Ethan W.
Poole
a,
Itxaso
Bustos
ab,
Thomas M.
Hood
a,
Jennifer E.
Smart
a and
Adrian B.
Chaplin
*a
aDepartment of Chemistry, University of Warwick, Gibbet Hill Road, Coventry CV4 7AL, UK. E-mail: a.b.chaplin@warwick.ac.uk
bFacultad de Química de San Sebastián, Universidad del País Vasco (UPV/EHU), Apdo. 1072, 20080 San Sebastián, Spain
First published on 21st December 2022
The synthesis and iridium coordination chemistry of a new pyridine-based phosphinito pincer ligand 2,6-(ArF2PO)2C5H3N (PONOP-ArF; ArF = 2-(CF3)C6H4) are described, where the P-donors have ortho-trifluoromethylphenyl substituents. The iridium(III) 2,2′-biphenyl (biph) derivative [Ir(PONOP-ArF)(biph)Cl] was obtained by reaction with [Ir(biph)(COD)Cl]2 (COD = 1,5-cyclooctadiene) and subsequent halide ion abstraction enabled isolation of [Ir(PONOP-ArF)(biph)]+ which features an Ir ← F–C bonding interaction in the solid state. Hydrogenolysis of the biphenyl ligand and formation of [Ir(PONOP-ArF)(H)2]+ was achieved by prolonged reaction of [Ir(PONOP-ArF)(biph)]+ with dihydrogen. This transformation paved the way for isolation and crystallographic characterisation of low valent iridium derivatives through treatment of the dihydride with tert-butylethylene (TBE). The iridium(I) π-complex [Ir(PONOP-ArF)(TBE)]+ is thermally stable but substitution of TBE can be achieved by reaction with carbon monoxide. The solid-state structure of the mono-carbonyl product [Ir(PONOP-ArF)(CO)]+ is notable for an intermolecular anagostic interaction between the metal centre and a pentane molecule which co-crystallises within a cleft defined by two aryl phosphine substituents.
Motivated by the aforementioned chemistry established by Krogh-Jespersen, Goldman and co-workers and as part of our work with low coordinate group 9 pincer complexes,4–6 we speculated that the bespoke trifluoromethyl-functionalised PONOP pincer ligand 2,6-(ArF2PO)2C5H3N (PONOP-ArF; ArF = 2-(CF3)C6H4) could pre-organise interaction between a C(sp3)–F bond and reactive iridium(I) derivative, and thereby promote subsequent concerted oxidative addition by reducing the associated kinetic barrier. We herein present work evaluating this hypothesis, using 1 as a well-defined iridium(III) derivative of PONOP-ArF and synthon for the reactive three coordinate iridium(I) complex {Ir(PONOP-ArF)}+ by successive halide ion abstraction and hydrogenolysis of the constituent 2,2′-biphenyl ligand (biph; Fig. 1). Whilst iridium(III) oxidative addition product 2 was ultimately not obtained, during the course of this work iridium complexes featuring a coordinated trifluoromethyl appendage, tert-butylethylene (TBE), and an intermolecular anagostic interaction with pentane have been crystallographically characterised.
