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Acta Crystallographica Section E: Crystallographic Communications logoLink to Acta Crystallographica Section E: Crystallographic Communications
. 2020 Apr 21;76(Pt 5):710–714. doi: 10.1107/S2056989020005289

Structure of a push–pull olefin prepared by ynamine hydro­boration with a borandiol ester

Joël Gubler a, Peter Chen a,*
PMCID: PMC7199258  PMID: 32431937

The title compound is a demonstration of hydro­boration of ynamines with borandiol ester. The bond lengths of the resulting push–pull olefin are discussed.

Keywords: crystal structure, hydro­boration, ynamine, push–pull olefin

Abstract

N-[(Z)-2-(2H-1,3,2-Benzodioxaborol-2-yl)-2-phenyl­ethen­yl]-N-(propan-2-yl)aniline, C23H22BNO2, contains a C=C bond that is conjugated with a donor and an acceptor group. An analysis that included similar push–pull olefins revealed that bond lengths in their B—C=C—N core units correlate with the perceived acceptor and donor strength of the groups. The two phenyl groups in the mol­ecule are rotated with respect to the plane that contains the BCCN atoms, and are close enough for significant π-stacking. Definite characterization of the title compound demonstrates, for the first time in a reliable way, that hydro­boration of ynamines with borandiol esters is feasible. Compared to olefin hydro­boration with borane, the ynamine substrate is activated enough to undergo reaction with the less active hydro­boration reagent catecholborane.

Chemical context  

Boronic esters are frequently used to transfer organic groups to transition metals, for example in the transmetallation step of the Suzuki–Miyaura reaction. Hydro­boration of ynamines with borandiol esters produces amino-functionalized boronic esters in one step and perfect atom economy.graphic file with name e-76-00710-scheme1.jpg

For true ynamines, to the best of our knowledge, only two attempts of such reactions have been reported so far. These either failed (Witulski et al., 2000) or were reported without reaction details and characterization data (Zhuo et al., 2001). More recently it was found that the exceptionally active Pier’s borane, HB(C6F5)2, can readily hydro­borate l-propynyl-2,2,6,6-tetra­methyl­piperidine (Wang et al., 2018). Borandiol esters are expected to be less reactive because the electron deficiency at the boron is reduced by π-donation from the oxygen atoms.

Given the limited precedent for ynamine hydro­boration, the more comprehensive literature for enamine hydro­boration was consulted (Goralski & Singaram, 2012; Dembitsky et al., 2002), as their reactivity is expected to be controlled by similar effects. Compared to simple olefin substrates, conjugation of the C=C bond with nitro­gen dictates the regioselectivity and increases the reactivity of enamines. However, the presence of a nitro­gen atom in the reactant and product enables the formation of unreactive Lewis acid–base adducts with the hydro­borating reagent. Building on the vast knowledge of the reactivity of different borane-amine adducts in hydro­boration (Brown & Murray, 1984; Brown et al., 1999), a bulky iso-propyl and an phenyl group were selected as substituents for the ynamine nitro­gen. The former should weaken adducts for steric reasons, whereas the phenyl group is expected to reduce the nucleophilicity of the nitro­gen by conjugation.

Ynamine hydro­boration using a borandiol ester was reinvestigated and succeeded for a substrate that follows the developed design principles. The product of such a reaction contains a C=C double bond flanked by both an electron-donating group (EDG), the amine, and an electron-withdrawing group (EWG), the boronate. Therefore it belongs to the class of push–pull (captodative) olefins, which are known to have unusual properties such as weak π-bonds or biradical reactivity (Viehe et al., 1985).

Structural commentary  

The asymmetric unit (Fig. 1) contains two almost identical (r.m.d.s = 0.11 Å) independent mol­ecules. As judged by the B1—C11—C10—N1 torsion angles of 171.6 (2) and 175.5 (2)°, the central C—C bond is only slightly twisted from planarity. The two phenyl groups in the mol­ecule are rotated, by 43 and 49°, with respect to that plane. The centroids of two phenyl groups in one mol­ecule are on average 3.747 Å apart, which suggests intra­molecular π-stacking. The mean distances are 1.521 Å for the B1—C11 bond, 1.365 Å for the C10—N1 bond and 1.369 Å for the central C10—C11 bond.

Figure 1.

Figure 1

The mol­ecular structures of the two independent mol­ecules of the title compound 1 with displacement ellipsoids drawn at the 50% probability level.

Supra­molecular features  

There is a short inter­molecular contact between the boron atom and an aniline ortho-HB1B⋯H9A(1 − x, 1 − y, Inline graphic + z) = 2.771 Å and B1A⋯H5B(1 − x, −y, −Inline graphic + z) = 2.856 Å (ΣrvdW[B,H] = 3.11 Å). The shortest inter­molecular distances between the catechol unit and boron are B1A⋯C21B i = 3.540 (4) Å, B1A⋯C20B i = 3.686 (4) Å (ΣrvdW[B,C] = 3.68 Å), B1A⋯H21B i = 3.113 Å and B1A⋯H20B i = 3.381 Å [symmetry code: (i) Inline graphic + x, 1 − y, z]. In addition there is a short contact between one of the other catechol hydrogen atoms and the meta-carbon of the aniline, H22B⋯C6B(x, 1 + y, z) of 2.877 Å (ΣrvdW[C,H] = 2.97 Å). All of these inter­actions involve atoms that are part of arenes and could be seen as inter­molecular π-stacking.

Methyl hydrogen atoms of the isopropyl group are at van der Waals distances with one of the oxygen atoms [O2A⋯H2BA(1 − x, −y, −Inline graphic + z) = 2.698 Å, O2B⋯H3AB(1 − x, 1 − y, Inline graphic + z) = 2.631 Å, ΣrvdW[O,H] = 2.70 Å] and with one of the anilic meta-H atoms [H8A⋯H2BC(1 − x, −y, −Inline graphic + z) = 2.388 Å, ΣrvdW[H,H] = 2.40 Å]. The nitro­gen atom is steric­ally shielded by surrounding groups and does not have any close inter­molecular neighbours.

Database survey  

Contributions from the zwitterionic resonance structure B=C—C=N+ are expected to increase with donor and acceptor group strength. This should be observable as a shortening of the B—C and C—N bonds and an elongation of the C—C bond. Following this idea, bond lengths of 1 were compared to those in the structurally related compounds 25 (Table 1, Fig. 2). C—N bond lengths are 1.341 Å (4), 1.350 Å (5), 1.362 Å (3), 1.365 Å (1), 1.394 Å (2). These numbers follow the expected N-donor strength, when the latter is estimated by the number of conjugating substituents on the nitro­gen: piperidine, diisopropyl > aniline > indole, carbazole. B—C lengths are 1.491 Å (4), 1.513 Å (3), 1.516 Å (5), 1.521 Å (1), 1.537 Å (2). Similarly, these numbers follow the B-acceptor strength: B(C6F5)2 > catecholboryl > pinacolboryl (Adamczyk-Woźniak et al., 2011). Following this, the zwitterionic resonance structure is most important in 4, which has a strong donor and a strong acceptor. On the other end of the scale lies 2, which has a weak donor and a weak acceptor. The other mol­ecules, including 1, lie between these two extremes.

