Libo
Xiang
a,
Junyi
Wang
b,
Julius
Bolch
a,
Alexander
Matler
a and
Qing
Ye
*a
aInstitute for Inorganic Chemistry and Institute for Sustainable Chemistry & Catalysis with Boron, Julius-Maximilians-Universität Würzburg, Am Hubland, 97074 Würzburg, Germany. E-mail: qing.ye@uni-wuerzburg.de
bDepartment of Chemistry and Biochemistry, Baylor University, Waco, Texas 76798, USA
First published on 9th December 2025
The reactions of the carborane-fused borirane (B10H10C2)BN(SiMe3)2 (1) with isocyanides proceed, for the first time, with a clearly defined sequence of coordination and insertion steps. The first equivalent of isocyanide undergoes selective 1,1-insertion into the borirane unit, affording a four-membered borete ring (2). A second equivalent initially coordinates reversibly to the boron center. Subsequent heating promotes its full insertion to generate the α-diimine product (3), which can reversibly capture an additional isocyanide molecule. Variable-temperature NMR studies reveal that 3 exhibits a remarkably higher isocyanide affinity than 2.
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| Fig. 1 Boriranes (I), carborane-fused boriranes (III), and their Lewis base (LB) adducts (II and IV). | ||
In recent years, increasing ring strain via annulation has emerged as a strategy to unlock the reaction chemistry of boriranes. A notable example is the fusion of a borirane ring with an o-carborane cage through a shared carbon–carbon bond (III).3 In addition to boosted ring strain energy, the o-carborane-fused boriranes exhibit boosted Lewis acidity due to the strong electron withdrawing nature of the o-carborane framework.4 This enables a stronger interaction between the boron center of the borirane and Lewis bases (IV), which in turn promotes ring-opening,1,5 rearrangement,6 and particularly ring enlargement reactions.3b,5 The difference in the reactivity of the o-carborane-fused aminoborirane 1 (Scheme 1) and its benzo-fused counterpart toward THF clearly highlights the impact of o-carborane fusing on the reactivity.3a,6 While 1 readily coordinates to THF and subsequently undergoes a ring-opening rearrangement to afford the first free carboranyl iminoborane, its benzo-fused counterpart is not Lewis acidic enough to bind THF, thereby preventing further reactions.6
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| Scheme 1 Reaction of 1 with 1.0 equiv. RNC (R: Xyl = 2,6-MeC6H4; Dipp = 2,6-iPr2C6H4; Mes* = 2,4,6-tBu3C6H2). | ||
The ring enlargement reactions reported for carborane-fused boriranes include: insertion of a sulfur atom into the B–CCb bond of a carbene-stabilized borirane;5a σ-bond insertion, for example, treatment of a carborane-fused borirane with BBr3, GeCl2 or GaCl3 leads to the insertion of the E–X σ-bond into the strained ring, with the E–X bond being converted into a dative interaction; 1,2-insertion of unsaturated polar bonds, a reaction mode that has demonstrated broad substrate scope, including alkyl ketones,5 aldehydes,3b,5b nitriles,3b,c,5b CO2,5b as well as Bestmann ylide;7 and 1,4-insertion of benzophenone, which involves dearomatization of one of the phenyl rings.3b
Indeed, the high versatility of the ring enlargement reactions highlights the potential of carborane-fused boriranes as modular building blocks for constructing novel carborane-based functional molecules.8 Isocyanides exhibit rich reactivity.9 In particular, their insertion chemistry makes them valuable C1 synthons and offers great potential in skeletal editing.10,11 However, the reactivity between boriranes and isocyanides has not been reported thus far.
Herein, we exploit a carborane-fused borirane of type III, which features both boosted ring strain energy from annulation and a non-coordinated boron center, to realize for the first time the reaction of borirane with isocyanides, enabling the modular construction of carborane-fused boretes and borirane-derived α-diimines.