Fig. 2 Synthesis and characterisation of iridium(III) complexes 1 and 3; [BArf4]− counter ions omitted for clarity. Solid-state structures of 1 and 3 drawn with thermal ellipsoids at 30% probability and without minor disordered components (1 × ArF substituent in 3) and solvent molecules. Selected metal-based bond lengths (Å) and angles (°): 1, Ir1–P2, 2.2800(8); Ir1–P3, 2.3050(8); Ir1–N20, 2.099(3); Ir1–C4, 2.066(3); Ir1–C15, 2.052(3); Ir1–Cl16, 2.4774(8); P2–Ir1–P3, 158.03(3); N20–Ir1–C15, 176.54(11); C4–Ir1–Cl16, 176.51(10); 3, Ir1–P2, 2.2795(9); Ir1–P3, 2.3075(8); Ir1–N20, 2.109(3); Ir1–C4, 2.026(3); Ir1–C15, 2.056(3); Ir1⋯F35, 2.543(2); P2–Ir1–P3, 160.17(3); N20–Ir–C15, 174.40(11); C4–Ir1⋯F35, 168.37(10); C, Ir⋯F, 2.514(8).12 |
Exploiting an iridium(III) precursor first described by Crabtree and informed by previous work in our laboratories involving {M(biph)Cl} (M = Rh, Ir) synthons,4,5,9–111 was synthesised through reaction of [Ir(biph)(COD)Cl]2 (COD = 1,5-cyclooctadiene) with PONOP-ArF in CH2Cl2 at 50 °C and isolated in 75% yield. In solution, 1 is characterised by time-averaged Cs symmetry and a significant downfield shift of the 31P resonance of the pincer ligand (δ 96.4 to 111.4), which is further notable for the loss of any significant coupling to 19F. Inequivalent 19F resonances are observed at very similar field to the free ligand: δ −57.1 and −57.3 (cf. δ −57.0), with the former significantly line broadened relative to the latter, presumably reflecting slower restricted rotation of the P–ArF bonds straddling the biphenyl ligand. The coordinated 13C resonances of the biphenyl ligand are located at δ 143.2 (m) and 140.2 (t, 2JPC = 9 Hz) with coupling to two equivalent 31P nuclei resolved for the latter. The structure of 1 was corroborated in the solid state by single crystal X-ray diffraction, exhibiting a pseudo-octahedral coordination geometry about the metal centre and unsymmetrically orientated ArF substituents (Fig. 2). The Ir1–C4 (2.066(3) Å) and Ir1–C15 (2.052(3) Å) distances are not statistically different, but the trend suggests in this system the chloride ligand exerts a greater trans influence than the pyridine-based donor.
Following our proposed retrosynthesis, 1 was treated with the halide ion abstracting agent Na[BArf4] (Arf = 3,5-(CF3)2C6H3), using the weakly coordinating solvent dichloromethane to accentuate the electrophilicity of the alkali metal and favour formation of a low-coordinate complex. The resulting derivative is formulated as [Ir(PONOP-ArF)(biph)][BArf4] 3 and was isolated from solution in 69% yield following filtration and crystallisation from CH2Cl2–hexane (Fig. 2). Crystallographic analysis of 3 indicates a dative bonding interaction between iridium and one of the triflouromethane groups is adopted in the solid state, as gauged by an Ir1⋯F35 contact of 2.543(2) Å, conferring a formally pseudo-octahedral metal coordination geometry (C4–Ir1–F35 = 168.37(10)°). This outcome is significant given the extremely limited number of well-defined transition metal examples of featuring M ← F–C bonding interactions. Indeed, a search of the CSD (v. 5.43) identified only iridium(III) 8-fluoroquinoline complex C with an Ir⋯F contact <2.8 Å (Fig. 2, Ir⋯F = 2.514(8) Å).12 Work by Togni and co-workers with PPh2(5,6,7,8-tetrafluoronaphthalenyl) is also notable, but the two iridium complexes studied in the solid state feature considerably more remote Ir⋯F contacts of ca. 3.0 Å.13 Moreover, preceding work in our group has involved characterisation of a series of rhodium(III) biph complexes of PPh2ArF with Rh⋯F contacts ranging from 2.363(2) to 2.459(2) Å.10 Consistent with the weakly interacting nature of the trifluoromethane group, the Ir1–C4 bond (2.026(3) Å) is significantly contracted relative to the Ir1–C15 (2.056(3) Å) bond distance. Indeed, isolated 3 adopts time-averaged C2v symmetry in CD2Cl2 solution at 298 K, indicating that rapid pseudorotation of the biph ligand and that Ir ← F–C bonding is not persistent on the NMR time scale.4,10 At this temperature, the pincer complex is characterised by single broad 31P and 19F resonances at δ 123.8 and δ −58.8, respectively (cf. δ 111.4 and δ −57.1/−57.3 for 1).
