Abstract
Ammonia, NH3, is an essential molecule, being part of fertilizers. It is currently synthesized via the Haber–Bosch process, from the very stable dinitrogen molecule, N2 and dihydrogen, H2. This process requires high temperatures and pressures, thereby generating ca 1.6 % of the global CO2 emissions. Alternative strategies are needed to realize the functionalization of N2 to NH3 under mild conditions. Here, we show that boron‐centered radicals provide a means of activating N2 at room temperature and atmospheric pressure whilst allowing a radical process to occur, leading to the production of borylamines. Subsequent hydrolysis released NH4 +, the acidic form of NH3. EPR spectroscopy supported the intermediacy of radicals in the process, corroborated by DFT calculations, which rationalized the mechanism of the N2 functionalization by R2B radicals.
Keywords: Boron Radical, Density-Functional Calculations, N2 Fixation, Reaction Mechanims, Reduction
Boron‐centered radicals, generated by reduction of R2BCl derivatives, react with N2 all the way to borylamine formation. DFT calculations rationalize the reduction/functionalization process, involving N−N bond splitting. Hydrolysis of the mixture yields NH4 +. Radical addition to N2 provides a new strategy for N2 fixation.
Introduction
Ammonia is one of the most abundantly produced chemicals worldwide. This compound is an essential component of fertilizers, providing nitrogen for plants to grow. Without fertilizers, the growing world's population could not be fed. Currently, 150 million t/y of NH3 is produced worldwide; this figure is expected to more than double by 2050. [1] Ammonia is also a promising material as a transportation fuel. [2] Ammonia is a prime candidate for energy storage in the hydrogen economy. Indeed, the energy density of liquid ammonia (11.5 MJ L−1), is higher than for liquid hydrogen (8.491 MJ L−1) and for compressed H2 at 690 bar and 15 °C (4.5 MJ L−1). [3]
Around 78 % of our planet's atmosphere is made up of nitrogen gas (N2) but its activation and conversion to NH3 remains a challenging task due to the inertness of the dinitrogen. Plants have developed mechanisms to activate and fix nitrogen from N2 using nitrogenase enzymes, but the process is slow and does not lend itself to industrialization. The industrial production of NH3 uses the Haber–Bosch (HB) process, during which hydrogen and nitrogen react at a high temperature and pressure over a metal catalyst.[ 4 , 5 ] The process uses natural gas as raw material and has a heavy CO2 footprint of 1.9 t of CO2 per t NH3. The HB process contributes 1.4 % of the world's CO2 emissions. [6] The process can only be run economically in large, capital‐intensive units.
Decarbonizing the HB process can potentially be done by sequestering and storing the generated CO2, [7] or by using the hydrogen gas produced by water splitting from renewable energy. [8] However, the primary step of the process—the actual HB ammonia production—remains energy and capital intensive. The process does not lend itself easily to medium‐sized production units that are aimed at using locally available renewable energy.
A clear need exists for a process to convert nitrogen to ammonia without the use of high temperatures and high pressures.
Researchers have been looking into developing processes for N2 transformation into N‐containing derivatives (i.e., N2 fixation) under mild, homogeneous conditions for several decades, especially processes that use carefully designed transition metal complexes (Figure 1, A). [9] The classical method for N2‐activation at a metal center relies on a two‐way electron flow. Donation of electron density from N2 to an empty orbital at the metal and back donation from a filled orbital of the metal to π* orbitals of N2, weakens the strong N≡N bond.[ 10 , 11 , 12 , 13 , 14 ] Despite impressive results obtained recently, only a few complexes have been demonstrated to efficiently reduce N2 to NH3 using carefully optimized sources of protons and electrons.[ 15 , 16 , 17 ] Notably, this strategy was successfully applied most recently to main group boron species (borylene derivatives).[ 18 , 19 , 20 ]
Figure 1.

A: Known catalytic N2 to NH3 transformations. B: Radical approach to N2‐activation: our strategy. C: Computed additions of R2B radicals on N2. D: Successful N2 to NH4 + transformation via B‐centered radicals.