Interestingly, even the addition of one more equivalent of the corresponding isocyanide to 2a or 2b at room temperature does not result in a second insertion. Instead, the isocyanide coordinates to the boron center of 2a/b to afford adduct 3a/b. However, since this coordination is rather weak, a dissociation equilibrium is present in solution at room temperature (Scheme 2), as evidenced by the only slight upfield shift of the 11B NMR signals: 2aδB 41.9 → 36.3, 2b, δB 42.5 → 36.6. Moreover, storing the pentane solution at −30 °C for 2 hours affords single crystals of 3a/b suitable for X-ray diffraction analysis. Redissolving these crystals in pentane affords a solution displaying the same NMR signals as the aforementioned reaction mixture. In the solid-state structure, the second isocyanide unambiguously coordinates to the B1 center, with a B1–C4 distance (3a: 1.6437(16) Å and 3b: 1.656(2) Å) expected for a C → B dative bond (Fig. 3). In addition, the increased coordination number at B1 leads to elongation of the surrounding bonds. In contrast, treatment of 2c with 1.0 equivalent of Mes*NC does not cause any change in the 11B NMR spectrum. It is nevertheless not surprising that 2c cannot further react with Mes*NC due to the steric hindrance.
On the NMR timescale, a rapid dynamic equilibrium process results in an averaged chemical shift that reflects the distribution of the species in equilibrium. Therefore, to gain further insight into the dissociation equilibrium of isocyanide, variable-temperature NMR (VT-NMR) experiments were conducted on 3a. As depicted in Fig. 4, as the temperature decreased, the 11B NMR signal of atom B1 gradually shifted upfield until it was obscured by the high-field resonances of the carborane cage. This observation is consistent with the expected enthalpy-driven formation of the adduct at lower temperatures. To further estimate the thermodynamic parameters of this equilibrium, the 11B-NMR signal of atom B1 in 2a (δB 41.9) as well as that in 3a was required. However, since the B1 signal of 3a overlapped with the signals of the carborane cage, its value (δB −4.3) could only be obtained through theoretical calculations at the M06L/pcSseg-2//PBEh-3c/def2-mSVP level of theory. To verify the reliability of this computational approach, the 11B-NMR signal of 2a was calculated using the same method, which showed excellent agreement with the experimental value (theo. δB: 40.2 vs. exp. δB: 41.9). Based on the 11B-NMR signals of atom B1 in 2a (δB 41.9) and 3a (δB −4.3), fitting of the variable temperature data to the Van't Hoff equation affords the enthalpy (ΔH° = −38.0 ± 0.8 kJ mol−1) and entropy (ΔS° = −146.1 ± 3.2 J mol−1 K−1) (R2 = 0.99). See the SI for details. From these values, the Gibbs free energy at 298 K was estimated to be ΔG° = 5.5 kJ mol−1.
Furthermore, 3a and 3b were found to undergo a slow transformation at room temperature, requiring about 8 days to form a new three-coordinate boron-containing species showing a 11B-NMR resonance at δB 46.7 (3a′) and δB 45.5 (3b′), respectively, accompanied by a distinct color change from yellow to reddish-brown. Heating the sample to 80 °C significantly accelerated this process, affording the same product within only 4 hours. In contrast to 3a/b, in which the isocyanide coordinated to boron readily dissociates so that only the molecular signals of 2a/b can be detected by high-resolution mass spectrometry (HRMS), the spectra of 3a′/3b′ clearly display molecular signals corresponding to 2a/b with an extra equivalent of the respective isocyanide. This suggests that the second isocyanide becomes firmly incorporated through insertion (Scheme 3). However, all attempts to grow single crystals of 3a′/3b′ were unsuccessful. Therefore, we decided to further convert them into Lewis base adducts, which facilitate crystallization. To this end, 3a′/3b′ was further treated with one more equivalent of the respective isocyanide at room temperature. The tricoordinate boron signal disappeared rapidly, indicating that the isocyanide indeed coordinated to the tricoordinate boron center, affording 4a/b (Scheme 3). This was further confirmed by single crystal characterization (Fig. 5).