Placing a solution of 3 in CD2Cl2 under an atmosphere of CO (1 atm) resulted in immediate and quantitative formation of the carbonyl derivative [Ir(PONOP-ArF)(biph)(CO)][BArf4] 4 (Fig. 3), which adopts a static Cs symmetric structure characterised by a broad upfield-shifted 31P resonance at δ 103.3 (cf. δ 123.8 for 3) and two 19F signals at δ −57.4 and −57.5; the latter is line broadened relative to the former, presumably reflecting slower restricted rotation of the P–ArF bonds straddling the biphenyl ligand (cf.1). Coordination of CO is corroborated by a sharp triplet resonance at δ 172.6 (2JPC = 8 Hz) in the 13C{1H} NMR spectrum, IR spectroscopy with ν(CO) = 2062 cm−1, ESI-MS, and structural elucidation by single crystal X-ray diffraction (Fig. 3). The solid-state structure of 4 is rather routine, but the metrics associated with coordination of biph (Ir1–C4 = 2.092(3), Ir1–C15 = 2.072(3) Å) enable compilation of the following trend in ligand trans influence for this iridium(III) system by comparison to the structures of 1 and 3: CF3 < py < Cl− ≤ CO.
Fig. 3 Reactivity of complex 3; MesH = mesitylene and [BArf4]− counter ions omitted for clarity. Solid-state structures of 4 and 6 drawn with thermal ellipsoids at 30% probability and without solvent molecules. Selected metal-based bond lengths (Å) and angles (°): 4, Ir1–P2, 2.3300(7); Ir1–P3, 2.3243(7); Ir1–N20, 2.102(2); Ir1–C4, 2.092(3); Ir1–C15, 2.072(3); Ir1–C16, 1.958(3); C16–O17, 1.123(4); P2–Ir1–P3, 159.85(2); N20–Ir1–C15, 171.25(10); C4–Ir1–Cl16, 177.09(11); 6, Ir1–P2, 2.2657(11); Ir1–P3, 2.2704(12); Ir1–N20, 2.058(4); Ir1–Cnt(C4,C5), 2.110(12); C4–C5, 1.304(12), P2–Ir1–P3, 156.46(5); N20–Ir1–Cnt(C4,C5), 175.3(4); C4–C5–C6, 130.6(10); D, Rh–Cnt(CC), 2.051(3); CC, 1.360(10); N–Rh–Cnt(CC), 174.27(14); CC–C, 127.7(5).15 Cnt = centroid. |
Moving on with our proposed retrosynthesis, 3 was heated in CH2Cl2 under an atmosphere of dihydrogen at 50 °C resulting in hydrogenolysis of the biph ligand and generation of the iridium(III) dihydride [Ir(PONOP-ArF)(H)2][BArf4] 5 within 8 days (1 atm H2)/3 days (4 atm H2), which is characterised by time-averaged C2v symmetry (δ31P 140.4; δ19F −57.0; δ1H −18.41 (br), T1 = 883 ± 17 ms (298 K, 600 MHz)) and was isolated in 84% yield (Fig. 3). Targeting in situ generation of the putative three coordinate iridium(I) complex {Ir(PONOP-ArF)}+, 5 was thereafter treated with 10 equivalents of the bulky sacrificial hydrogen acceptor TBE in the inert hydrocarbon solvent mesitylene.14 Heating at 50 °C resulted in quantitative formation of iridium(I) π-complex [Ir(PONOP-ArF)(TBE)][BArf4] 6 within 16 hours, which was isolated and fully characterised (Fig. 3). In d8-toluene solution, coordination of TBE is corroborated by downfield alkene 1H resonances at δ 4.55, 3.33 and 3.16, and conferral of asymmetry in the metal coordination sphere, viz. δ31P 151.9, 143.0 (2JPP = 380 Hz) and δ19F −56.6, −57.4, −58.6, −58.9. Crystals suitable for analysis by X-ray diffraction were obtained by recrystallisation from mesitylene–pentane and enable, to the best of our knowledge, structural elucidation of an iridium–TBE complex in the solid state for the first time (CSD v. 5.43). A neutral rhodium PNP pincer complex D reported by Ozerov and co-workers is the closest well-defined structural precedent (Fig. 3), but we are reluctant to make a detailed comparison of the metrics in 6 as the TBE ligand is not located with very high precision due to the quality of data collected (Rint = 0.0883).15
