7115.96 (14)C62—N5—C68111.7 (5)
O9—K1—O859.14 (11)C62—N5—C74109.2 (6)
O5—K1—O8116.81 (13)C68—N5—C74109.6 (5)
O6—K1—O8100.66 (11)C62—N5—K2110.4 (4)
O4—K1—O897.99 (15)C68—N5—K2107.7 (4)
O7—K1—O8140.91 (13)C74—N5—K2108.1 (3)
O9—K1—N2119.17 (13)N4—C57—C58113.6 (7)
O5—K1—N2118.79 (15)O10—C58—C57110.6 (9)
O6—K1—N260.90 (13)O10—C59—C60108.5 (6)
O4—K1—N260.26 (16)C59—C60—O11109.5 (6)
O7—K1—N2118.90 (13)O11—C61—C62109.9 (6)
O8—K1—N261.17 (12)N5—C62—C61114.4 (5)
O9—K1—N361.21 (12)N4—C63—C64114.2 (6)
O5—K1—N361.12 (15)O12—C64—C63111.1 (8)
O6—K1—N3118.86 (13)O12—C65—C66109.1 (6)
O4—K1—N3119.57 (16)O13—C66—C65110.6 (6)
O7—K1—N360.81 (13)O13—C67—C68109.4 (5)
O8—K1—N3119.23 (12)N5—C68—C67114.1 (5)
N2—K1—N3179.61 (15)N4—C69—C70112.5 (7)
C41—O4—C40108.8 (6)O14—C70—C69110.9 (6)
C41—O4—K1116.5 (4)O14—C71—C72109.8 (5)
C40—O4—K1118.1 (4)O15—C72—C71109.9 (5)
C43—O5—C42110.1 (5)O15—C73—C74110.1 (5)
C43—O5—K1117.3 (4)N5—C74—C73114.0 (6)
C42—O5—K1113.6 (4)C75—O16—C78105.8 (7)
C47—O6—C46110.5 (4)O16—C75—C76109.3 (9)
C47—O6—K1117.6 (3)C75—C76—C77104.4 (8)
C46—O6—K1118.1 (3)C78—C77—C76102.9 (8)
C48—O7—C49110.8 (5)O16—C78—C77106.3 (7)
C48—O7—K1115.1 (3)C79—O17—C82107.3 (16)
C49—O7—K1116.0 (3)O17—C79—C80101.2 (15)
C52—O8—C53110.3 (5)C81—C80—C7993 (2)
C52—O8—K1114.9 (3)C82—C81—C80106 (3)
C53—O8—K1114.0 (3)C81—C82—O17106 (2)
C54—O9—C55110.0 (4)C79B—O17B—C82B103.9 (17)
C54—O9—K1118.8 (3)C80B—C79B—O17B102.6 (19)
C55—O9—K1118.7 (3)C81B—C80B—C79B113 (2)
C45—N2—C51110.0 (6)C80B—C81B—C82B110.4 (18)
C45—N2—C39109.9 (5)C81B—C82B—O17B92.6 (15)
C51—N2—C39108.5 (5)
Selected bond lengths and angles (Å, °) for 1-Dy and 1-Y top
1-Dy1-Y
Ln1—O12.3790 (18)2.369 (2)
Ln1—O22.3838 (17)2.370 (2)
Ln1—O32.4022 (16)2.390 (2)
Ln1—O42.3932 (17)2.382 (2)
Ln1—N12.431 (2)2.420 (3)
Ln1—Cl12.5888 (6)2.5803 (9)
Ln1—Cl22.5835 (6)2.5730 (8)
N1—C11.141 (3)1.144 (4)
B1—C11.621 (3)1.629 (4)
B1—C181.625 (3)1.630 (5)
B1—C241.632 (4)1.626 (5)
B1—C301.641 (3)1.642 (5)
C1—N1—Ln1163.92 (19)164.6 (3)
N1—C1—B1178.7 (3)178.4 (3)
 

Acknowledgements

We thank Dr Michael Wojnar for assistance with X-ray crystallography.

Funding information

Funding for this research was provided by: National Science Foundation (grant No. CHE-1855328).

References

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