In sharp contrast to 2a/b, which mainly exist in a non-coordinated form in the presence of one equivalent of isocyanide at room temperature, 3a′/3b′ readily form adducts under the same conditions, with the equilibrium (Scheme 4) shifting gradually toward dissociation of the adducts upon heating. As shown in Fig. 6, VT-NMR data of 4a show that upon increasing the temperature, the signal corresponding to the three-coordinate boron species appears and gradually shifts downfield, reaching 45.7 ppm at 100 °C. This value is nearly identical to that of 3a′ (46.7 ppm), indicating that 4a exists predominantly in the non-coordinated form in solution at 100 °C. To quantify the thermodynamic parameters of this equilibrium, the 11B resonance of the four-coordinate species in 4a was obtained by DFT calculations (δB −8.2), since this signal is obscured within the resonance region of the carborane cage and thus difficult to identify experimentally. To ensure the reliability of the calculated NMR shifts, we also computed the 11B chemical shift of 3a′, which showed agreement with the experimental value (theo. δB 41.5 vs. exp. δB 46.7). Van't Hoff fitting of the data gave the enthalpy (ΔH° = −45.1 ± 2.9 kJ mol−1) and entropy (ΔS° = −153.1 ± 8.3 J mol−1 K−1) (R2 = 0.98). At 298 K, the corresponding Gibbs free energy is ΔG° = 0.5 kJ mol−1. See the SI for details. Remarkably, 3a′ exhibits higher isocyanide affinity than 2a (3a′: −45.1 ± 2.9 kJ mol−1vs. 2a: –38.0 ± 0.8 kJ mol−1). This may be attributed to the presence of additional electron-withdrawing imino groups near the three-coordinate boron center in 3a′. Furthermore, likely due to steric hindrance, further heating of 4a/b did not promote insertion of the third equivalent of isocyanide. No detectable spectral changes occurred even after prolonged heating at 110 °C in toluene-d8 for one week.
2a (light green block crystals, 96 mg, 83%): 1H NMR (C6D6): δ = 6.90 to 6.84 (m, 3H, CH of Xyl), 3.64 to 2.18 (m, 10H, BH), 2.01 (s, 6H, CMe3), 0.23 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 6.91 to 6.85 (m, 3H, CH of Xyl), 3.04 (s, 1H, BH), 3.00 (s, 1H, BH), 2.88 (s, 2H, BH), 2.75 (s, 2H, BH), 2.58 (s, 2H, BH), 2.20 (s, 2H, BH), 2.01 (s, 6H, CMe3), 0.23 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 41.9 (s, BN(SiMe3)2), 2.5 (d, J = 152.3 Hz, BCb), −0.9 (d, J = 150.1 Hz, BCb), −4.5 (d, J = 150.1 Hz, BCb), −8.6 to −11.1 (m, BCb); 11B{1H} NMR (C6D6): δ = 42.0 (s, BN(SiMe3)2), 2.5 (s, BCb), −1.0 (s, BCb), −4.5 (s, BCb), −9.2 (s, BCb), −10.6 (s, BCb); 13C{1H} NMR (C6D6): δ = 146.0 (C of Xyl), 125.1 (C of Xyl), 124.8 (C of Xyl), 89.1 (C of Cb), 18.3 (CMe3), 3.4 (SiMe3); HRMS (m/z): [M + H2O] calcd for C17H39N2B11Si2O, 464.3625; found 464.3616.
