Introduction

The current utilization of dinitrogen (N2) predominantly relies on the Haber-Bosch process, also known as ammonia (NH3) synthesis1,2,3. Over the past six decades, the N−H bond formation facilitated by homogenous transition metal catalysts via associative and dissociative pathways has been extensively studied4,5,6,7,8,9,10,11,12,13. Typical pathways for synthesizing NH3, such as the Chatt14 and Schrock15 cycles, along with studies by Nishibayashi16 and Peters17, have been successively proposed. However, developing methods for the direct dinitrogen-element (N−E) bond formation beyond NH3 lags behind and remains a longstanding and challenging issue18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38. The formation of diazenido and hydrazido intermediates in associative pathways is pivotal for constructing N−E bonds, but two major scientific challenges remain unresolved. Firstly, diazenido intermediates formed via the initial electrophilic functionalization of coordinated N2 tend to decompose, especially with 3 d metals, through N−H and N−Si homolytic cleavage, β-silyl elimination or other unclear pathways (Fig. 1a)26,29,30,39,40,41,42. Secondly, the thermolabile nature of methyl-, silyl-, germyl-, and phosphanyldiazenes complicates the isolation of diazenido compounds containing N−C, N−Si, N−Ge, and N−P bonds (Fig. 1a)43,44,45. To address the above issues, we draw inspiration from nitrogenase, which features a multi-metallic active site surrounded by crucial amino acid residues that polarize N2 and enhance charge transfer from the iron center to N246,47,48. Using both transition-metal complexes and Lewis acids (LA) to co-activate N2 thus represents a promising approach18,19,20,21,22,23,24,25,28,49,50,51,52,53,54,55,56,57,58, but further electrophilic derivatizations of the coordinated N2 using Lewis acids remain extremely limited22,28,54. In this work, we present a Lewis acid-promoted strategy for forming N−C, N−Si, N−Ge, and N−P bonds. More accessible conditions for N−C bond formation were achieved by inhibiting undesired side reactions59 at the Cr(0) center (Fig. 1b, top). Furthermore, we use Lewis acids to trap and stabilize a series of fleeting diazenido intermediates containing N−B, N−Si, N−Ge, and N−P bonds (Fig. 1b, below), confirming the feasibility of the initial step of electrophilic derivatization of Cr-N2 complexes to form various N−E bond-containing diazenido complexes.

Fig. 1: N−E bond formation via associative pathways.
figure 1

a Challenges for diverse N−E bonds formation via diazenido complexes. b N−E bond formation beyond N−H bond promoted by Lewis acids. LA Lewis acid.

Results

Synthesis and characterization

Considering that the Nβ atom in diazenido intermediates is already sp2-hybridized with a lone pair of electrons60,61, we hypothesized that additional Lewis acids might trap and stabilize such intermediates (Fig. 1b, below). As given in Fig. 2A, this idea was validated by adding 1.0 equiv of AlMe3 or BF3•Et2O to the proposed fleeting diazenido intermediates [Cp*(IiPr2Me2)Cr(NNSiMe3)] (formed in situ by reaction of [Cp*(IiPr2Me2)Cr(N2)2]K(sol) 1-K and 1.0 equiv of Me3SiCl, sol = THF or Et2O, IiPr2Me2 = 1,3-diisopropyl-4,5-dimethylimidazol-2-yildene, Fig. 2A, left) at low temperature, resulting in the Lewis acid trapped products 2a and 2b. Both 2a and 2b are paramagnetic and have a solution magnetic moment of 2.4(1) μB and 2.7(1) μB at 296 K, respectively. X-ray crystallography reveals that compared with the diazenido [Cp*(IiPr2Me2)Cr(NNSiiPr3)] (1.243(2) Å for N−N bond)35, the N−N distances in 2a and 2b are significantly elongated, with lengths of 1.3060(17) Å and 1.3108(17) Å, respectively (Fig. 2B).