In attempt to induce formation of 2 by dissociation of TBE and C(sp3)–F bond cyclometallation, isolated 6 was heated in mesitylene at elevated temperature (120 °C, Fig. 4). Analysis of the reaction mixture by NMR spectroscopy after 24 hours, however, indicated that 2 was stable under these conditions with only ca. 10% decomposition of the anion apparent from the 19F{1H} NMR spectrum.16 Reactions involving C–H bond cyclometallation of tert-butyl and neo-pentyl substituted PNP pincer ligands have previously been reported for iridium and demonstrate that formation of iridacyclobutane and – most pertinent to this study – iridacyclopentane rings are possible.17
Placing a solution of 6 in mesitylene under an atmosphere of CO (1 atm) resulted in immediate conversion into square planar iridium(I) carbonyl complex [Ir(PONOP-ArF)(CO)][BArf4] 7 (Fig. 4) at room temperature and shows that TBE can be readily substituted if the incoming ligand is a sufficiently strong donor (i.e. not a CF3 appendage). Complex 7 was isolated in 74% yield and the structure verified by a combination of NMR and IR spectroscopy. Sharp 31P and 19F singlet resonances δ 151.1 and δ −56.3 are consistent with C2v symmetry and coordination of CO is marked out by a sharp triplet resonance at δ 179.0 (2JPC = 9 Hz) in the 13C{1H} NMR spectrum (CD2Cl2). Analysis by IR spectroscopy identified a single carbonyl stretching band centred at ν(CO) = 2040 cm−1 and confirmed formation of a mono-carbonyl derivative. In line with the electron-withdrawing character of the phosphine substituents in 7, this band is significantly blue-shifted relative to alkyl substituted PONOP homologues such as [Ir(2,6-(tBu2PO)2C5H3N)(CO)][BArf4] (ν(CO) = 2010 cm−1).18 The structure of 7 is further substantiated in the solid state using single crystals grown from CH2Cl2−pentane (Fig. 4). The metal coordination geometry and associated metrics are in harmony with the spectroscopic data and otherwise unremarkable. Wider inspection of the unit cell, however, revealed an interesting intermolecular interaction between the iridium centre and a molecule of pentane which co-crystallises within a cleft defined by two aryl phosphine substituents (Fig. 4, left).19 Supported by the lattice, this anagostic interaction is characterised by an ⋯–C contact of 2.92 Å and Ir⋯H–C angle of 144°.20,21 Whilst it is not uncommon for M⋯H–C interactions of this nature to be observed in solid-state structures of square planar platinum group complexes, a search of the CSD (v. 5.43) identified only 2 palladium(II) examples with intermolecular M⋯H contacts <3.0 Å with an alkane.22
1 H NMR (CD2Cl2, 500 MHz): δ 7.67 (dd, 3JHH = 7.4, 3JPH = 3.5, 4H, 3-ArF), 7.63 (t, 3JHH = 7.9, 1H, 4-py), 7.49 (t, 3JHH = 7.6, 4H, 4-ArF), 7.44 (t, 3JHH = 7.6, 4H, 5-ArF), 7.36 (dd, 3JHH = 7.3, 2JPH = 2.9, 4H, 6-ArF), 6.60 (d, 3JHH = 7.9, 2H, 3-py).
13 C{ 1 H} NMR (CD2Cl2, 126 MHz): δ 161.2 (d, 2JPC = 10, 2-py), 142.5 (s, 4-py), 137.9 (d, 1JPC = 40, 1-ArF), 133.1 (d, 2JPC = 3, 6-ArF), 132.8 (qd, 2JFC = 32, 2JPC = 25, 2-ArF), 132.0 (s, 5-ArF), 130.3 (s, 4-ArF), 126.7 (br, 3-ArF), 124.8 (q, 1JFC = 275, ArF{CF3}), 106.5 (d, 3JPC = 2, 3-py).
19 F{ 1 H} NMR (CD2Cl2, 376 MHz): δ −57.0 (d, 4JPF = 64).
31 P{ 1 H} NMR (CD2Cl2, 162 MHz): δ 96.4 (sept, 4JPF = 64).
HR ESI-MS (positive ion, 4 kV): 774.0588 ([M+Na]+, calcd 774.0592) m/z.