2b (light green block crystals, 93 mg, 74%): 1H NMR (C6D6): δ = 7.07 (m, 3H, CH of Dipp), 2.76 (sep, J = 6.8 Hz, 2H, CH of iPr), 1.31 (d, J = 6.9 Hz, 6H, Me of iPr), 1.11 (d, J = 6.7 Hz, 6H, Me of iPr), 0.25 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 7.07 (m, 3H, CH of Dipp), 3.03 (s, 1H, BH), 2.99 (s, 1H, BH), 2.87 (s, 2H, BH), 2.76 (s, 2H, BH), 2.76 (sep, J = 6.8 Hz, 2H, CH of iPr), 2.65 (s, 2H, BH), 2.19 (s, 2H, BH), 1.31 (d, J = 6.9 Hz, 6H, Me of iPr), 1.10 (d, J = 6.8 Hz, 6H, Me of iPr), 0.25 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 42.5 (s, BN(SiMe3)2), 2.1 (d, J = 143.2 Hz, BCb), 0.7 (d, J = 149.7 Hz, BCb), −4.5 (d, J = 147.3 Hz, BCb), −9.8 (m, BCb); 11B{1H} NMR (C6D6): δ = 42.4 (s, BN(SiMe3)2), 2.6 (s, BCb), −0.8 (s, BCb), −4.5 (s, BCb), −9.3 (s, BCb), −10.4 (s, BCb); 13C{1H} NMR (C6D6): δ = 144.0 (C of Dipp), 135.8 (C of Dipp), 125.9 (C of Dipp), 122.9 (C of Dipp), 89.6 (C of Cb), 29.0 (CHMe2), 25.2 (CHMe2), 21.1 (CHMe2), 3.6 (SiMe3); HRMS (m/z): [M + H]+ calcd for C21H46N2B11Si2, 503.4223; found 503.4227; elemental analysis: calcd for C21H45B11N2Si2: C, 50.38; H, 9.06; N, 5.60; found C, 50.28; H, 9.04; N, 5.47.
2c (yellow block crystals, 110 mg, 75%): 1H NMR (C6D6): δ = 7.35 (s, 2H, CH of Mes*), 3.54 to 2.24 (m, 10H, BH), 1.43 (s, 18H, CMe3), 1.32 (s, 9H, CMe3), 0.26 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 7.35 (s, 2H, CH of Mes*), 3.06 (m, 2H, BH), 2.90 (s, 2H, BH), 2.79 (s, 1H, BH), 2.74 (s, 1H, BH), 2.14 (s, 2H, BH), 1.43 (s, 18H, CMe3), 1.32 (s, 9H, CMe3), 0.26 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 42.8 (s, BN(SiMe3)2), 2.4 (d, J = 136.6 Hz, BCb), −0.7 (d, J = 136.2 Hz, BCb), −4.4 (d, J = 138.7 Hz, BCb), −10.3 (m, BCb); 11B{1H} NMR (C6D6): δ = 43.3 (s, CbBN4), 2.5 (s, BCb), −0.4 (s, BCb), −4.4 (s, BCb), −9.7 (s, BCb); 13C{1H} NMR (C6D6): δ = 146.3 (C of Mes*), 144.6 (C of Mes*), 138.3 (C of Mes*), 122.4 (C of Mes*), 90.8 (C of Cb), 37.1 (CMe3), 34.7 (CMe3), 32.8 (CMe3), 31.7 (CMe3), 3.9 (SiMe3); HRMS (m/z): [M + OH]− calcd for C27H58ON2B11Si2, 603.5111; found 603.5154; elemental analysis: calcd for C27H57B11N2Si2: C, 55.45; H, 9.82; N, 4.79; found C, 55.03; H, 9.96; N, 4.88.
