Introduction

Carbon monoxide (CO) is a diatomic molecule that represents an iconic ligand in organometallic chemistry and a reagent of paramount importance in metallurgical processes1,2 and catalysis3. The (reversible) coordination and insertion of carbon monoxide (Fig. 1a) plays a crucial role in many industrial processes, e.g. the Monsanto and CativaTM processes for the manufacture of acetic acid4,5,6, the Fischer-Tropsch process where syngas (CO/H2) is converted to hydrocarbons7,8,9,10,11, and the Mond process for the purification of nickel2,12. Additionally, the controlled release of carbon monoxide (decarbonylation) has found applications in bond formation processes13,14,15 and therapeutic applications16,17,18,19. These processes have traditionally been dominated by transition metal compounds, but in recent years, researchers have developed innovative approaches to bring selective transformations of CO into the realm of molecular main group chemistry20,21,22. Successful strategies have been based on low-valent and multiply-bonded compounds, geometrically constrained species, and frustrated Lewis pairs. Initial findings cover diverse types of transformations with carbon monoxide, including the fundamentally important reactions of coordination/dissociation and insertion/extrusion (Fig. 1b). The detailed understanding and control of these elementary reactions in the chemistry of carbon monoxide with main group elements is the basis for the development of selective and competitive transformations. Consequently, the identification of model systems that can equilibrate between isolable compounds via coordination/dissociation and insertion/extrusion pathways is extremely important. For the coordination/dissociation of CO, a small number of such systems has been identified20,21, but the situation is even more challenging for the case of insertion/extrusion pathways. Very rare examples include one low-valent boron compound23 and an aluminum species that reversibly incorporates CO into a cyclic framework24. As a crucial point, the shuttling between the insertion and the extrusion of CO in these two cases does not cover the synthetically important class of compounds with terminal acyl groups C(O)R (R = alkyl, aryl) and is achieved through conventional thermal activation of the reactants. In an orthogonal approach, the light-driven extrusion of CO from a terminal acyl germane has been reported, but required activated acyl groups and very harsh reaction conditions (400 W high-pressure Hg vapor lamp, containing “hard” UV-C radiation which is not part of ambient light as it is absorbed by the ozone layer)25. In addition, no signs of reversibility of this transformation have been reported, a crucial part en route to potential catalytic transformations of CO. In view of the light-responsive nature of many organobismuth species26,27,28, bismuth acyl compounds are extremely attractive targets, but have remained elusive to date, despite attempts at their synthesis29.

Fig. 1: Reactivity of carbon monoxide (CO) in transition and main group metal chemistry.
Fig. 1: Reactivity of carbon monoxide (CO) in transition and main group metal chemistry.
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a Fundamental transformations of carbon monoxide in transition metal chemistry and b main group metal chemistry. c State of the art in photochemically-driven CO insertion/extrusion with main group complexes. UV = ultraviolet, Ph = phenyl, R = organic substituent, Ar = aryl, LED = light-emitting diode.

Here we report the synthesis of isolable and thoroughly characterized diaryl bismuthides, [BiR2], which enable an inverse-polarity-approach to access bismuth acyl compounds (thereby introducing the Bi–C(O)R structural motif to main group chemistry) and engage in visible-light-induced reversible CO extrusion/insertion reactions.

Results and Discussion

The in-situ generation of simple bismuthides [BiR2] has been suggested based on trapping experiments (R = aryl, alkyl)30,31,32,33,34,35,36. These parent compounds do not benefit from stabilizing electronic effects (such as aromatization or the α-silyl effect)37,38,39,40 that aim at significant delocalization of electron density. One set of single-crystal X-ray diffraction data of a diphenyl bismuthide (without additional analytical data or a yield) has serendipitously been reported41, granting first glimpses at the yet elusive class of diaryl bismuthides. But a rational synthesis facilitating the isolation and characterization of these simple bismuthides has not been reported to date. We envisioned that the reduction of isolable, low-valent dibismuthanes, R2Bi–BiR2, might pave the way to the elusive parent bismuthides [BiR2]. Indeed, the reaction of compounds 1-4 with potassium graphite (KC8) in the presence of [2.2.2]cryptand (crypt) in THF gave the target compounds 5-8 in 38-84% isolated yield (Fig. 2). The bismuthides are intensely dark orange to dark red compounds that appear almost black in the solid state and could be fully characterized.