31 P{ 1 H} NMR (CD2Cl2, 162 MHz): δ 42.6 (s).
1 H NMR (CD2Cl2, 500 MHz): δ 9.06 (br, 2H, ArF), 8.60 (d, 3JHH = 7.5, 1H, 6-biph), 8.04 (t, 3JHH = 8.2, 1H, 4-py), 7.61–7.77 (m, 6H, ArF), 7.18 (d, 3JHH = 8.2, 2H, 3-py), 7.12–7.28 (m, 10H, 3,5-biph + ArF), 7.04 (t, 3JHH = 7.4, 1H, 4-biph), 6.68 (d, 3JHH = 7.4, 1H, 3′-biph), 6.15 (t, 3JHH = 7.4, 1H, 4′-biph), 5.86 (d, 3JHH = 7.5, 1H, 6′-biph), 5.76 (t, 3JHH = 7.5, 1H, 5′-biph).
13 C{ 1 H} NMR (CD2Cl2, 126 MHz): δ 159.8 (vt, JPC = 5, 2-py), 154.3 (s, 2-biph), 153.5 (s, 2′-biph), 143.9 (s, 4-py), 143.1–143.3 (m, 1-biph), 139.8 (t, 2JPC = 9, 1′-biph), 135.2 (s, 6′-biph), 134.6 (s, 6-biph), 133.2 (s, ArF), 132.9 (br, ArF), 131.4 (q, 2JFC = 33, 2/2′-ArF), 130.9 (s, ArF), 130.3–130.6 (m, ArF), 129.6 (q, 2JFC = 33, 2/2′-ArF), 127.6–127.8 (m, ArF), 127.1–127.3 (m, ArF), 126.1 (s, 5-biph), 125.3 (s, 5′-biph), 123.8 (q, 1JFC = 275, ArF{CF3}), 123.1 (s, 4-biph), 122.9 (q, 1JFC = 275, ArF{CF3}), 122.2 (s, 4′-biph), 120.3 (s, 3-biph), 119.6 (s, 3′-biph), 105.1 (vt, JPC = 5 3-py). Not all ArF signals unambiguously located.
19 F{ 1 H} NMR (CD2Cl2, 282 MHz): δ −57.1 (br, 6F), −57.3 (s, 6F).
31 P{ 1 H} NMR (CD2Cl2, 121 MHz): δ 111.4 (s).
HR ESI-MS (positive ion, 4 kV): 1096.0945 ([M–Cl]+, calcd 1096.0952) m/z.
1 H NMR (CD2Cl2, 500 MHz, selected data): δ 8.27 (t, 3JHH = 8.3, 1H, 4-py), 7.40 (d, 3JHH = 8.3, 2H, 3-py). The spectrum is characterised by broad overlapping aromatic signals consistent with a fluxional time-averaged C2v symmetric structure on the timescale of the experiment.
13 C{ 1 H} NMR (CD2Cl2, 126 MHz, selected data): δ 160.0 (s, 2-py), 147.3 (s, 4-py), 131.2 (q, 2JFC = 33, 2-ArF), 123.3 (q, 1JFC = 275, ArF{CF3}), 106.8 (vt, JPC = 5, 3-py).
19 F{ 1 H} NMR (CD2Cl2, 376 MHz): δ −58.8 (br, 12F, ArF), −62.9 (s, 24F, Arf).
31 P{ 1 H} NMR (CD2Cl2, 162 MHz): δ 123.8 (s).
HR ESI-MS (positive ion, 4 kV): 1096.0963 ([M]+, calcd 1096.0952) m/z.