Table 1. Comparison of bond lengths (in Å) in 1 with those in the similar compounds 25 .

Average distances and standard deviations are given whenever there is more than one mol­ecule in the asymmetric unit. Typical bond lengths for vinyl­boranes and conjugated enamines were obtained from statistical analysis.

Compound B—C C—C C—N CCDC
1 1.521 (3) 1.369 (3) 1.365 (3) title compound
2 1.537 (4) 1.335 (4) 1.394 (3) 861787a
3 1.513 (4) 1.380 (3) 1.362 (3) 1529736
4 1.491 (7) 1.393 (6) 1.341 (6) 1843575c
5 1.516 (2) 1.371 (2) 1.350 (2) 1997665d
Vinyl boronates 1.561 (15) 1.341 (12)
Enamines ∼1.34 ∼1.36

Notes: (a) Hatayama & Okuno (2012); (b) Liu et al. (2017); (c) Wang et al. (2018); (d) new.

Figure 2.

Figure 2

Chemical structure of reference compounds. 9-[(E)-2-(4,4,5,5-Tetra­methyl-1,3,2-dioxaborolan-2-yl)ethen­yl]-9H-carbazole, 2 (Hatayama & Okuno, 2012), 3-(2H-1,3,2-benzodioxaborol-2-yl)-1-methyl-1H-indole, 3 (Liu et al., 2017), 1-{(Z)-2-[bis­(penta­fluoro­phen­yl)boran­yl]prop-1-en-1-yl}-2,2,6,6-tetra­methyl­piperidine, 4 (Wang et al., 2018) and N-[(Z)-2-(2H-1,3,2-benzodioxaborol-2-yl)-2-phenyl­ethen­yl]-N-(propan-2-yl)propan-2-amine, 5 (CCDC 1997665).

In order to compare with olefins that either have a donor or an acceptor group, the Cambridge Structural Database (CSD, Version 5.41, update of November 2019; Groom et al., 2016) was searched for vinyl boronates and enamines. Bond-length distributions and the exact query structures are shown in Fig. 3 and Fig. 4. The data set for vinyl boronates consists of about 90% of pinacol boronates and contains only a few catechol boronates. Compared with typical bond lengths in this data set, the B—C bond is shorter and the C=C bond is longer in 15, which indicates stronger conjugation. The only exception is 2, whose C=C bond is shorter.

Figure 3.

Figure 3

Statistical analysis of B—C and C—C bond lengths in vinyl boronates. The query substructure and restrictions are shown on the left. Problematic or irrelevant structures were removed. The bond distances of reference compounds are marked.

Figure 4.

Figure 4

Statistical analysis of C—C and C—N bond lengths in enamines. The query substructure and restrictions are shown on the left. Problematic or irrelevant structures were removed. The bond distances of reference compounds are marked.

For enamines the C—C bond length has an average of 1.341 Å, which is about 0.025 Å longer than the value of 1.316 (15) Å for regular inter­nal olefins (Allen et al., 2006). In 1, 3, 4 and 5, the C—C bonds are on average 1.378 Å, and thereby longer than in enamines. C—N bond lengths for enamines are distributed more uniformly than C—C lengths. Inspection of the structures in which C—N distances are longer than 1.39 Å revealed that these structures typically either have a nitro­gen whose lone pair is not coplanar with the C=C bond, or a nitro­gen that is part of a carbazole or morpholine. As conjugation with the formal double bond between C10 and C11 is absent or reduced in these, only structures with C—N bond lengths below 1.39 Å were used for comparison. The average C—N bond length of about 1.36 Å for that subset is similar to the C—N bond lengths in 1, 3, 4 and 5. Overall, comparison with enamines reveals that C—C bonds are longer in push–pull olefins, whereas C—N bond lengths are unaffected. This suggests that conjugation with the boron affects the C—C bond length more than the C—N bond length.

Synthesis and crystallization  

The title compound was prepared by the multi-step sequence shown in Fig. 5.

Figure 5.

Figure 5

Reaction sequence used for the synthesis of the title compound.

N -isopropyl- N -(phenyl­ethyn­yl)aniline: In a 100 ml Schlenk flask, 5.8 ml of N-isopropyl amine (40 mmol, 1.0 eq.) were diluted with 40 ml of dry THF. 24.7 ml of a n-BuLi solution in hexa­nes (1.62 mol l−1, 40 mmol, 1.0 eq.) were added over 5 min at 195 K. A colourless solid formed and after 15 min the suspension was warmed to room temperature over 30 min. Upon addition of 5.69 g of 2-chloro­ethynyl­benzene (96%, 40 mmol, 1.0 eq., prepared according to Li et al., 2014), the reaction mixture turned black. The sealed Schlenk flask was heated in an oil bath at 338 K (caution: the closed flask may burst if this temperature is exceeded). The reaction progress was monitored by GC–FID. After 6 h the reaction mixture was cooled to room temperature. 100 ml of tert-butyl methyl ether were added, the organic phase washed with ice-cold water (3 × 50 ml), dried with MgSO4 and concentrated on the rotavap. 8.25 g of black viscous liquid were obtained and purified by Kugelrohr distillation (433 K, 0.2 mbar) to yield 6.34 g (purity 83 wt%, yield 56%) of the colourless liquid N-isopropyl-N-(phenyl­ethyn­yl)aniline. 1H NMR (400 MHz, CDCl3): δ (ppm) = 1.40 (d, 6.5 Hz, 6H, 2 × CH3), 4.10 (hept, 6.4 Hz, 1H, CH of i-Pr), 6.92 (tt, 7.4 Hz, 1.2 Hz, 1H, para-H of aniline), 7.16–7.33 (m, 7H, arene H), 7.38–7.41 (m, 2H, ortho-H of phenyl group). 13C{1H} NMR (100 MHz, CDCl3): δ (ppm) = 20.6 (s, 2 × CH3), 49.6 (s, CH of i-Pr), 72.0 (s, alkynic carbon farther from N), 86.4 (s, alkynic carbon closer to N), 115.5 (s, ortho-C of aniline), 120.8 (s, para-C of aniline), 125.2 (s, ipso-C of phenyl group), 126.2 (s, para-C of phenyl group), 128.4 (s, meta-C of phenyl group), 129.3 (s, meta-C of aniline), 130.2 (s, ortho-C of phenyl group), 144.4 (s, ipso-C of aniline). EI–MS (70 eV) m/z = 236, 235 (M +), 220 (M + − CH3), 194, 193, 192 (M + − C3H7), 165, 117, 115, 90, 89, 77, 63, 51, 43. ATR–IR ν (cm−1)(%T) = 534 (70), 629 (61), 688 (22), 745 (18), 783 (82), 865 (87), 881 (87), 904 (87), 996 (80), 1025 (73), 1056 (66), 1129 (70), 1147 (52), 1170 (67), 1254 (41), 1312 (67), 1348 (77), 1367 (76), 1396 (51), 1490 (38), 1594 (46), 1932 (96), 2217 (38, C≡C-stretch), 2872 (94), 2932 (91), 2976 (80), 3034 (93), 3057 (93).