3a (colorless needle crystals, 97 mg, 88%), 1H NMR (C6D6): δ = 6.91 to 6.84 (m, 3H, CH of Xyl), 6.71 (t, J = 7.8 Hz, 1H, CH of Xyl), 6.55 (d, 2H, J = 7.6 Hz, CH of Xyl), 3.67 to 2.16 (m, 10H, BH), 3.06 (s, 6H, Me of Xyl), 2.02 (s, 6H, Me of Xyl), 0.26 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 6.91 to 6.85 (m, 3H, CH of Xyl), 6.74 to 6.70 (m, 1H, CH of Xyl), 6.57 (d, J = 7.6 Hz, 2H, CH of Xyl), 3.04 (s, 1H, BH), 2.97 (s, 1H, BH), 2.87 (s, 2H, BH), 2.76 (s, 2H, BH), 2.64 (s, 2H, BH), 2.21 (s, 2H, BH), 2.07 (s, 6H, Me of Xyl), 2.03 (s, 6H, Me of Xyl), 0.27 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 36.3 (s, BN(SiMe3)2), 2.0 (d, J = 138.1 Hz, BCb), 0.8 (d, J = 146.2 Hz, BCb), −4.9 (d, J = 148.2 Hz, BCb), −8.9 (m, BCb); 11B{1H} NMR (C6D6): δ = 36.5 (s, BN(SiMe3)2), 2.0 (s, BCb), −0.8 (s, BCb), −4.8 (s, BCb), −10.3 (s, BCb); 13C{1H} NMR (C6D6): δ = 146.1 (C of Xyl), 135.0 (C of Xyl), 125.2 (C of Xyl), 124.7 (C of Xyl), 124.1 (C of Xyl), 122.8 (C of Xyl), 89.1 (C of Cb), 18.3 (CHMe2), 18.2 (CHMe2), 3.5 (SiMe3); HRMS (m/z): only 2a was detected. Elemental analysis: calcd for C26H46B11N3Si2: C, 54.24; H, 8.05; N, 7.30; found C, 53.95; H, 8.14; N, 7.12.
3a′ (brown oil): 1H NMR (C6D6): δ = 6.88 to 6.81 (m, 3H, CH of Xyl), 6.75 to 6.67 (m, 3H, CH of Xyl), 3.45 to 2.76 (m, 10H, BH), 2.02 (s, 6H, Me of Xyl), 1.74 (s, 6H, Me of Xyl), 0.31 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 6.87 to 6.81 (m, 3H, CH of Xyl), 6.75 to 6.67 (m, 3H, CH of Xyl), 3.06 (s, 2H, BH), 2.86 (s, 2H, BH), 2.74 (s, 2H, BH), 2.63 (s, 2H, BH), 2.25 (s, 2H, BH), 2.03 (s, 6H, Me of Xyl), 1.74 (s, 6H, Me of Xyl), 0.31 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 46.7 (s, BN(SiMe3)2), 1.93 to −0.69 (m, BCb), −5.0 (d, J = 138.7 Hz, BCb), −10.8 (m, BCb); 11B{1H} NMR (C6D6): δ = 46.6 (s, BN(SiMe3)2), 1.4 (s, BCb), −0.4 (s, BCb), −5.0 (s, BCb), −10.6 (s, BCb); 13C{1H} NMR (C6D6): δ = 151.4 (C of Xyl), 144.1 (C of Xyl), 127.7 (C of Xyl), 124.5 (C of Xyl), 123.8 (C of Xyl), 123.4 (C of Xyl), 77.8 (C of Cb), 19.1 (CHMe2), 18.0 (CHMe2), 4.3 (SiMe3); HRMS (LIFDI): calcd for C26H46B11N3Si2, 577.4254; found 577.4248.