On the other hand, theoretical calculations show that the incorporation of N2 can take place in some organic molecules.[ 21 , 22 ] The lack of experimental proof demonstrating the feasibility of such a direct insertion process is obviously due to kinetic limitations, i.e., the involvement of high‐energy transition states and intermediates.
For example, the addition of H2 across N2 to afford NH3 implies the formation of diazene, HN=NH, as the first intermediate. Although this step leads to the formation of two strong NH bonds, calculations show that the reaction is far too endothermic to become feasible (ΔH°=56.0 and 51.0 kcal mol−1 for cis and trans diazene, respectively).
We reasoned that the use of high‐energy radicals might provide a kinetically and thermodynamically favorable pathway to N2 functionalization. The reaction between N2 and the high‐energy radical H⋅ is, however, known to be endothermic (ΔH°=9.0 kcal mol−1), which precludes a radical chain process initiated by H atom transfer. [23] To develop the first N2 functionalization process based on radical addition, we performed a computational study (using density functional theory, DFT) to identify radicals (R⋅) forming compounds of the type RN2⋅ in an exothermic (and exergonic) reaction (Figure 1C). We inferred that, in addition to creating a strong σ‐interaction, delocalization of the radical onto the π* system of N2 could be the key to such an exergonic process (Figure 1B). [24] Calculations, therefore, focused on various R2B⋅ derivatives. Experimental work was subsequently dedicated to generating such radicals under mild conditions. We report here the first functionalization of N2 with three radical derivatives, namely Cy2B⋅, (DIP)B⋅ (DIP=Di‐isopinocampheyl) and Bis(bicyclo[2.2.1]‐2‐heptyl)B⋅, generated at room temperature in the presence of potassium (K). NMR and EPR spectroscopies and DFT calculations have unambiguously established the in situ formation of borylamines from N2 and boron‐centered radicals. NH4 + was then obtained by simple hydrolysis of the borylamine intermediates, thereby providing an unprecedented strategy for the transformation of dinitrogen to ammonia under mild conditions.
Results and Discussion
Reaction Optimization: NH4 + Synthesis from N2
As a first step, the additions of CatB⋅ (Cat=catechol) and Cy2B⋅ on N2 were computed by DFT (Figure 1, C). [25] Both radicals are computed to have an exothermic (ΔH=−16.9 kcal mol−1, CatB; ΔH=−32.1 kcal mol−1, Cy2B) and exoergic (ΔG=−7.5 kcal mol−1, CatB; ΔG=−22.1 kcal mol−1, Cy2B) reaction with N2. According to these calculations, both radicals were promising candidates to react with N2 and we set out to generate them in solution under N2 upon one‐electron reduction of the corresponding R2BCl derivative. It should be noted, however, that few R2B−BR2 compounds are known to be synthesized via this reductive strategy under N2, implying favored radical coupling rather than addition on N2.[ 26a , 26b , 26c ] The efficiency of the BB bond formation appeared to depend on the substituents at B, with the presence of donor atoms being very favorable. [27] The donor atoms likely stabilize the radical, thereby increasing its concentration and thus the radical coupling. Accordingly, several (RO)2B−B(OR)2 compounds have been synthesized in good to excellent yields from (RO)2BCl and Na/Hg under N2 in toluene at 90 °C. [28] Therefore, the reduction of Cy2BCl to form a higher‐energy non‐stabilized boryl radical was chosen as the more promising candidate. [29] Thus, as a preliminary investigation a stoichiometric mixture of Cy2BCl and K (2.0 mmol) in THF (12 mL) was stirred for 12 h under N2 (1 bar), followed by hydrolysis with an excess of HCl in Et2O to convert all N containing species into NH4Cl. Quantification was achieved by dissolution of the solid residue and integration vs. 1,3,5‐trimethoxybenzene as internal standard by 1H NMR spectroscopy (see ESI for details on the quantification method). It revealed that NH4 + is indeed produced, albeit in a small yield (0.046 mmol, 7 % yield, Table 1, entry 1). Further studies then showed that this yield could be significantly improved, up to 41 %, by lowering the concentration of the reagents and by using an excess of K (entry 2). A thorough screening of solvents and reducing agents was carried out under these conditions.