1 H NMR (CD2Cl2, 500 MHz): δ 8.33 (t, 3JHH = 8.3, 1H, 4-py), 7.91 (d, 3JHH = 7.2, 2H, 3-ArF), 7.65–7.80 (m, 15H, 2-Arf + 4,5,6-ArF + 6-biph), 7.61 (d, 3JHH = 7.6, 1H, 3-biph), 7.55 (br, 4H, 4-Arf), 7.48–7.54 (m, 2H, 3′-ArF), 7.44 (d, 3JHH = 8.3, 2H, 3-py), 7.40 (t, 3JHH = 7.8, 2H, 4′-ArF), 7.31 (t, 3JHH = 7.5, 1H, 4-biph), 7.18 (t, 3JHH = 7.4, 1H, 5-biph), 7.11 (d, 3JHH = 7.7, 1H, 3′-biph), 7.05 (t, 3JHH = 7.8, 2H, 5′-ArF), 6.92 (dvt, 3JHH = 8.0, JPH = 16, 2H, 6′-ArF), 6.60 (t, 3JHH = 7.5, 1H, 4′-biph), 6.32 (t, 3JHH = 7.4, 1H, 5′-biph), 5.45 (d, 3JHH = 7.5, 1H, 6′-biph).
13 C{ 1 H} NMR (CD2Cl2, 126 MHz): δ 172.6 (t, 2JPC = 7, CO), 162.2 (q, 1JCB = 50, 1-Arf), 159.1 (s, 2-py), 153.5 (s, 2′-biph), 151.9 (s, 2-biph), 148.2 (s, 4-py), 147.0 (t, 2JPC = 10, 1′-biph), 136.8 (s, 6-biph), 135.2 (s, 2-Arf), 134.7 (s, 6′-ArF), 133.4 (obscured t, 2JPC = 7, 1-biph), 133.3 (s, 4′-ArF), 132.5 (vt, JPC = 15, 5-ArF), 131.0 (vt, JPfC = 14, 5′-ArF), 130.7 (s, 6′-biph), 129.9 (s, 5-biph), 129.3 (qq, 2JFC = 32, 3JCB = 3, 3-Arf), 129.2–129.4 (m, 3-ArF), 128.3–128.4 (m, 3′-ArF), 128.0 (s, 5′-biph), 126.7 (s, 4′-biph), 126.4 (s, 4-biph), 125.0 (q, 1JFC = 273, Arf{CF3}), 125 (obscured, 1′-ArF), 123.5 (q, 1JFC = 274, ArF{CF3}), 123.4 (s, 3-biph), 123.3 (s, 3′-biph), 122.9 (q, 1JFC = 274, ArF{CF3}), 117.9 (sept, 3JFC = 4, 4-Arf), 107.2 (vt, JPC = 6, 3-py). Not all ArF signals unambiguously located.
19 F{ 1 H} NMR (CD2Cl2, 376 MHz): δ −57.4 (s, 6F, ArF), −57.5 (br, 6F, ArF), −62.9 (s, 24F, Arf).
31 P{ 1 H} NMR (CD2Cl2, 162 MHz): δ 103.3 (br s).
HR ESI-MS (positive ion, 4 kV): 1124.0902 ([M]+, calcd 1124.0901) m/z.
IR (ATR): ν(CO) 2062 cm−1.
1 H NMR (CD2Cl2, 500 MHz): δ 8.22 (dvt, 3JHH = 8.0, JPH = 16, 4H, 6-ArF), 8.01 (t, 3JHH = 8.2, 1H, 4-py), 7.88 (d, 3JHH = 7.1, 4H, 3-ArF), 7.81 (t, 3JHH = 7.4, 4H, 5-ArF), 7.77 (t, 3JHH = 7.4, 4H, 4-ArF), 7.71–7.74 (m, 8H, 2-Arf), 7.55 (br, 4H, 4-Arf), 7.19 (d, 3JHH = 8.2, 2H, 3-py), −18.41 (br, 2H, Ir–H).
13 C{ 1 H} NMR (CD2Cl2, 126 MHz): δ 162.1 (q, 1JCB = 50, 1-Arf), 160.1 (br, 2-py), 145.7 (s, 4-py), 137.5 (br, 6-ArF), 135.2 (s, 2-Arf), 134.4 (s, 4-ArF), 132.5 (vt, JPC = 13, 5-ArF), 131.0 (q, 2JFC = 33, 2-ArF), 130.6 (vt, JPC = 58, 1-ArF), 129.3 (qq, 2JFC = 32, 3JCB = 3, 3-Arf), 129.1 (br, 3-ArF), 125.0 (q, 1JFC = 273, Arf{CF3}), 123.8 (q, 1JFC = 275, ArF{CF3}), 117.9 (sept, 3JFC = 4, 4-Arf), 105.8 (br, 3-py).