Fig. 2: Preparation of diaryl bismuthides and their molecular structures.
Fig. 2: Preparation of diaryl bismuthides and their molecular structures.
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a Synthesis of aryl-substituted bismuthides 5-8; crypt = [2.2.2]cryptand. THF = tetrahydrofuran, rt = room temperature. b Molecular structures of compounds 5-7 in the solid state. 5 and 7 crystallize in the monoclinic space group P21/c (Z = 4) and 6 in the triclinic space group P\(\bar{1}\) (Z = 2). Displacement ellipsoids are shown at the 50% level. Hydrogen atoms are omitted and the CH2 groups of [2.2.2]cryptand displayed as wireframe for clarity. Note that XRD data of 7 (without any additional analytical data or a yield of the compound) have previously been reported with different cell parameters41. Selected bond lengths (Å) and angles (°): 5, Bi1−C1/14, 2.259(5)/2.271(5), C1−Bi1−C14, 92.36(18); 6, Bi1−C1/10, 2.307(5)/2.312(5), C1−Bi1−C10, 95.52(16); 7, Bi1−C1/7, 2.273(4)/2.301(5), C1−Bi1−C7, 97.88(16).

1H and 13C{1H} NMR spectra of compounds 5-8 show the expected signal pattern for the respective aryl substituents at bismuth and one equivalent of [2.2.2]cryptand chelating a potassium ion. Extreme changes in chemical shifts of the aryl groups compared to the neutral parent compounds (BiR3) and the dibismuthane starting materials are not apparent42,43,44,45,46,47,48, suggesting a significant localization of two lone pairs at the bismuth atom. Single-crystal X-ray analyses confirmed the suggested structures of compounds 5-7 (Fig. 2b).

The bismuth atoms do not show any directional bonding interactions towards the [K(crypt)]+ cations based on distance criteria. They are found in a bent coordination geometry (C−Bi−C, 92.36(18) − 97.88(16)°), with Bi−C bond lengths of 2.259(5) to 2.312(5) Å. These values are close to those reported for the corresponding dibismuthanes (e.g. Ph4Bi2: Bi−C, 2.26(2)/2.28(2) Å; C−Bi−C/Bi, 90.9(5) − 98.3(8)°)49 and triaryl bismuthanes (e.g. Mes3Bi: Bi−C, 2.31(1) − 2.32(1) Å; C−Bi−C, 94.7(4) − 107.6(4)°)50. The close similarities in Bi–C bond lengths speak against significant Bi–C multiple bond character, hinting at a considerable charge localization at the bismuth atoms of the bismuthides.

While solid samples of compounds 5-8 are stable at −30 °C for months, they slowly decompose in solution at 23 °C, resulting in the formation of bismuth black51 and phenanthrene (for 5), mesitylene (for 6), benzene (for 7) or 1,3-diisopropylbenzene (for 8).

Based on the initial analyses of the simple diaryl bismuthides 5-8, which suggested a high concentration of negative charge at the bismuth atoms, we hypothesized that inversed polarity synthetic strategies should be viable. In such approaches, the [BiR2] synthon would be nucleophilic, which contrasts with established strategies for the creation of BiIII–C bonds that typically exploit electrophilic bismuth precursors (such as bismuth halides) and reagents with nucleophilic carbon atoms (as in organo lithium compounds and Grignard reagents). This approach would promise to bring previously inaccessible structural motifs within reach. Specifically, the yet elusive bismuth acyl species R2Bi–C(O)R’ were identified as particularly attractive synthetic targets. Indeed, addition of 1-adamantanecarbonyl chloride to solutions of 5 or 6 at room temperature resulted in a color change from dark orange/red to yellow, and the acyl bismuthanes 9 and 10 could be isolated in 62-84% yield as yellow (9) or orange (10) solids and fully characterized (Fig. 3a).