N -[( Z )-2-(2 H -1,3,2-benzodioxaborol-2-yl)-2-phenyl­ethen­yl]- N -(propan-2-yl)aniline: Under a counterflow of argon, 3.08 g of N-isopropyl-N-(phenyl­ethyn­yl)aniline (13.1 mmol, 1.0 eq.) were placed in an oven-dried 20 ml Schlenk flask with a Young valve. The flask and its contents were purged three times by applying high vacuum followed by flushing with argon. 6.5 ml dry tert-butyl methyl ether were added and the mixture stirred vigorously to ensure mixing of the two liquids. 2.1 ml of catecholborane (19.5 mmol, 1.5 eq.) were added, the flask closed, and the reaction mixture heated to 323 K for 16 h. Cooling to room temperature led to the precipitation of the product. The supernatant was removed and the precipitate recrystallized from 40 ml of tert-butyl methyl ether. X-ray quality crystals were obtained in a yield of 1.88 g (40%). Notes: (a) Schlenk techniques are necessary because ynamines and catecholborane are moisture-sensitive; (b) the reaction also works well in diethyl ether, 1,4-dioxane or THF.

1H NMR (600 MHz, CDCl3): δ (ppm) = 1.34 (d, 6.8 Hz, 6H, CH3 of i-Pr), 3.89 (hept, 6.8 Hz, 1H, CH of i-Pr), 6.77–6.80 (m, 2H, H5 & H9), 6.81–6.85 (m, 2H, H7 & H15), 6.85–6.92 (m, 6H, H6 & H8 & H13 & H14 & H16 & H17), 6.95–6.98 (m, 2H, 2 × catechol-H), 7.11–7.14 (m, 2H, 2 × catechol-H), 7.53 (s, 1H, H10).

13C1H NMR (151 MHz, CDCl3): δ (ppm) = 22.2 (s, C1 & C2), 57.4 (s, C3), 98.1 (br s, C11), 111.7 (s, 2 × catechol-C), 121.8 (s, 2 × catechol-C), 124.3 (s, C15), 124.6 (s, C7), 126.3 (s, C5 & C9), 126.9 (s, C14 & C16), 128.0 (s, C6 & C8), 129.4 (s, C13 & C17), 138.8 (s, C12), 143.3 (s, C4), 144.9 (s, C10), 148.9 (s, C18 & C23). Inverse gated {13}C{1}H} NMR with D1 = 60 s measured to get integrable 13C NMR.

11B NMR (160 MHz, CDCl3): δ (ppm) = 33.2 (s).

Refinement  

Crystal data, data collection and structure refinement details are summarized in Table 2. H atoms were positioned geometrically and refined as riding: C—H = 0.95–0.98 Å and U iso(H) = 1.2U eq(C) or 1.5U eq(C-meth­yl). The absolute structure was not determined because of unreliable Flack and Hooft parameters.

Table 2. Experimental details.

Crystal data
Chemical formula C23H22BNO2
M r 355.22
Crystal system, space group Orthorhombic, P c a21
Temperature (K) 100
a, b, c (Å) 17.8540 (11), 11.5361 (6), 18.5366 (12)
V3) 3817.9 (4)
Z 8
Radiation type Mo Kα
μ (mm−1) 0.08
Crystal size (mm) 0.38 × 0.2 × 0.07
 
Data collection
Diffractometer Bruker–Nonius Kappa APEXII
Absorption correction Multi-scan (SADABS; Bruker, 2015)
T min, T max 0.703, 0.733
No. of measured, independent and observed [I > 2σ(I)] reflections 60829, 8781, 7379
R int 0.047
(sin θ/λ)max−1) 0.652
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.039, 0.086, 1.03
No. of reflections 8781
No. of parameters 491
No. of restraints 1
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.25, −0.24

Computer programs: APEX2 and SAINT (Bruker, 2015), SHELXT (Sheldrick, 2015a ), SHELXL (Sheldrick, 2015b ) and OLEX2 (Dolomanov et al., 2009).

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989020005289/lh5953sup1.cif

e-76-00710-sup1.cif (1.8MB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989020005289/lh5953Isup2.hkl

e-76-00710-Isup2.hkl (697.1KB, hkl)

Supporting information file. DOI: 10.1107/S2056989020005289/lh5953Isup3.cml

CCDC reference: 1997061

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

Acknowledgments

X-ray services were provided by SMoCC – The Small Mol­ecule Crystallography Center of ETH Zurich. The authors acknowledge Kevin Breitwieser and Nils Trapp for proof-reading the manuscript.

supplementary crystallographic information

Crystal data

C23H22BNO2 Dx = 1.236 Mg m3
Mr = 355.22 Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pca21 Cell parameters from 9981 reflections
a = 17.8540 (11) Å θ = 2.5–26.8°
b = 11.5361 (6) Å µ = 0.08 mm1
c = 18.5366 (12) Å T = 100 K
V = 3817.9 (4) Å3 Plate, clear light yellow
Z = 8 0.38 × 0.2 × 0.07 mm
F(000) = 1504

Data collection

Bruker–Nonius Kappa APEXII diffractometer 8781 independent reflections
Radiation source: sealed tube 7379 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.047
Detector resolution: 8.33 pixels mm-1 θmax = 27.6°, θmin = 2.8°
ω and φ scans h = −23→23
Absorption correction: multi-scan (SADABS; Bruker, 2015) k = −14→14
Tmin = 0.703, Tmax = 0.733 l = −24→24
60829 measured reflections

Refinement

Refinement on F2 Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.039 w = 1/[σ2(Fo2) + (0.0401P)2 + 0.7053P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.086 (Δ/σ)max < 0.001
S = 1.03 Δρmax = 0.25 e Å3
8781 reflections Δρmin = −0.24 e Å3
491 parameters Absolute structure: Flack x determined using 3185 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
1 restraint Absolute structure parameter: −0.7 (4)
Primary atom site location: structure-invariant direct methods