19 F{ 1 H} NMR (CD2Cl2, 376 MHz): δ −57.0 (s, 12F, ArF), −62.9 (s, 24F, Arf).
31 P{ 1 H} NMR (CD2Cl2, 162 MHz): δ 140.4 (s).
HR ESI-MS (positive ion, 4 kV): 946.0487 ([M]+, calcd 946.0481) m/z.
1 H NMR (d8-toluene, 500 MHz, selected data): δ 6.73 (t, 3JHH = 8.2, 1H, 4-py), 6.12–6.32 (m, 2H, 3/5-py), 4.48–4.62 (m, 1H, CHCH2), 3.38–3.28 (m, 1H, CHCHH), 3.16 (d, 3JHH = 8.1, 1H, CHCHH), −0.04 (s, 9H, tBu). The spectrum is characterised by very broad ArF signals consistent with a C1 symmetric structure on the timescale of the experiment.
13 C{ 1 H} NMR (d8-toluene, 126 MHz, selected data): δ 161.5 (br, 2/6-py), 145.7 (s, 4-py), 104.2–104.8 (m, 3/5-py), 82.8 (br, H=CH2, confirmed by HMQC), 44.4 (br, CHH2), 35.5 (s, tBu{C}), 28.0 (s, tBu{CH3}).
19 F{ 1 H} NMR (d8-toluene, 376 MHz): δ −56.6 (br, 3F, ArF), −57.4 (br, 3F, ArF), −58.6 (br, 3F, ArF), −58.9 (br, 3F, ArF), −62.9 (s, 24F, Arf).
31 P{ 1 H} NMR (d8-toluene, 162 MHz): δ 151.9 (d, 2JPP = 380, 1P), 143.0 (d, 2JPP = 380, 1P).
HR ESI-MS (positive ion, 4 kV): 1028.1251 ([M]+, 1028.1264 calcd) m/z.
1 H NMR (CD2Cl2, 500 MHz): δ 8.13 (t, 3JHH = 8.3, 1H, 4-py), 8.02 (dvt, 3JHH = 8.2, JPH = 16, 4H, 6-ArF), 7.95 (d, 3JHH = 7.5, 4H, 3-ArF), 7.84 (t, 3JHH = 7.7, 4H, 4-ArF), 7.76 (t, 3JHH = 7.9, 4H, 5-ArF), 7.70–7.75 (m, 8H, 2-Arf), 7.54 (br, 4H, 4-Arf), 7.18 (d, 3JHH = 8.3, 2H, 3-py).
13 C{ 1 H} NMR (CD2Cl2, 126 MHz): δ 179.0 (t, 2JPC = 9, CO), 162.3 (vt, JPC = 9, 2-py), 162.2 (q, 1JCB = 50, 1-Arf), 148.7 (s, 4-py), 135.9 (vt, JPC = 20, 6-ArF), 135.2 (br, 2-Arf), 134.8 (s, 4-ArF), 133.1 (vt, JPC = 13, 5-ArF), 131.5 (qvt, 2JFC = 33, JPC = 7, 2-ArF), 129.6 (vt, JPC = 60. 1-ArF), 129.6 (obscured, 3-ArF), 129.3 (qq, 2JFC = 31, 3JCB = 3, 3-Arf), 125.0 (q, 1JFC = 272, Arf{CF3}), 123.8 (q, 1JFC = 275, ArF{CF3}), 117.9 (sept, 3JFC = 4, 4-Arf), 105.8 (vt, JPC = 7, 3-py).
19 F{ 1 H} NMR (CD2Cl2, 376 MHz): δ −56.3 (s, 12F, ArF), −62.9 (s, 24F, Arf).
31 P{ 1 H} NMR (CD2Cl2, 162 MHz): δ 151.1 (s).
HR ESI-MS (positive ion, 4 kV): 974.0448 ([M]+, 974.0431 calcd) m/z.
IR (ATR): ν(CO) 2040 cm−1.
Footnote |
† Electronic supplementary information (ESI) available: NMR, IR and ESI-MS spectra of isolated compounds. CCDC 2217137–2217141. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d2dt03608h |
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