Fig. 3: Synthesis and characterization of acyl bismuthanes.
Fig. 3: Synthesis and characterization of acyl bismuthanes.
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a Synthesis of acyl bismuthanes 9 and 10. crypt = [2.2.2]cryptand, THF = tetrahydrofuran, rt = room temperature, Mes = mesityl = 2,4,6-trimethylphenyl. b Molecular structures of compounds 9 (orthorhombic space group P212121, Z = 4) and 10 (orthorhombic space group Pbca, Z = 8) in the solid state. Displacement ellipsoids are shown at the 50% level. Hydrogen atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): 9, Bi1−C1/14, 2.233(6)/2.245(6), Bi1−C15, 2.389(5), C15−O1, 1.196(7), C1−Bi1−C14, 92.5(2), C1/14−Bi1−C15, 88.9(2)/89.3(2); 10, Bi1−C1/10, 2.273(4)/2.273(5), Bi1−C11, 2.405(5), C11−O1, 1.211(7), C1−Bi1−C10, 101.80(17), C1/10−Bi1−C11, 87.94(16)/104.96(17). c UV/vis spectrum of 9 in CH2Cl2 (0.99 mm) and results from (TD)-DFT calculations (see text; isovalue = 0.03) performed at the ZORA-BLYP-D3(BJ)/TZ2P in THF (COSMO) level of theory. UV/vis = ultraviolet-visible, exp. = experimental, TD-DFT = time-dependent density functional theory, HOMO = highest occupied molecular orbital, LUMO = lowest unoccupied molecular orbital.

1H NMR spectra of compounds 9 and 10 show the expected signal pattern for the aryl substituents at bismuth and three signals for the adamantyl group in the aliphatic region. Broad resonances in the 13C NMR spectra at 253.81 (9) and 247.47 ppm (10) were assigned to the carbonyl carbon atoms. These signals show a considerable low-field shift when compared to those of lighter group 15 acyl compounds, e.g. Me2NC(O)Ad (177.0 ppm)52 or TeriPrPC(O)Ad (226.4 ppm, Ter = 2,6-bis-(2,4,6-trimethylphenyl)phenyl)53, which is ascribed to inefficient n(Bi)→π*(C=O) interactions due to poor orbital overlap in 9 and 10, as compared to the lighter pnictogen species. Yellow plate-shaped crystals of 9 and 10 were analyzed by single-crystal XRD (Fig. 3b). The bismuth atoms in compounds 9 and 10 show a trigonal pyramidal coordination geometry with Bi−Caryl bond lengths in the expected ranges. While the C−Bi−C angles in 9 are all close to 90° (88.9(2) to 92.5(2)°), the corresponding angles in 10 vary from 87.94(16) to 104.96(17)°, which was ascribed to the higher flexibility of the monodentate aryl ligands. The C=O bond lengths of 1.196(7) (9) and 1.211(7) Å (10) compare well to that in a closely related acyl phosphane (iPrTerPC(O)Ad; 1.2118(16) Å)53. In IR spectra of compounds 9 and 10, the C=O stretching bands were found at wave numbers of 1691 and 1690 cm–1, which are slightly larger than those reported for the acyl phosphane iPrTerPC(O)Ad (1653 cm–1)53 and the acyl arsane TMS2AsC(O)tBu (1667 cm–1)54. Again, this is in agreement with inefficient n(Bi)→π*(C=O) interactions compared to the analogous interactions in the P and As species.

The bismuth acyl structural motif was further investigated by a quantitative Kohn-Sham molecular orbital theory analysis in combination with a quantitative energy decomposition analysis, establishing a covalent character for the hitherto unknown Bi–acyl bonding in compounds 9 and 10 (Supp. Inf., pages S44-S46). Both electrostatic and orbital interaction attractive terms equally participate to this Bi-acyl interaction (45-46% of attractive interactions), with rather small contributions by dispersion interactions (8–9% of attractive interactions). A small charge transfer is observed from the SOMO of the [R2Bi] to the SOMO of the [C(O)adamantyl] fragment, which mainly involve the px(Bi) (dominant contributor) and px(C) (35%), s(C) (12%) and px(O) (31%) atomic orbitals of the CO functional group, respectively (Supp. Inf., page S46).

Experimental UV/vis spectroscopic measurements revealed broad absorption maxima at ca. 400 nm for both compounds (with a shoulder at higher wavelengths in the case of 9), which stretch into the region of visible light. For compound 9, TD-DFT calculations assign these bands to the HOMO-1 → LUMO and the HOMO → LUMO + 1 transitions (Fig. 3c and Supp. Inf., page S47). In particular, the aromatic backbone (HOMO-1, LUMO), the Bi–acyl group (HOMO, LUMO) and the acyl group (LUMO + 1) are involved in these transitions (for details on the analysis of 10, see Supp. Inf., page S47).