3b (off-white block crystals, 93 mg, 74%): 1H NMR (C6D6): δ = 7.08 to 7.04 (m, 3H, CH of Dipp), 6.97 to 6.93 (m, 1H, CH of Dipp), 6.83 to 6.81 (m, 2H, CH of Dipp), 3.39 (sept, J = 6.9 Hz, 2H, CH of iPr), 2.80 (sep, J = 6.8 Hz, 2H, CH of iPr), 1.31 (d, J = 6.9 Hz, 6H, Me of iPr), 1.09 (d, J = 6.8 Hz, 6H, Me of iPr), 1.07 (d, J = 6.9 Hz, 12H, Me of iPr), 0.27 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 7.08 to 7.06 (m, 3H, CH of Dipp), 6.97 to 6.94 (m, 1H, CH of Dipp), 6.84 to 6.82 (m, 2H, CH of Dipp), 3.39 (sep, J = 6.9 Hz, 2H, CH of iPr), 3.06 (s, 1H, BH), 2.99 (s, 1H, BH), 2.88 (s, 2H, BH), 2.79 (sep, J = 6.8 Hz, 2H, CH of iPr), 2.77 (s, 2H, BH), 2.72 (s, 2H, BH), 2.21 (s, 2H, BH), 1.31 (d, J = 6.9 Hz, 6H, Me of iPr), 1.10 (d, J = 6.7 Hz, 6H, Me of iPr), 1.07 (d, J = 6.9 Hz, 12H, Me of iPr), 0.27 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 36.6 (s, BN(SiMe3)2), 2.1 (d, J = 145.3 Hz, BCb), 0.6 (d, J = 146.7 Hz, BCb), −4.9 (d, J = 146.4 Hz, BCb), −9.8 (m, BCb); 11B{1H} NMR (C6D6): δ = 36.4 (s, BN(SiMe3)2), 2.1 (s, BCb), −0.6 (s, BCb), −4.9 (s, BCb), −10.2 (s, BCb); 13C{1H} NMR (C6D6): δ = 145.5 (C of Dipp), 144.0 (C of Dipp), 135.9 (C of Dipp), 129.9 (C of Dipp), 125.8 (C of Dipp), 123.6 (C of Dipp), 123.0 (C of Dipp), 89.7 (C of Cb), 30.0 (CHMe2), 29.0 (CHMe2), 25.2 (CHMe2), 22.6 (CHMe2), 21.1 (CHMe2), 3.8 (SiMe3); HRMS (m/z): only 2b was detected. Elemental analysis: calcd for C34H62B11N3Si2·0.2C5H12: C, 59.83; H, 9.22; N, 5.98; found C, 60.77; H, 8.92; N, 6.02.
3b′ was a brown oily residue that could not be purified, and no satisfactory NMR spectra were obtained. However, some diagnostic resonances were observed (see Fig. S46 and S47), and HRMS data support the proposed formulation. 1H NMR (C6D6): δ = 7.06 to 6.99 (m, 7H, CH of Dipp), 6.87 to 6.85 (m, 2H, CH of Dipp), 3.37 (sep, J = 7.2 Hz, 2H, CH of iPr), 2.89 (sep, J = 6.9 Hz, 2H, CH of iPr), 1.25 (d, J = 6.9 Hz, 6H, Me of iPr), 1.10 (d, J = 6.9 Hz, 18H, Me of iPr), 0.37 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 45.5 (s, BN(SiMe3)2), 2.1 to −0.2 (m, BCb), −5.2 (d, J = 154.3 Hz, BCb), −10.3 (br, BCb); 11B{1H} NMR (C6D6): δ = 45.5 (s, BN(SiMe3)2), 1.6 (s, BCb), 0.1 (s, BCb), −5.1 (s, BCb), −10.3 (s, BCb); HRMS (LIFDI): calcd for C34H62B11N3Si2, 689.5506; found 689.5514.