Fig. 2: Synthesis and molecular structures of complexes 2, 3, 4, 6 and 7.
figure 2

A Synthesis of complexes 2a, 2b, 3, 4, 6 and 7. B Molecular structure of 2a, 2b, 3, 4, and 6 with thermal ellipsoids at 30% probability. H atoms omitted for clarity. Selected bond lengths [Å] and angles [deg] of 2a: Cr1-N3 1.6801(3), N3−N4 1.3060(17), N4−Al1 1.9659(17), N3−N4−Si1 111.98(11); 2b: Cr1-N3 1.6768(13), N3−N4 1.3108(17), N4−B1 1.574(2), N3−N4−Si1 115.34(10); 3: Cr1-N3 1.684(2), N3−N4 1.295(3), N4−B1 1.574(4), N3−N4−Ge1 116.27(18); 4: Cr1−N3 1.6753(11), N3−N4 1.3144(16), N4−B1 1.581(2), N3−N4−P1 113.47(10); 6: Cr1–N3 1.7104(17), N3–N4 1.231(2), N4–B1 1.423(3), N3–N4–B1 138.56(19).

It should be pointed out that N−Ge or N−P bond-containing complexes cannot be synthesized from 1-K because undesired redox reactions always arise during the direct functionalization of 1-K with Me3GeCl or iPr2PCl, leading primarily to [Cp*(IiPr2Me2)CrCl] and [Cp*(IiPr2Me2)Cr(ƞ1-N2)(µ-ƞ1:ƞ1-N2)Cr(IiPr2Me2)Cp*]. To our delight, the method used to prepare 2a and 2b provides an opportunity to isolate Lewis acid-stabilized species 3 and 4 (Fig. 2A, left). Both 3 and 4 are paramagnetic and have a solution magnetic moment of 2.4(1) μB and 2.7(1) μB at 296 K, respectively. The N−N bond lengths of 3 (1.295(3) Å) and 4 (1.3144(16) Å) also lie between the values for a N−N single bond (1.46 Å for H2NNH2) and a N = N double bond (1.25 Å for HN = NH) (Fig. 2B). These results indicate that the Lewis acids can effectively trap fleeting diazenido intermediates and prevent undesired side reactions.

B and Al-based electrophiles, unlike their Si, Ge, and P counterparts, possess an extra empty p orbital, making them capable of acting as Lewis acids. Therefore, when reacting with N2 complexes, the products often display a dinuclear structure, as seen in forms such as [(MNNBR2)2]23 and [(MNNAlR2)2]36,50. In fact, the dinuclear complex 7 can be obtained during the reaction of complex 1-K with 1.0 equiv Et2AlCl (Fig. 2A, right), although obtaining high-quality data for 7 has been challenging. The reaction between 1-K and common B-based electrophiles (Cy2BCl, Ph2BCl, Mes2BF) does not result in boryldiazenido intermediates, but instead leads to side reactions, such as single electron transfer or the dissociation of IiPr2Me2. Fortunately, treatment of 1-K with the more electron-rich boron electrophile 5 yields the boryl-functionalized diazenido complex 6 (Fig. 2A, right). Compound 6 is paramagnetic and has a solution magnetic moment of 2.8(1) μB at 296 K. The Cr1−N3 bond length of crystal 6 (1.7104(17) Å) is shorter than the typical single bond, indicating a multiple bond characteristic. The N−N bond distance (1.231(2) Å) is in the range of the typical N = N double bond, and the N3−N4−B1 angle (138.56(19)°) suggests an sp2 hybridized geometry for the Nβ atom. The N4−B1 bond length (1.423(3) Å) is shorter than complexes 2b, 3, and 4, indicating N4−B1 bond is a covalent bond with multiple B−N bonding (Fig. 2B). The presence of an empty p orbital on the B atom, along with the significant steric hindrance, are crucial for stabilizing and isolating this diazenido product. The strong vibration peak at 1602 cm−1 in IR spectra of 6 is assigned to N−N vibration of the η1-diazenide fragment. A 15N−15N stretching vibration at 1540 cm−1 of the 15N2-labeled sample of 6 is consistent with the mass difference between 15N2 and 14N2 (Fig. S6).

To elucidate how Lewis acids stabilize those Cr diazenido intermediates, 2b was analyzed using density functional theory (DFT) calculations as an example. Significant energy release (ΔG = −24.6 kcal/mol) from the corresponding Cr diazenido and BF3•THF to 2b indicates a strong driving force for the Lewis acid coordination and the enhanced stability of complex 2b. Moreover, Fuzzy bond order (FBO) analysis shows that the FBO of N−N bonds decreases from 1.9 to 1.6 after BF3 coordination, accompanied by Cr−N bond shortening (Fig. 3), consistent with the strong activation effect of Lewis acid on diazenido complexes62. Mayer bond orders and Wiberg bond indices (WBI) are also provided (see Fig. S41 for details), and the trends are qualitatively consistent.