Table 1.
Exploring the reaction parameters: step 1) N2+R2BCl+x red. (6 h, solvent, temperature, N2 pressure); step 2: hydrolysis with excess HCl; step 3 quantification of NH4 +. Standard reaction conditions: 0.16 mmol Cy2BCl unless otherwise specified; stirring at 700 rpm at room temperature for 6 h, open flask in glove box. Yield is calculated as 3×n(NH4 +)/n(Cy2BCl)×100 thus considering only N(BCy2)3 to be formed during the reaction (see text). All reactions were reproduced at least twice (entry 2, done 6 times). Yield accuracy was estimated at ±4 %.
|
|
[R2BCl] [mol L−1] |
Solvent |
Reducing agent |
Stoich. Red |
PN2 [bar] |
Yield |
|---|---|---|---|---|---|---|
|
1 |
0.17 |
THF |
K |
1 |
1 |
7 |
|
2 |
0.04 |
THF |
K |
2.5 |
1 |
41 |
|
3 |
0.04 |
MeTHF |
K |
2.5 |
1 |
0 |
|
4 |
0.04 |
Pentane |
K |
2.5 |
1 |
0 |
|
5 |
0.04 |
Toluene |
K |
2.5 |
1 |
0 |
|
6 |
0.04 |
Et2O |
K |
3.3 |
1 |
0 |
|
7 |
0.04 |
Dioxane |
K |
3.3 |
1 |
Trace |
|
8 |
0.04 |
THF |
Na |
2.5 |
1 |
0 |
|
9 |
0.04 |
THF |
Na/Hg |
2.5 |
1 |
0 |
|
10 |
0.04 |
THF |
Na/naphtalene |
2.5 |
1 |
0 |
|
11 |
0.04 |
THF |
KC8 |
2.5 |
1 |
0 |
|
12 |
0.04 |
THF |
SmI2 |
2.5 |
1 |
0 |
|
13[a] |
0.04 |
THF |
K |
2.5 |
1 |
0 |
|
14[b] |
0.04 |
THF |
K |
2.5 |
1 |
0 |
|
15[c] |
0.02 |
THF |
K |
2.5 |
1 |
56 |
|
16 |
0.02 |
THF |
K |
1 |
1 |
30 |
|
17[d] |
0.04 |
THF |
K |
2.5 |
1 |
56 |
|
18 |
0.04 |
THF |
K |
2.5 |
20 |
60 |
|
19 |
0.04 |
THF |
K |
2.5 |
40 |
76 |
|
20 |
0.04 |
THF |
K |
2.5 |
80 |
94 |
|
21[e] |
0.04 |
THF |
K |
2.5 |
1 |
48 |
|
22[f] |
0.08 |
THF |
K |
2.5 |
1 |
38 |
|
23[g] CatBCl |
0.04 |
THF |
K |
2.5 |
1 |
0 |
|
24[h] DIP‐Cl |
0.04 |
THF |
K |
2.5 |
1 |
28 |
|
25[i] BCHBCl |
0.04 |
THF |
K |
2.5 |
1 |
43 |
[a] reaction at 60 °C; [b] reaction at −70 °C; [c] reaction conducted on a 0.08 mmol scale; [d] K was cut into 5 pieces; [e] reaction conducted on a 10 times scale compared to standard; [f] reaction conducted on a 100 times scale compared to standard; [g] CatBCl=catechol‐chloroborane; [h] DIP‐Cl=Di‐isopinocampheyl‐chloroborane; [i] BCHBCl=Bis(bicyclo[2.2.1]‐2‐heptyl)chloroborane.