Special details

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. 8 reflections were omitted (some are equivalents). These were checked visually and are all results of high background around the beamstop (beginning ice formation or crystalline powder covering the sample). 0 1 0 is clearly shadowed by the beamstop. Absolute structure is not claimed due to unreliable Flack and Hooft parameters.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
O1B 0.18188 (9) 0.59842 (13) 0.60028 (9) 0.0155 (4)
O2B 0.30086 (9) 0.67252 (13) 0.61169 (9) 0.0158 (4)
N1B 0.23745 (11) 0.25154 (16) 0.65127 (11) 0.0159 (4)
C1B 0.10503 (15) 0.2002 (2) 0.62440 (14) 0.0210 (6)
H1BA 0.0874 0.2806 0.6251 0.032*
H1BB 0.0642 0.1485 0.6390 0.032*
H1BC 0.1215 0.1800 0.5756 0.032*
C2B 0.14877 (15) 0.2209 (2) 0.75303 (14) 0.0205 (6)
H2BA 0.1928 0.2152 0.7844 0.031*
H2BB 0.1096 0.1686 0.7707 0.031*
H2BC 0.1301 0.3008 0.7533 0.031*
C3B 0.17032 (14) 0.1869 (2) 0.67659 (13) 0.0160 (5)
H3B 0.1840 0.1028 0.6776 0.019*
C4B 0.30570 (13) 0.18933 (19) 0.64199 (14) 0.0147 (5)
C5B 0.32986 (14) 0.1121 (2) 0.69452 (14) 0.0189 (5)
H5B 0.3009 0.1007 0.7369 0.023*
C6B 0.39606 (14) 0.0518 (2) 0.68521 (16) 0.0230 (6)
H6B 0.4126 −0.0006 0.7214 0.028*
C7B 0.43822 (15) 0.0673 (2) 0.62365 (16) 0.0275 (6)
H7B 0.4841 0.0267 0.6177 0.033*
C8B 0.41341 (15) 0.1423 (2) 0.57066 (15) 0.0238 (6)
H8B 0.4420 0.1522 0.5279 0.029*
C9B 0.34704 (14) 0.2033 (2) 0.57938 (14) 0.0191 (5)
H9B 0.3301 0.2543 0.5426 0.023*
C10B 0.23179 (13) 0.36795 (19) 0.63924 (13) 0.0151 (5)
H10B 0.1820 0.3949 0.6321 0.018*
C11B 0.28538 (13) 0.4526 (2) 0.63563 (13) 0.0156 (5)
C12B 0.36555 (13) 0.4370 (2) 0.65557 (13) 0.0142 (5)
C13B 0.38562 (14) 0.3878 (2) 0.72178 (13) 0.0172 (5)
H13B 0.3476 0.3630 0.7541 0.021*
C14B 0.46041 (15) 0.3748 (2) 0.74087 (14) 0.0209 (5)
H14B 0.4731 0.3410 0.7860 0.025*
C15B 0.51658 (14) 0.4110 (2) 0.69433 (14) 0.0210 (6)
H15B 0.5677 0.4012 0.7071 0.025*
C16B 0.49740 (14) 0.4614 (2) 0.62906 (14) 0.0188 (5)
H16B 0.5356 0.4869 0.5972 0.023*
C17B 0.42288 (14) 0.4749 (2) 0.60995 (14) 0.0169 (5)
H17B 0.4106 0.5103 0.5652 0.020*
C18B 0.18063 (14) 0.71629 (19) 0.58605 (13) 0.0140 (5)
C19B 0.12056 (14) 0.7829 (2) 0.56544 (13) 0.0178 (5)
H19B 0.0715 0.7518 0.5614 0.021*
C20B 0.13606 (15) 0.8997 (2) 0.55079 (14) 0.0198 (5)
H20B 0.0966 0.9492 0.5356 0.024*
C21B 0.20801 (15) 0.9445 (2) 0.55794 (13) 0.0192 (5)
H21B 0.2165 1.0242 0.5478 0.023*
C22B 0.26793 (14) 0.8754 (2) 0.57958 (13) 0.0179 (5)
H22B 0.3171 0.9059 0.5849 0.022*
C23B 0.25211 (13) 0.76087 (19) 0.59287 (13) 0.0151 (5)
B1B 0.25681 (15) 0.5724 (2) 0.61526 (14) 0.0149 (6)
O1A 0.59813 (9) −0.09865 (13) 0.40292 (10) 0.0176 (4)
O2A 0.71747 (9) −0.17253 (13) 0.39845 (9) 0.0174 (4)
N1A 0.65302 (11) 0.24387 (17) 0.34366 (11) 0.0161 (4)
C1A 0.52189 (14) 0.2942 (2) 0.37802 (15) 0.0228 (6)
H1AA 0.5416 0.3104 0.4263 0.034*
H1AB 0.5027 0.2146 0.3764 0.034*
H1AC 0.4813 0.3485 0.3671 0.034*
C2A 0.58421 (14) 0.3081 (2) 0.32256 (14) 0.0177 (5)
H2A 0.5976 0.3923 0.3213 0.021*
C3A 0.55869 (14) 0.2754 (2) 0.24731 (15) 0.0227 (6)
H3AA 0.5407 0.1952 0.2473 0.034*
H3AB 0.6008 0.2829 0.2137 0.034*
H3AC 0.5180 0.3272 0.2323 0.034*
C4A 0.72025 (13) 0.3083 (2) 0.35237 (13) 0.0139 (5)
C5A 0.76423 (13) 0.2910 (2) 0.41332 (13) 0.0150 (5)
H5A 0.7496 0.2358 0.4487 0.018*
C6A 0.82952 (14) 0.3543 (2) 0.42245 (14) 0.0199 (5)
H6A 0.8596 0.3423 0.4640 0.024*
C7A 0.85112 (15) 0.4353 (2) 0.37098 (15) 0.0233 (6)
H7A 0.8964 0.4776 0.3768 0.028*
C8A 0.80630 (14) 0.4541 (2) 0.31124 (16) 0.0227 (6)
H8A 0.8204 0.5105 0.2765 0.027*
C9A 0.74113 (14) 0.3912 (2) 0.30178 (14) 0.0182 (5)
H9A 0.7106 0.4047 0.2607 0.022*
C10A 0.64818 (14) 0.1276 (2) 0.35658 (13) 0.0157 (5)
H10A 0.5984 0.1001 0.3624 0.019*
C11A 0.70180 (13) 0.0433 (2) 0.36266 (12) 0.0136 (5)
C12A 0.78275 (13) 0.0582 (2) 0.34518 (13) 0.0143 (5)
C13A 0.83799 (13) 0.0207 (2) 0.39292 (13) 0.0159 (5)
H13A 0.8239 −0.0154 0.4369 0.019*
C14A 0.91359 (14) 0.0353 (2) 0.37700 (15) 0.0184 (5)
H14A 0.9505 0.0104 0.4105 0.022*
C15A 0.93517 (15) 0.0860 (2) 0.31277 (14) 0.0209 (6)
H15A 0.9868 0.0967 0.3021 0.025*
C16A 0.88076 (14) 0.1212 (2) 0.26390 (14) 0.0209 (6)
H16A 0.8952 0.1549 0.2193 0.025*
C17A 0.80555 (14) 0.1074 (2) 0.27994 (13) 0.0166 (5)
H17A 0.7689 0.1317 0.2460 0.020*
C18A 0.59638 (14) −0.2147 (2) 0.42114 (13) 0.0155 (5)
C19A 0.53579 (14) −0.2820 (2) 0.43916 (14) 0.0196 (5)
H19A 0.4864 −0.2514 0.4402 0.024*
C20A 0.55064 (15) −0.3974 (2) 0.45574 (14) 0.0212 (6)
H20A 0.5102 −0.4469 0.4685 0.025*