Indeed, the light-responsiveness of compound 9 could be translated into a highly selective chemical transformation. When a solution of 9 in toluene was stored at ambient temperature and ambient light for 24 h, a color change from yellow to colorless was observed. NMR spectroscopic investigations revealed the quantitative formation (spectroscopic yield >95%) of a new bismepine species with an adamantyl substituent. Additionally, a resonance at 184.5 ppm (in C6D6) was detected in the 13C NMR spectrum, indicating the release of carbon monoxide. Layering of the solution with n-pentane and storage at −30 °C led to the formation of colorless crystals, which were identified as the adamantyl-substituted bismepine 11 via single-crystal XRD (Fig. 4a,b). Compound 11, which results from a visible-light-induced CO extrusion of the starting material, was isolated in 83% yield and fully characterized. Since the formation of 11 was strongly impeded under exclusion of ambient light, we also investigated if the CO extrusion can be accelerated via irradiation with light of a suitable wavelength. Due to the broad absorption maximum at 400 nm in the UV/vis spectrum of 9, a blue LED with an emission maximum at 460 nm was chosen. Irradiation of a solution of 9 in CD2Cl2 for 25 min led to a complete discoloration. A 1H NMR spectrum of the solution confirmed the formation of 11 in 81% spectroscopic yield.

Fig. 4: Visible-light-induced reversible CO extrusion/insertion chemistry of acyl bismuthanes.
Fig. 4: Visible-light-induced reversible CO extrusion/insertion chemistry of acyl bismuthanes.
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a Light-induced CO extrusion of 9 and 10 in solution under formation of 11 and 12. *: Compound 12 was prepared and isolated in 20% yield using a different synthetic approach. rt = room temperature, LED = light-emitting diode, CD2Cl2 = dichloromethane-d2, Mes = mesityl = 2,4,6-trimethylphenyl. b Molecular structures of compound 11 (orthorhombic space group Pnma, Z = 4) and 12 (monoclinic space group P21/n, Z = 4) in the solid state. Displacement ellipsoids are shown at the 50% level. Hydrogen atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): 11, Bi1 − C1, 2.2557(19); Bi1 − C8, 2.308(2); C1 − Bi1 − C1’, 90.39(10), C1 − Bi1 − C8, 100.99(6); 12, Bi1 − C1, 2.281(4); Bi1 − C10, 2.297(3); Bi1 − C19, 2.347(3); C1 − Bi1 − C10, 97.88(13); C1 − Bi1 − C19, 92.98(12); C10 − Bi1 − C19; 118.09(13). c 13C{1H} NMR spectra (126 MHz) of 9 in CD2Cl2 30 min (bottom, blue) and 25 h (top, red) after 13CO was added. The resonance signal assigned to the carbonyl group of 9 is highlighted by a grey box. ppm = parts-per-million. d) Equilibrium reactions rationalizing the light-induced reactivity of 9 and 10 when exposed to 13CO.

Despite their similar spectroscopic properties, acyl bismuthane 10 did not show any signs of CO extrusion under ambient light, which is why more forcing photochemical conditions were examined. Irradiation of 10 in CD2Cl2 with a blue LED (λ = 460 nm) for 25 min led to the incomplete, but highly selective conversion into a new compound containing two mesityl units and one adamantyl group in 36% spectroscopic yield according to 1H NMR spectroscopy. This compound was identified as the CO extrusion product 12 through comparison of its NMR spectroscopic data with that of an independently prepared and fully characterized sample of 12 (Supp. Inf., page S9). Further irradiation under the same conditions, as well as other photochemical (LED λ = 365 nm or Hg vapor lamp) or thermal (60 °C, 50 h, in C6D6) conditions led to a partial and unselective decomposition of the starting material along with the formation of bismuth black51, which was ascribed to the lack of a stabilizing chelating ligand, the steric pressure in 12 (evidenced by an extremely large C–Bi–C angle of 118°, see Supp. Inf., page S12), and the negligible involvement of the aromatic backbone in lower energy photochemical processes (Supp. Inf., page S47). Tetramesityl dibismuthane, trimesityl bismuth, and mesitylene were identified as the main products via 1H NMR spectroscopy.

Previous reports about reversible CO extrusion and insertion in other main group compounds23,24,55 prompted us to investigate the reversibility of the formation of 11 and 12. Indeed, the reaction 9 → 11 + CO was calculated to show a Gibbs free energy close to zero (∆G = +0.4 kcal·mol–1 at the ZORA-BLYP-D3(BJ)/TZ2P level of theory), suggesting the possibility of an equilibrium scenario. The addition of CO (1.0 bar) to a solution of 11 in CD2Cl2 led to the formation of minor amounts (ca. 6%) of 9 after 4 d, according to 1H NMR spectroscopy indicating a partial reversibility and suggesting a thermodynamic equilibrium. Longer reaction times, higher temperatures (up to 40 °C), or Lewis basic solvents such as THF did not increase the yield considerably, while exclusion of light impeded the reaction. The addition of CO (1.0 bar) to a solution of 12 in CD2Cl2 resulted in an unselective and incomplete reaction. The formation of 10 (in ca. 10% spectroscopic yield) was confirmed by 1H and 13C{1H} NMR spectroscopy, as well as mass spectrometry, proving the reversibility of the CO extrusion, albeit with lower selectivity than in the case of compounds 9/11 (see Supp. Inf., page S22).