No NH4 + production was observed in toluene, Et2O, pentane or 2Me‐THF, no matter what the reducing agent was, while trace amounts were observed in 1,4‐dioxane (entries 3–7). We then tested the use of several strong one‐electron reducing agents, such as Na, Na/Hg, Na/naphthalene, KC8 and SmI2 in THF. Despite the fact that the chloroborane is reduced, as attested by the formation of BH species in the crude mixture by 11B NMR (vide infra), in none of cases, NH4 + was observed after hydrolysis of the crude mixture (entries 8–12). To ascertain that all reagents were needed for the reaction to proceed, the control reactions (under Ar; without K; and without Cy2BCl) were carried out. As expected, in none of these cases was NH4 + observed after hydrolysis. Further optimizations were carried out to increase the efficiency in N−B bond formation, and thus the yield of NH4 + after hydrolysis. Due to the use of solid K, the stirring efficiency was found to be particularly important. A strong agitation was most likely required to prevent passivation of the K surface.
The first parameter evaluated was the stoichiometry between K and Cy2BCl (entries 16 vs. 1). A 2.5‐fold excess of K was found to be favorable, although some of it remained unconsumed at the end of the reaction. Decreasing the concentration of chloroborane from 0.04 to 0.02 mol L−1 led to a significant increase in yield (entries 15 vs. 2), which was, however, counterbalanced by cutting the K into several pieces (entries 17 vs. 15).
The effect of N2 pressure was also tested. Increasing the pressure to 20 and 40 bars resulted in major improvements in the yields: up to 60 % and 76 %, respectively (entries 18 and 19 vs. 2). At 80 bar, a 94 % yield was obtained (entry 20), attesting a highly efficient N2 functionalization by the Cy2B radicals. Running the reaction on a ten‐fold scale provided a slightly improved yield (entry 21, 48 % vs. 41 % entry 2), while a hundred‐fold scale reaction (with doubled concentration) showed a very moderate decreased yield (entry 22, 38 % vs. 41 % entry 2). Finally, two experiments were carried out with 15N2 gas, either mixed with 14N2 or pure (ESI). 15NH4 + was observed after hydrolysis when pure 15N2 was used, while both 15NH4 + and 14NH4 + were obtained as expected from the mixture providing definitive evidence of the direct functionalization of N2 under these conditions. The kinetics of the reaction were measured by hydrolysis and 1H NMR quantification of aliquots under conditions of entry 2. These studies led to the conclusion that the reaction is essentially completed after 2 h (ESI), even though the color of the medium continues to darken over time.
NMR Monitoring: Identification of Borylamines and Boron Containing Side Products
All of the above reactions were monitored by 11B NMR with the aim to characterize the products prior to hydrolysis. Unfortunately, the N−B‐containing products were not observed, most likely because of signal broadening due to N−B coupling. On the other hand, side products corresponding to the known Cy2BH2 − (δ=−9.0 ppm, triplet) and Cy2BH (δ=17.0 ppm, doublet) could be observed in variable proportions, depending on the applied conditions. When stoichiometric amounts of K and Cy2BCl were used (entry 16), only Cy2BH was observed, forming colorless crystals of (Cy2BH)2 upon concentration of crude mixtures. On the other hand, the anion Cy2BH2 − was formed when an excess of K was used for the reaction. The observation of signals attributed to Cy2BH2 − and (Cy2BH)2 in the 1H coupled 11B spectrum of the reaction carried out in THF‐D8 demonstrated that intramolecular H migration to the B‐centered radical is faster than the intermolecular abstraction of D atom from the solvent. [29]
We also found that the intensity of these two signals is inversely proportional to the yield in NH4 + obtained after hydrolysis, indicating that the formation of B−H derivatives competes with the coupling of the B‐based radical with N2.
Multinuclear NMR experiments (1H, 15N, 15N‐1H HMBC) demonstrated that a mixture of two borylamine compound(s), N(BCy2)3 and NH(BCy2)2 were generated by the reduction process, with relative ratios also depending on the experimental conditions (see ESI). Above all, NMR analyses carried out on samples taken before hydrolysis of a reaction performed under the conditions of entry 20, previously found to give the best yield in NH4 + without BH‐type secondary products, revealed that N(BCy2)3 is formed with a yield exceeding 90 %. The 15N‐1H HMBC spectrum of a reaction carried out in THF‐D8 showed a cross‐signal for the NH(BCy2)2 compound, thereby pointing to a faster intramolecular HAT (H atom transfer) process at a generated N radical, than D abstraction from the solvent.