C21A 0.62240 (15) −0.4420 (2) 0.45425 (14) 0.0221 (6)
H21A 0.6302 −0.5212 0.4661 0.027*
C22A 0.68384 (15) −0.3727 (2) 0.43561 (14) 0.0215 (6)
H22A 0.7335 −0.4024 0.4346 0.026*
C23A 0.66814 (14) −0.2591 (2) 0.41882 (13) 0.0159 (5)
B1A 0.67343 (15) −0.0740 (2) 0.38806 (15) 0.0149 (5)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
O1B 0.0139 (8) 0.0119 (8) 0.0206 (9) 0.0005 (7) 0.0001 (7) 0.0023 (7)
O2B 0.0137 (8) 0.0144 (8) 0.0194 (9) −0.0010 (6) −0.0018 (7) 0.0016 (7)
N1B 0.0115 (10) 0.0142 (9) 0.0218 (11) 0.0004 (8) 0.0030 (8) 0.0028 (8)
C1B 0.0183 (13) 0.0203 (12) 0.0245 (15) −0.0017 (10) −0.0016 (11) −0.0009 (11)
C2B 0.0194 (14) 0.0215 (13) 0.0206 (13) −0.0021 (11) 0.0031 (11) 0.0012 (10)
C3B 0.0142 (13) 0.0135 (11) 0.0205 (13) −0.0017 (10) 0.0030 (10) 0.0013 (10)
C4B 0.0115 (12) 0.0112 (10) 0.0213 (13) −0.0010 (9) −0.0012 (10) −0.0023 (10)
C5B 0.0187 (13) 0.0162 (12) 0.0218 (14) −0.0021 (10) −0.0029 (10) 0.0006 (10)
C6B 0.0174 (13) 0.0157 (12) 0.0360 (16) 0.0007 (10) −0.0082 (12) 0.0023 (11)
C7B 0.0144 (13) 0.0196 (12) 0.0487 (19) 0.0027 (11) 0.0015 (13) −0.0046 (12)
C8B 0.0196 (14) 0.0191 (13) 0.0328 (16) −0.0020 (11) 0.0108 (11) −0.0065 (11)
C9B 0.0173 (13) 0.0168 (12) 0.0232 (13) −0.0015 (10) 0.0015 (10) −0.0014 (10)
C10B 0.0132 (12) 0.0174 (11) 0.0147 (11) 0.0022 (9) 0.0007 (9) 0.0013 (10)
C11B 0.0146 (12) 0.0169 (11) 0.0152 (12) 0.0014 (10) 0.0027 (10) 0.0006 (10)
C12B 0.0133 (12) 0.0120 (11) 0.0173 (12) 0.0018 (9) 0.0002 (10) −0.0012 (10)
C13B 0.0182 (13) 0.0161 (12) 0.0172 (13) 0.0000 (10) 0.0021 (10) −0.0014 (10)
C14B 0.0217 (14) 0.0217 (13) 0.0195 (13) 0.0023 (11) −0.0053 (11) 0.0007 (11)
C15B 0.0143 (13) 0.0208 (12) 0.0281 (15) 0.0023 (10) −0.0057 (11) −0.0022 (11)
C16B 0.0144 (12) 0.0178 (12) 0.0244 (14) −0.0007 (10) 0.0032 (10) −0.0005 (10)
C17B 0.0177 (12) 0.0163 (11) 0.0169 (12) 0.0007 (10) 0.0008 (10) 0.0008 (10)
C18B 0.0171 (12) 0.0124 (11) 0.0124 (11) −0.0024 (10) 0.0031 (9) 0.0000 (9)
C19B 0.0140 (13) 0.0202 (13) 0.0191 (13) 0.0031 (10) 0.0011 (10) 0.0001 (10)
C20B 0.0236 (14) 0.0186 (12) 0.0171 (13) 0.0061 (11) 0.0014 (11) 0.0014 (10)
C21B 0.0277 (14) 0.0125 (11) 0.0172 (13) 0.0003 (11) 0.0044 (11) −0.0002 (10)
C22B 0.0217 (13) 0.0174 (11) 0.0147 (12) −0.0032 (10) 0.0000 (10) −0.0025 (9)
C23B 0.0158 (12) 0.0167 (11) 0.0127 (11) 0.0028 (10) −0.0025 (9) −0.0023 (10)
B1B 0.0128 (13) 0.0191 (13) 0.0129 (13) −0.0004 (11) 0.0016 (11) −0.0006 (11)
O1A 0.0134 (9) 0.0138 (8) 0.0258 (10) −0.0012 (7) 0.0003 (7) 0.0027 (7)
O2A 0.0139 (9) 0.0146 (8) 0.0237 (10) −0.0005 (7) 0.0028 (7) 0.0023 (7)
N1A 0.0116 (10) 0.0147 (10) 0.0220 (11) 0.0002 (8) −0.0036 (8) 0.0030 (8)
C1A 0.0161 (13) 0.0221 (13) 0.0304 (15) 0.0042 (11) 0.0001 (11) 0.0005 (12)
C2A 0.0128 (12) 0.0150 (11) 0.0251 (14) 0.0015 (10) −0.0032 (10) 0.0033 (10)
C3A 0.0154 (14) 0.0273 (14) 0.0254 (14) 0.0027 (11) −0.0061 (11) 0.0047 (11)
C4A 0.0121 (12) 0.0119 (11) 0.0175 (12) 0.0009 (9) 0.0005 (10) −0.0018 (9)
C5A 0.0157 (12) 0.0142 (10) 0.0151 (12) 0.0010 (9) 0.0010 (10) −0.0004 (9)
C6A 0.0160 (12) 0.0214 (12) 0.0223 (14) 0.0021 (10) −0.0038 (10) −0.0035 (11)
C7A 0.0155 (13) 0.0179 (12) 0.0366 (16) −0.0054 (11) 0.0001 (12) −0.0006 (11)
C8A 0.0198 (14) 0.0182 (12) 0.0300 (15) −0.0014 (11) 0.0034 (11) 0.0066 (11)
C9A 0.0175 (13) 0.0173 (12) 0.0198 (13) 0.0018 (10) −0.0009 (10) 0.0033 (10)
C10A 0.0129 (12) 0.0171 (12) 0.0172 (12) −0.0036 (10) −0.0012 (9) 0.0010 (10)
C11A 0.0125 (12) 0.0146 (11) 0.0138 (12) 0.0000 (9) −0.0014 (9) 0.0005 (9)
C12A 0.0143 (12) 0.0123 (11) 0.0164 (12) −0.0009 (9) 0.0007 (10) −0.0042 (10)
C13A 0.0162 (12) 0.0143 (11) 0.0170 (13) 0.0002 (10) 0.0011 (10) 0.0002 (10)
C14A 0.0140 (12) 0.0166 (12) 0.0247 (14) 0.0000 (10) −0.0032 (10) −0.0033 (10)
C15A 0.0152 (13) 0.0220 (12) 0.0255 (14) −0.0017 (10) 0.0056 (11) −0.0028 (11)
C16A 0.0229 (14) 0.0215 (13) 0.0182 (13) −0.0034 (11) 0.0064 (11) 0.0000 (11)
C17A 0.0165 (12) 0.0167 (12) 0.0166 (12) −0.0003 (10) −0.0014 (10) −0.0008 (10)
C18A 0.0185 (13) 0.0154 (11) 0.0127 (12) −0.0018 (10) −0.0012 (9) 0.0004 (9)
C19A 0.0151 (13) 0.0228 (13) 0.0211 (13) −0.0022 (11) −0.0002 (10) 0.0028 (11)
C20A 0.0236 (14) 0.0209 (13) 0.0190 (13) −0.0103 (11) −0.0021 (11) 0.0036 (10)
C21A 0.0294 (15) 0.0155 (12) 0.0215 (13) −0.0025 (11) −0.0005 (11) 0.0047 (10)
C22A 0.0216 (14) 0.0191 (12) 0.0237 (14) 0.0030 (11) −0.0002 (11) 0.0019 (11)
C23A 0.0137 (12) 0.0178 (12) 0.0164 (12) −0.0037 (10) 0.0009 (10) 0.0009 (10)
B1A 0.0126 (13) 0.0177 (13) 0.0143 (13) −0.0006 (11) 0.0002 (11) −0.0026 (11)