To gain further insights into the reversibility of CO extrusion/insertion, exchange experiments with 13C-labeled carbon monoxide were performed. 13CO (1.5 bar) was added to solutions of 9 and 10 in CD2Cl2, the samples were stored under ambient light at room temperature and the reactions monitored via 1H and 13C{1H} NMR spectroscopy (for more details see Supp. Inf., pages S23-S26). For compound 9, a sixfold increase of the intensity of the 13C NMR spectroscopic resonance assigned to its carbonyl group was observed after 25 h (Fig. 4c), despite approximately 65% of the starting material having undergone CO extrusion. While CO extrusion still occurs under an atmosphere of (13)CO, it does so at a slower rate and without complete consumption of the starting material (approximately 16% of 9 remain, even after 16 d). These findings can be rationalized by an equilibrium between 9 and 11 + CO, where the CO extrusion is favored, even under an atmosphere of CO (as suggested in Fig. 4d). In the 13C{1H} NMR spectra of the reaction of 10 and 13CO the increase of the intensity of the resonance signal of the carbonyl group was even more noticeable, since no CO extrusion occurs under ambient light (for more details see Supp. Inf., page S27). Reversible (13)CO insertion/extrusion was further proved by the appearance of the resonances for the tertiary carbon atoms of the adamantyl group in [Bi]–13C(O)adamantyl as doublets (1JCC = 23 Hz (9’), 22 Hz (10’)) in the 13C NMR spectra of these experiments.

In conclusion we have established the reliable access to simple monoanionic diaryl bismuthides, [BiR2]. Via a synthetic strategy of polarity inversion, these compounds grant access to complexes featuring the bismuth–acyl structural motif, R2Bi–C(O)alkyl, introducing this functional group to synthetic chemistry. Exploiting the light-responsive nature of organobismuth species, this functional group paved the ground to the visible-light-driven reversible insertion and extrusion of carbon monoxide with a well-defined organometallic main group compound. While the polarity inversion approach brings previously inaccessible synthetic strategies and unknown functional groups into reach, the bismuth-acyl species promise the future exploitation of visibile-light-driven carbonyl insertion/extrusion reactions and catalysis with state-of-the art main group complexes.

Methods

Representative methods are given below. More detailed information including all analytical data are presented in the Supplementary Information.

Synthesis of 5

Potassium graphite (KC8, 87 mg, 646 μmol) was added to a suspension of dibismuthane 1 (250 mg, 323 μmol) and [2.2.2]cryptand (243 mg, 646 μmol) in THF (10 mL). The reaction mixture was stirred at rt for 1 min and then filtered. The filtrate was layered with n-pentane (10 mL) and stored at −30 °C. After 1 d dark orange crystals of 5 had formed, which were isolated by filtration, washed with n-pentane (3 ×3 mL) and dried in vacuo. Yield: 436 mg, 543 μmol, 84%.

Synthesis of 9

A solution of 1-adamantanecarbonyl chloride (99 mg, 498 μmol) in THF (4 mL) was added to a suspension of bismuthide 5 (400 mg, 498 μmol) in THF (10 mL). The yellow suspension was filtered and all volatiles removed under reduced pressure. The residue was extracted with a mixture of toluene (4 mL) and THF (10 mL), layered with n-pentane (8 mL) and stored at −30 °C. After 3 d yellow crystals of 9 had formed, which were isolated by filtration, washed with n-pentane (3 ×2 mL) and dried in vacuo. Yield: 170 mg, 309 μmol, 62%.

13CO exchange experiments

In a J. Young NMR tube, 9 (30 mg, 55 μmol) was dissolved in CD2Cl2 (0.5 mL). The atmosphere above the solution was exchanged with 13CO (1.5 bar) via three freeze/pump/thaw cycles. The reactions were monitored via 1H and 13C{1H} NMR spectroscopy and the samples stored at room temperature between each measurement.