Fig. 3: DFT calculations.
figure 3

Fuzzy bond orders (blue) and Hirshfeld atomic charges (orange) for [Cp*(IiPr2Me2)Cr(NNSiMe3)] (left) and 2b (right). Wavefunctions were generated at the PWPB95/def2-QZVPP level of theory.

We have recently reported several N2 functionalization reactions utilizing mono/bis-phosphine or NHC-appended cyclopentadienyl Cr−N2 complexes, yielding N−H, N−C, N−Si bonds, and hetero-bimetallic Cr−N2 complexes29,33,35,63,64. However, setbacks arose when employing mono-phosphine or NHC-appended cyclopentadienyl Cr−N2 complexes to investigate N−C bond formation. Direct functionalization of complex 1-K with MeOTf, MeOTs, Me3OBF4, or MeI did not yield N−C bond products. In addition, our afore-mentioned reaction processes given on the left of Fig. 2A involving the reaction of 1-K with MeOTf followed by adding Lewis Acid BEt3 produced only very few crystals of the N−C bond formation product [(Cp*(IiPr2Me2)CrNN(BEt3)(Me)] (8). Hence, we speculated that an alternative strategy would be needed for making N−C bonds. After experimenting, we found that the order of adding LA (Lewis acids) and EX (electrophiles) had a remarkable effect on the N−C bond formation. Thus, treating 1-crypt with 1.0 equiv of BEt3 or AlMe3 led to two new vibration peaks (Fig. 4C, left, red line at 1738 cm−1, 1900 cm−1 for BEt3 and blue line at 1755 cm−1, 1911 cm−1 for AlMe3) accompanied by incomplete conversion of 1-crypt. These two new peaks are assigned as N2-related peaks because the corresponding 15N peaks with BEt3 were at 1685 cm−1 and 1838 cm−1 (for details, see Figure S10), suggesting an equilibrium between 1-crypt and the Lewis acids adducts may exist. The reduced N2 stretching, indicative of lower bond order and increased polarization, is reminiscent of the effect of acidic residues in nitrogenase active sites on Fe-bound N2, which enhance polarization and facilitate protonation. This inspired further addition of MeOTf to explore N−C bond formation. Fortunately, complex 8 was successfully isolated this time (Fig. 4A). Complex 8 is paramagnetic and has a solution magnetic moment of 3.2(1) μB at 296 K. The N−N bond length of crystal 8 is 1.289(2) Å, reflecting the strong interaction between the empty boron p-orbital and the N2 π* orbital. The N3−N4−B1 angle is 124.01(17)°, suggesting sp2 hybridization of the Nβ atom with a dative coordinated boron atom (Fig. 4B). Furthermore, we found that complexes 2a, 2b, 3, and 4 could also be synthesized using this method.

Fig. 4: Synthesis and mechanistic investigations.
figure 4

A Synthesis of complexes 2a, 2b, 3, 4, and 8. B Molecular structure of 8 with thermal ellipsoids at 30% probability. H atoms omitted for clarity. Selected bond lengths [Å] and angles [deg] of 8: Cr1−N3 1.6902(16), N3−N4 1.289(2), N4−B1 1.618(3), N3−N4−C22 114.19(18). C Variation of vibration peaks during adding Lewis acids to 1-crypt.