Geometric parameters (Å, º)

O1B—C18B 1.385 (3) O1A—C18A 1.382 (3)
O1B—B1B 1.399 (3) O1A—B1A 1.402 (3)
O2B—C23B 1.385 (3) O2A—C23A 1.384 (3)
O2B—B1B 1.398 (3) O2A—B1A 1.396 (3)
N1B—C3B 1.488 (3) N1A—C2A 1.487 (3)
N1B—C4B 1.425 (3) N1A—C4A 1.421 (3)
N1B—C10B 1.365 (3) N1A—C10A 1.365 (3)
C1B—H1BA 0.9800 C1A—H1AA 0.9800
C1B—H1BB 0.9800 C1A—H1AB 0.9800
C1B—H1BC 0.9800 C1A—H1AC 0.9800
C1B—C3B 1.523 (4) C1A—C2A 1.523 (4)
C2B—H2BA 0.9800 C2A—H2A 1.0000
C2B—H2BB 0.9800 C2A—C3A 1.515 (4)
C2B—H2BC 0.9800 C3A—H3AA 0.9800
C2B—C3B 1.520 (3) C3A—H3AB 0.9800
C3B—H3B 1.0000 C3A—H3AC 0.9800
C4B—C5B 1.389 (3) C4A—C5A 1.390 (3)
C4B—C9B 1.385 (4) C4A—C9A 1.390 (3)
C5B—H5B 0.9500 C5A—H5A 0.9500
C5B—C6B 1.382 (3) C5A—C6A 1.386 (3)
C6B—H6B 0.9500 C6A—H6A 0.9500
C6B—C7B 1.379 (4) C6A—C7A 1.390 (4)
C7B—H7B 0.9500 C7A—H7A 0.9500
C7B—C8B 1.382 (4) C7A—C8A 1.383 (4)
C8B—H8B 0.9500 C8A—H8A 0.9500
C8B—C9B 1.387 (4) C8A—C9A 1.382 (4)
C9B—H9B 0.9500 C9A—H9A 0.9500
C10B—H10B 0.9500 C10A—H10A 0.9500
C10B—C11B 1.369 (3) C10A—C11A 1.370 (3)
C11B—C12B 1.489 (3) C11A—C12A 1.491 (3)
C11B—B1B 1.521 (4) C11A—B1A 1.519 (3)
C12B—C13B 1.399 (3) C12A—C13A 1.394 (3)
C12B—C17B 1.398 (3) C12A—C17A 1.397 (3)
C13B—H13B 0.9500 C13A—H13A 0.9500
C13B—C14B 1.389 (4) C13A—C14A 1.392 (3)
C14B—H14B 0.9500 C14A—H14A 0.9500
C14B—C15B 1.387 (4) C14A—C15A 1.381 (4)
C15B—H15B 0.9500 C15A—H15A 0.9500
C15B—C16B 1.385 (4) C15A—C16A 1.389 (4)
C16B—H16B 0.9500 C16A—H16A 0.9500
C16B—C17B 1.386 (3) C16A—C17A 1.385 (3)
C17B—H17B 0.9500 C17A—H17A 0.9500
C18B—C19B 1.374 (3) C18A—C19A 1.372 (3)
C18B—C23B 1.382 (3) C18A—C23A 1.381 (3)
C19B—H19B 0.9500 C19A—H19A 0.9500
C19B—C20B 1.401 (3) C20A—H20A 0.9500
C20B—H20B 0.9500 C20A—C21A 1.381 (4)
C20B—C21B 1.391 (4) C21A—H21A 0.9500
C21B—H21B 0.9500 C21A—C22A 1.401 (4)
C21B—C22B 1.393 (4) C22A—H22A 0.9500
C22B—H22B 0.9500 C22A—C23A 1.375 (3)
C22B—C23B 1.374 (3)
C18B—O1B—B1B 105.28 (18) C18A—O1A—B1A 105.46 (18)
C23B—O2B—B1B 105.43 (18) C23A—O2A—B1A 105.50 (18)
C4B—N1B—C3B 118.34 (18) C4A—N1A—C2A 117.83 (18)
C10B—N1B—C3B 119.02 (19) C10A—N1A—C2A 118.9 (2)
C10B—N1B—C4B 122.6 (2) C10A—N1A—C4A 123.2 (2)
H1BA—C1B—H1BB 109.5 H1AA—C1A—H1AB 109.5
H1BA—C1B—H1BC 109.5 H1AA—C1A—H1AC 109.5
H1BB—C1B—H1BC 109.5 H1AB—C1A—H1AC 109.5
C3B—C1B—H1BA 109.5 C2A—C1A—H1AA 109.5
C3B—C1B—H1BB 109.5 C2A—C1A—H1AB 109.5
C3B—C1B—H1BC 109.5 C2A—C1A—H1AC 109.5
H2BA—C2B—H2BB 109.5 N1A—C2A—C1A 111.9 (2)
H2BA—C2B—H2BC 109.5 N1A—C2A—H2A 107.0
H2BB—C2B—H2BC 109.5 N1A—C2A—C3A 111.5 (2)
C3B—C2B—H2BA 109.5 C1A—C2A—H2A 107.0
C3B—C2B—H2BB 109.5 C3A—C2A—C1A 112.1 (2)
C3B—C2B—H2BC 109.5 C3A—C2A—H2A 107.0
N1B—C3B—C1B 111.5 (2) C2A—C3A—H3AA 109.5
N1B—C3B—C2B 111.6 (2) C2A—C3A—H3AB 109.5
N1B—C3B—H3B 107.2 C2A—C3A—H3AC 109.5
C1B—C3B—H3B 107.2 H3AA—C3A—H3AB 109.5
C2B—C3B—C1B 111.9 (2) H3AA—C3A—H3AC 109.5
C2B—C3B—H3B 107.2 H3AB—C3A—H3AC 109.5
C5B—C4B—N1B 120.3 (2) C5A—C4A—N1A 119.6 (2)
C9B—C4B—N1B 119.9 (2) C5A—C4A—C9A 119.7 (2)
C9B—C4B—C5B 119.8 (2) C9A—C4A—N1A 120.6 (2)
C4B—C5B—H5B 120.0 C4A—C5A—H5A 120.1
C6B—C5B—C4B 120.1 (2) C6A—C5A—C4A 119.9 (2)
C6B—C5B—H5B 120.0 C6A—C5A—H5A 120.1
C5B—C6B—H6B 119.8 C5A—C6A—H6A 119.9