4a: 1H NMR (C6D6): δ = 6.78 to 6.66 (m, 7H, CH of Xyl), 6.50 (d, J = 7.6, 2H, CH of Xyl), 3.66 to 2.22 (m, 10H, BH), 2.09 (s, 6H, Me of Xyl), 2.01 (s, 6H, Me of Xyl), 1.75 (s, 6H, Me of Xyl), 0.36 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 6.78 to 6.67 (m, 7H, CH of Xyl), 6.52 (d, J = 7.6, 2H, CH of Xyl), 3.11 (s, 1H, BH), 2.88 (s, 3H, BH), 2.81 (m, 2H, BH), 1.70 (s, 2H, BH), 2.29 (s, 2H, BH), 2.09 (s, 6H, Me of Xyl), 2.01 (s, 6H, Me of Xyl), 1.75 (s, 6H, Me of Xyl), 0.36 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 0.2 (br, BCb), −5.4 (d, J = 141.7 Hz, BCb), −10.5 (br, BCb); 11B{1H} NMR (C6D6): δ = 0.0 (br, BCb), −5.4 (s, BCb), −10.2 (br, BCb); 13C{1H} NMR (C6D6): δ = 150.9 (C of Xyl), 144.0 (C of Xyl), 135.4 (C of Xyl), 123.9 (C of Xyl), 122.9 (C of Xyl), 78.1 (C of Cb), 19.1 (CHMe2), 18.2 (CHMe2), 18.1 (CHMe2), 5.0 (SiMe3); elemental analysis: calcd for C35H55N4B11Si2: C, 59.47; H, 7.84; N, 7.93; found C, 59.83; H, 8.07; N, 7.61.
4b: 1H NMR (C6D6): δ = 7.02 to 6.91 (m, 7H, CH of Dipp), 6.84 to 6.82 (m, 2H, CH of Dipp), 3.38 (sep, J = 7.0 Hz, 2H, CH of iPr), 2.81 (sep, J = 6.8 Hz, 2H, CH of iPr), 2.40 (br, 2H, CH of iPr), 1.27 (d, J = 6.9 Hz, 6H, Me of iPr), 1.24 (d, J = 6.8 Hz, 6H, Me of iPr), 1.06 (d, J = 6.9 Hz, 24H, Me of iPr), 0.33 (s, 18H, SiMe3); 1H{11B} NMR (C6D6): δ = 7.03 to 6.91 (m, 7H, CH of Dipp), 6.84 to 6.82 (m, 2H, CH of Dipp), 3.38 (sep, J = 7.0 Hz, 2H, CH of iPr), 3.09 (s, 1H, BH), 2.92 (s, 1H, BH), 2.86 (s, 2H, BH), 2.80 (sep, J = 6.8 Hz, 2H, CH of iPr), 2.72 (br, 2H, CH of iPr), 2.41 (s, 2H, BH), 2.26 (s, 2H, BH), 1.27 (d, J = 7.0 Hz, 6H, Me of iPr), 1.24 (d, J = 6.9 Hz, 6H, Me of iPr), 1.06 (d, J = 6.9 Hz, 24H, Me of iPr), 0.33 (s, 18H, SiMe3); 11B NMR (C6D6): δ = 2.4 to −0.5 (m, BCb), −5.1 (d, J = 161.2 Hz, BCb), −10.3 (br, BCb); 11B{1H} NMR (C6D6): δ = 1.8 (s, BCb), 0.1 (s, BCb), −5.2 (s, BCb), −11.3 (s, BCb); 13C{1H} NMR (C6D6): δ = 144.9 (C of Dipp), 141.7 (C of Dipp), 134.9 (C of Dipp), 125.4 (C of Dipp), 124.4 (C of Dipp), 123.1 (C of Dipp), 122.7 (C of Dipp), 122.4 (C of Dipp), 77.8 (C of Cb), 31.6 (CHMe2), 29.7 (CHMe2), 28.9 (CHMe2), 28.7 (CHMe2), 24.9 (CHMe2), 24.4 (CHMe2), 22.7 (CHMe2), 22.2 (CHMe2), 21.1 (CHMe2), 4.1 (SiMe3); HRMS (LIFDI): calcd for C47H79N4B11Si2, 876.6867; found 876.6906.
CCDC 2497356–2497362 (2a–2c, 3a, 3b, 4a and 4b) contain the supplementary crystallographic data for this paper.13a–g
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