To investigate the role of Lewis acids in the above-discussed N−C bond formation, we conducted experiments to verify the interaction between BEt3 and 1-crypt. When we added 2.0 equiv of BEt3 to the solution of 1-crypt, the peaks at 1738 cm−1 and 1900 cm−1 were significantly enhanced (see Fig. 4C, right, red line for 1.0 equiv BEt3 and green line for 2.0 equiv BEt3). This suggests an equilibrium between 1-crypt and 10-BEt3, with 1-crypt favoring reaction with two equivalents of BEt3 (Fig. 4A). The coupling vibration of two [NNBEt3] substituents shifts one peak to lower frequencies and the other to higher frequencies. In addition, two new peaks (385 and 416 ppm), distinct from 1-crypt (404 and 413 ppm), were observed in the in situ 15N NMR spectra of 1-crypt with 2.0 equiv. BEt3. The Δδ for Cr-bound and terminal N atoms increases from 9 to 31 ppm, indicating polarization of N2 unit but less than Szymczak’s Fe-N2 system (Δδ = 109 ppm)54. This result is consistent with smaller IR shifts (1780, 1869 cm⁻¹ to 1738, 1900 cm⁻¹). The calculated stretching vibration peaks for the NN bond in the IR spectrum are 1779 cm−1 and 1878 cm−1 for 1-crypt, and 1752 cm−1 and 1917 cm−1 for 10-BEt3, which are in good agreement with experimental values. DFT calculations show that the ΔG value for 1-crypt coordination with one equivalent of BEt3 in THF at −30 °C is +0.7 kcal/mol, whereas coordination with two equivalents is −0.8 kcal/mol, confirming the equilibrium between 1-crypt and 10-BEt3. AIM (atoms in molecules) analysis of 10-BEt3 confirms dative B–N interactions (see Figure S42 for details). Moreover, BEt3 coordination significantly enhances the participation of the N₂ moiety in HOMO (Orbitals contributions in HOMO: Nα 13.8%, Nβ 20.2%, Cr 34.5% for 10-BEt3 and Nα 7.1%, Nβ 12.0%, Cr 46.1% for 1-crypt, see Figure S43 for more details). This enhancement increases the likelihood of NN unit participation in functionalization and reduces the side reactions between Cr and electrophilic reagents.

Interestingly, coordination of two BEt₃ molecules lowers the activation barrier for functionalization with MeOTf (18.7 to 15.6 kcal/mol), while it increases with one BEt₃ (18.7 to 22.3 kcal/mol), consistent with the higher yield of 8 using 2.0 equiv. BEt₃. Therefore, the primary role of BEt₃ is to mitigate undesirable side reactions between MeOTf and the Cr center to some extent. Furthermore, once the N−C bond is formed, BEt3 does not dissociate, stabilizing the CrNNMe framework and preventing its rapid decomposition. Diazenido intermediates stabilized by Lewis acid coordination exhibit characteristic UV-Vis absorption peaks around 620 nm (Figures S23S29). Due to the structural similarity of these complexes, 2b was chosen as a representative for TD-DFT calculations to simulate its UV-Vis spectrum. NTO analysis reveals that the absorption peak around 620 nm primarily arises from π to π* excitation within the CrNN unit (Figure S44).

Further transformations of these Lewis acid-coordinated products were explored. However, the reactions of 2b with CO2, tBuNCO, PhSiH3, nBu3SnH, DIBAL-H or KC8 did not yield any clear N-containing products yet. Encouragingly, the coordinated BEt3 in 8 can initiate two distinct reaction pathways with a Lewis acid or base. First, BEt₃ can be replaced by AlMe₃, forming 9, with no significant structural changes observed after Lewis acid substitution (Fig. 5). Second, the removal of BEt3 by IMe4 (1,3-dimethyl-4,5-dimethylimidazol-2-ylidene) induces a transition of the [NNMe] moiety from end-on to side-on coordination, yielding the bis-side-on [NNMe]-coordinated complex 11 (Fig. 5). The N−N distance increases from 1.289(2) Å to 1.387(2) and 1.389(2) Å, indicating a greater potential for further conversion of the [NNMe] fragment.

Fig. 5: Further transformation of complex 8.
figure 5

Selected bond lengths [Å] and angles [deg] of 9: Cr1−N3 1.694(2), N3−N4 1.286(3), N4−Al1 1.944(2), N3−N4−Al1 121.28(16); 11: N1−N2 1.389(2), N3−N4 1.387(2), N1−N2−C1 119.39(15), N3−N4−C2 119.42(17).

Functionalization of N2 with electrophiles often requires strict low-temperature conditions to prevent undesired side reactions29. Given its success in evading undesired redox reactions to form N−E bonds, we persisted in investigating the potential of more accessible reaction conditions. UV−Vis measurements revealed that two bands (463 nm, 654 nm) attributed to complex 8 emerged when 1.0 equiv BEt3 and 1.0 equiv MeOTf were added to 1-crypt successively at −30 °C, 0 °C and 20 °C (for details, see Figures S30S32). Based on these results, we conducted a 0.05 mmol scale reaction at approximately room temperature, confirming the formation of 8, albeit with difficulty in determining the yield.

In summary, we have synthesized a series of N−E (E = B, C, Si, Ge, P) bond-containing complexes from N2 with the aid of Lewis acids, offering a potential approach for isolating N−B, N−Ge, N−P bond-containing compounds in 3 d metals. Extra Lewis acids not only suppress undesirable side reactions, but also provide possibilities for more accessible reaction conditions. Moreover, a end-on to side-on switch of [NNMe] unit is achieved, creating greater opportunities for N2 transformations. We hope this study will facilitate the development of more manageable and diverse N2 functionalization reactions.