C7B—C6B—C5B 120.3 (2) C5A—C6A—C7A 120.3 (2)
C7B—C6B—H6B 119.8 C7A—C6A—H6A 119.9
C6B—C7B—H7B 120.2 C6A—C7A—H7A 120.2
C6B—C7B—C8B 119.7 (2) C8A—C7A—C6A 119.6 (2)
C8B—C7B—H7B 120.2 C8A—C7A—H7A 120.2
C7B—C8B—H8B 119.7 C7A—C8A—H8A 119.8
C7B—C8B—C9B 120.5 (2) C9A—C8A—C7A 120.4 (2)
C9B—C8B—H8B 119.7 C9A—C8A—H8A 119.8
C4B—C9B—C8B 119.6 (2) C4A—C9A—H9A 120.0
C4B—C9B—H9B 120.2 C8A—C9A—C4A 120.1 (2)
C8B—C9B—H9B 120.2 C8A—C9A—H9A 120.0
N1B—C10B—H10B 114.4 N1A—C10A—H10A 114.0
N1B—C10B—C11B 131.2 (2) N1A—C10A—C11A 131.9 (2)
C11B—C10B—H10B 114.4 C11A—C10A—H10A 114.0
C10B—C11B—C12B 125.0 (2) C10A—C11A—C12A 125.3 (2)
C10B—C11B—B1B 115.2 (2) C10A—C11A—B1A 115.1 (2)
C12B—C11B—B1B 119.6 (2) C12A—C11A—B1A 119.5 (2)
C13B—C12B—C11B 120.9 (2) C13A—C12A—C11A 120.8 (2)
C17B—C12B—C11B 121.1 (2) C13A—C12A—C17A 118.0 (2)
C17B—C12B—C13B 118.0 (2) C17A—C12A—C11A 121.2 (2)
C12B—C13B—H13B 119.6 C12A—C13A—H13A 119.5
C14B—C13B—C12B 120.9 (2) C14A—C13A—C12A 120.9 (2)
C14B—C13B—H13B 119.6 C14A—C13A—H13A 119.5
C13B—C14B—H14B 119.9 C13A—C14A—H14A 119.8
C15B—C14B—C13B 120.3 (2) C15A—C14A—C13A 120.3 (2)
C15B—C14B—H14B 119.9 C15A—C14A—H14A 119.8
C14B—C15B—H15B 120.3 C14A—C15A—H15A 120.3
C16B—C15B—C14B 119.4 (2) C14A—C15A—C16A 119.4 (2)
C16B—C15B—H15B 120.3 C16A—C15A—H15A 120.3
C15B—C16B—H16B 119.7 C15A—C16A—H16A 119.9
C15B—C16B—C17B 120.5 (2) C17A—C16A—C15A 120.3 (2)
C17B—C16B—H16B 119.7 C17A—C16A—H16A 119.9
C12B—C17B—H17B 119.5 C12A—C17A—H17A 119.5
C16B—C17B—C12B 120.9 (2) C16A—C17A—C12A 121.0 (2)
C16B—C17B—H17B 119.5 C16A—C17A—H17A 119.5
C19B—C18B—O1B 127.9 (2) C19A—C18A—O1A 128.7 (2)
C19B—C18B—C23B 122.6 (2) C19A—C18A—C23A 122.0 (2)
C23B—C18B—O1B 109.4 (2) C23A—C18A—O1A 109.3 (2)
C18B—C19B—H19B 122.0 C18A—C19A—H19A 121.8
C18B—C19B—C20B 115.9 (2) C18A—C19A—C20A 116.4 (2)
C20B—C19B—H19B 122.0 C20A—C19A—H19A 121.8
C19B—C20B—H20B 119.3 C19A—C20A—H20A 119.0
C21B—C20B—C19B 121.4 (2) C21A—C20A—C19A 121.9 (2)
C21B—C20B—H20B 119.3 C21A—C20A—H20A 119.0
C20B—C21B—H21B 119.2 C20A—C21A—H21A 119.4
C20B—C21B—C22B 121.6 (2) C20A—C21A—C22A 121.3 (2)
C22B—C21B—H21B 119.2 C22A—C21A—H21A 119.4
C21B—C22B—H22B 121.8 C21A—C22A—H22A 122.0
C23B—C22B—C21B 116.4 (2) C23A—C22A—C21A 116.1 (2)
C23B—C22B—H22B 121.8 C23A—C22A—H22A 122.0
C18B—C23B—O2B 109.24 (19) C18A—C23A—O2A 109.3 (2)
C22B—C23B—O2B 128.6 (2) C22A—C23A—O2A 128.3 (2)
C22B—C23B—C18B 122.1 (2) C22A—C23A—C18A 122.4 (2)
O1B—B1B—C11B 124.4 (2) O1A—B1A—C11A 124.2 (2)
O2B—B1B—O1B 110.6 (2) O2A—B1A—O1A 110.4 (2)
O2B—B1B—C11B 125.0 (2) O2A—B1A—C11A 125.5 (2)
O1B—C18B—C19B—C20B −176.7 (2) O1A—C18A—C19A—C20A −179.5 (2)
O1B—C18B—C23B—O2B 0.0 (3) O1A—C18A—C23A—O2A −0.5 (3)
O1B—C18B—C23B—C22B 177.9 (2) O1A—C18A—C23A—C22A 178.9 (2)
N1B—C4B—C5B—C6B 179.9 (2) N1A—C4A—C5A—C6A −179.4 (2)
N1B—C4B—C9B—C8B −179.9 (2) N1A—C4A—C9A—C8A 179.4 (2)
N1B—C10B—C11B—C12B −9.7 (4) N1A—C10A—C11A—C12A −9.7 (4)
N1B—C10B—C11B—B1B 175.5 (2) N1A—C10A—C11A—B1A 171.6 (2)
C3B—N1B—C4B—C5B −45.6 (3) C2A—N1A—C4A—C5A 132.7 (2)
C3B—N1B—C4B—C9B 132.5 (2) C2A—N1A—C4A—C9A −45.1 (3)
C3B—N1B—C10B—C11B 159.6 (3) C2A—N1A—C10A—C11A 165.3 (2)
C4B—N1B—C3B—C1B −123.7 (2) C4A—N1A—C2A—C1A −120.9 (2)
C4B—N1B—C3B—C2B 110.3 (2) C4A—N1A—C2A—C3A 112.7 (2)
C4B—N1B—C10B—C11B −19.1 (4) C4A—N1A—C10A—C11A −17.5 (4)
C4B—C5B—C6B—C7B −0.4 (4) C4A—C5A—C6A—C7A 0.1 (4)
C5B—C4B—C9B—C8B −1.8 (4) C5A—C4A—C9A—C8A 1.6 (4)
C5B—C6B—C7B—C8B −1.0 (4) C5A—C6A—C7A—C8A 1.3 (4)
C6B—C7B—C8B—C9B 1.0 (4) C6A—C7A—C8A—C9A −1.3 (4)
C7B—C8B—C9B—C4B 0.5 (4) C7A—C8A—C9A—C4A −0.1 (4)
C9B—C4B—C5B—C6B 1.8 (4) C9A—C4A—C5A—C6A −1.6 (4)
C10B—N1B—C3B—C1B 57.5 (3) C10A—N1A—C2A—C1A 56.4 (3)
C10B—N1B—C3B—C2B −68.4 (3) C10A—N1A—C2A—C3A −69.9 (3)
C10B—N1B—C4B—C5B 133.1 (2) C10A—N1A—C4A—C5A −44.5 (3)
C10B—N1B—C4B—C9B −48.8 (3) C10A—N1A—C4A—C9A 137.6 (2)
C10B—C11B—C12B—C13B −50.5 (3) C10A—C11A—C12A—C13A 132.2 (3)
C10B—C11B—C12B—C17B 131.9 (3) C10A—C11A—C12A—C17A −49.3 (3)
C10B—C11B—B1B—O1B −0.5 (4) C10A—C11A—B1A—O1A 1.7 (4)
C10B—C11B—B1B—O2B 176.9 (2) C10A—C11A—B1A—O2A −179.8 (2)
C11B—C12B—C13B—C14B −179.0 (2) C11A—C12A—C13A—C14A −179.5 (2)
C11B—C12B—C17B—C16B 179.3 (2) C11A—C12A—C17A—C16A 179.9 (2)
C12B—C11B—B1B—O1B −175.6 (2) C12A—C11A—B1A—O1A −177.2 (2)
C12B—C11B—B1B—O2B 1.7 (4) C12A—C11A—B1A—O2A 1.4 (4)
C12B—C13B—C14B—C15B 0.2 (4) C12A—C13A—C14A—C15A −1.0 (4)
C13B—C12B—C17B—C16B 1.6 (3) C13A—C12A—C17A—C16A −1.6 (3)
C13B—C14B—C15B—C16B 0.8 (4) C13A—C14A—C15A—C16A −0.6 (4)
C14B—C15B—C16B—C17B −0.5 (4) C14A—C15A—C16A—C17A 1.1 (4)
C15B—C16B—C17B—C12B −0.6 (4) C15A—C16A—C17A—C12A 0.1 (4)
C17B—C12B—C13B—C14B −1.3 (3) C17A—C12A—C13A—C14A 2.0 (3)
C18B—O1B—B1B—O2B 1.1 (3) C18A—O1A—B1A—O2A −1.2 (3)
C18B—O1B—B1B—C11B 178.7 (2) C18A—O1A—B1A—C11A 177.5 (2)
C18B—C19B—C20B—C21B −0.9 (4) C18A—C19A—C20A—C21A 0.1 (4)
C19B—C18B—C23B—O2B −177.8 (2) C19A—C18A—C23A—O2A 179.4 (2)
C19B—C18B—C23B—C22B 0.1 (4) C19A—C18A—C23A—C22A −1.2 (4)
C19B—C20B—C21B—C22B 0.3 (4) C19A—C20A—C21A—C22A −0.2 (4)
C20B—C21B—C22B—C23B 0.5 (4) C20A—C21A—C22A—C23A −0.3 (4)
C21B—C22B—C23B—O2B 176.8 (2) C21A—C22A—C23A—O2A −179.7 (2)
C21B—C22B—C23B—C18B −0.7 (4) C21A—C22A—C23A—C18A 1.0 (4)
C23B—O2B—B1B—O1B −1.1 (3) C23A—O2A—B1A—O1A 1.0 (3)
C23B—O2B—B1B—C11B −178.7 (2) C23A—O2A—B1A—C11A −177.8 (2)
C23B—C18B—C19B—C20B 0.7 (4) C23A—C18A—C19A—C20A 0.6 (4)
B1B—O1B—C18B—C19B 177.0 (2) B1A—O1A—C18A—C19A −178.8 (3)
B1B—O1B—C18B—C23B −0.6 (3) B1A—O1A—C18A—C23A 1.0 (3)
B1B—O2B—C23B—C18B 0.7 (3) B1A—O2A—C23A—C18A −0.3 (3)
B1B—O2B—C23B—C22B −177.1 (2) B1A—O2A—C23A—C22A −179.7 (3)
B1B—C11B—C12B—C13B 124.1 (3) B1A—C11A—C12A—C13A −49.1 (3)
B1B—C11B—C12B—C17B −53.5 (3) B1A—C11A—C12A—C17A 129.4 (2)

Funding Statement

This work was funded by Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung grant .

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989020005289/lh5953sup1.cif

e-76-00710-sup1.cif (1.8MB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989020005289/lh5953Isup2.hkl

e-76-00710-Isup2.hkl (697.1KB, hkl)

Supporting information file. DOI: 10.1107/S2056989020005289/lh5953Isup3.cml

CCDC reference: 1997061

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


Articles from Acta Crystallographica Section E: Crystallographic Communications are provided here courtesy of International Union of Crystallography

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