Methods

General procedure for the synthesis of Lewis acids stabilization complexes

Conditions A

In a nitrogen atmosphere glovebox, excess KC8 (0.3 mmol, 40.5 mg) was added into the THF (6 mL) solution of complex Cp*Cr(IiPr2Me2)Cl (0.1 mmol, 40.3 mg). The solution was stirred for 24 h at room temperature, generating the Cr(0)-N2 complex 1-K, as evidenced by two peaks (1760 cm−1, 1846 cm−1) in the IR spectra. The solvent was filtered, and the filtrate was concentrated to approximately 4 mL before adding 2 mL of Et2O. The solution was frozen in the coldwell chilled externally with liquid nitrogen. Meanwhile, a solution of Lewis acids (0.1 mmol) in hexane or Et2O was also frozen in the coldwell chilled externally with liquid nitrogen. Immediately upon thawing, the solution of Lewis acids was added to the frozen 1-K equipped with a magnetic stirring bar. The solution was slowly warmed to −70 °C while stirring for 30 min. Then the reaction solution was frozen in the coldwell chilled externally with liquid nitrogen again. Meanwhile, a solution of electrophile (EX) (0.1 mmol) in THF was also frozen in the coldwell chilled externally with liquid nitrogen. Immediately upon thawing, the solution of electrophile was added to the frozen reaction solution. The solution was slowly warmed to −30 °C while stirring for 70 min. Volatile materials were removed under vacuum. The solid residues were extracted with hexane/Et2O or Et2O/THF. The filtrate was concentrated and placed in a −30 °C freezer, yielding crystals.

Conditions B

In a nitrogen atmosphere glovebox, excess KC8 (0.3 mmol, 40.5 mg) was added into the THF (6 mL) solution of complex Cp*Cr(IiPr2Me2)Cl (0.1 mmol, 40.3 mg). The solution was stirred for 24 h at room temperature, generating the Cr(0)-N2 complex 1-K, as evidenced by two peaks (1760 cm−1, 1846 cm−1) in the IR spectra. The solvent was filtered, and the filtrate was concentrated to approximately 4 mL before adding 2 mL of Et2O. The solution was frozen in the coldwell chilled externally with liquid nitrogen. Meanwhile, a solution of electrophile (EX) (0.1 mmol) in THF was also frozen in the coldwell chilled externally with liquid nitrogen. Immediately upon thawing, the solution of electrophile was added to the frozen 1-K equipped with a magnetic stirring bar. The solution was slowly warmed to −70 °C while stirring for 30 min. Then the reaction solution was frozen in the coldwell chilled externally with liquid nitrogen again. Meanwhile, a solution of Lewis acids (0.1 mmol) in hexane or Et2O was also frozen in the coldwell chilled externally with liquid nitrogen. Immediately upon thawing, the solution of Lewis acids was added to the frozen reaction solution. The solution was slowly warmed to −30 °C while stirring for 70 min. Volatile materials were removed under vacuum. The solid residues were extracted with hexane/Et2O or Et2O/THF. The filtrate was concentrated and placed in a −30 °C freezer, yielding crystals.

Computational details

Density functional theory (DFT) calculations were performed using ORCA 6.0.0 to investigate the electronic structures65. All geometric structures were optimized at the TPSSh/ def-TZVP level of theory66, incorporating dispersion corrections via the Becke-Johnson damping scheme (D3BJ)67. The optimized geometries closely match the single-crystal structures, supporting the validity of the computational approach. Additionally, to further ensure accuracy, we conducted single-point energy calculations on the optimized geometries using the double-hybrid functional PWPB95 with def2-QZVPP basis sets68. Solvent effects were considered by employing the SMD implicit solvent model with tetrahydrofuran (THF) as the solvent in these single-point calculations69. UV-Vis spectrum of 2b was computed using the long-range-corrected DFT functional CAM-B3LYP70 with the def2-TZVP basis sets based on the optimized geometric structure using the Gaussian 16 package71. We have carefully validated the spin states of all paramagnetic species, ensuring that the computed electronic structures are physically meaningful. The figures were prepared by Visual Molecular Dynamics (VMD) program72, and the corresponding wavefunction analysis was performed by Multiwfn73.