With these results in hand, other halogeno boranes were tested under optimized conditions. The chlorocatecholborane did not lead to formation of any NH4 + after hydrolysis (entry 23), which implies, in accord with earlier reports, [28] that the B−B bond forming process is favored over that of the N−B bond. On the other hand, two other dialkylchloroborane were used successfully to achieve this transformation. Using DIP‐Cl under the standard conditions used in entry 2 resulted in the formation of NH4 + in 28 % yield (entry 24), to be compared with the 41 % and 43 % yields obtained under the same conditions with Cy2BCl and Bis(bicyclo[2.2.1]‐2‐heptyl)chloroborane (entry 25), respectively. These results clearly bring to light the major influence of the alkyl substituents at B, an effect which will be the subject of a subsequent study.
EPR Monitoring: Evidence of Organic Radical Formation
The proposed reaction scheme, involving formation of organic radicals, was further confirmed by EPR measurements (X band) carried out either at room temperature or at 110 K. The samples were prepared under the same conditions as above, i.e., in a dedicated glove box under N2, upon mixing at room temperature under vigorous stirring Cy2BCl and K in dry THF (entry 17). EPR analyses were conducted on aliquots collected at different reaction times. The spectra collected after 90, 150 and 210 minutes of stirring are shown in Figure 2.
Figure 2.

EPR spectra recorded at RT after stirring a mixture of Cy2BCl/K in THF under N2 for a) 90; b) 150, c) 210 minutes. d) Experimental spectrum recorded at 110 K after 4 h of stirring; e) simulated spectrum using easyspin (Matlab toolbox).
The spectra in Figure 2, A reveal that stable organic radical(s) accumulate in solution after one hour of reaction. At first sight, those spectra seem to consist of three lines of relative intensity: 1/2/1. Further studies on longer reaction times, however, revealed that the intensity of the central signal at g=2.0034 increases more rapidly than the two peripheral ones. This outcome is consistent with the conclusion that the apparent triplet developing over time in fact results from the presence of at least two different organic radicals. We also found that the temperature (RT vs. 110 K) of the resonator has only a limited effect on the number, shape and relative intensity of those signals and that those signals eventually disappear over time. Key insights into the nature of the radicals involved in solution were provided by simulation of the experimental data. The three‐line signal showing a large peak‐to‐peak line width could be readily simulated with a 1 : 1 : 1 triplet at g=2.0036 attributed to a 14N (I=1)‐centered radical featuring a hyperfine constant, aN=11.8 G (see Figure S25, ESI). [30] The broad and unsmooth character of the experimental lines (Figure 2) is, moreover, consistent with the existence of low, superhyperfine, and thus unresolved, interactions (<1 G) with surrounding hydrogen atoms. Such features could correspond to the computed intermediate radicals I, or more likely M proposed in Figure 4 (vide infra). Attributing the additional central singlet at g=2.0034 remains hypothetical at this stage. Based on relevant previous studies involving similar organic radicals,[ 31 , 32 , 33 , 34 , 35 ] we propose an attribution of that additional signal either to a C‐ or B‐centered radicals featuring low, and thus unresolved, hyperfine coupling constants (I[B11]=3/2, I[B10]=3). This attribution was further supported by EPR measurements performed under an Ar atmosphere. In the absence of N2, we found that the colorless solution remains EPR silent until a brown red color appears leading to the development of one intense singlet signal at g=2.0034 (see Figure S26, ESI) consistent with the formation of the radical discussed above. Taken together, these measurements provide unambiguous evidence supporting the existence of in situ generated organic radicals, most notably nitrogen‐centered species as intermediates in the direct chemical reduction of Cy2BCl by K in THF under N2.
Figure 4.
Computed pathway: the energies are relative to “6 A+N2′′. Functionalization to the hydrazine (Cy2B)2NN(BCy2)2 derivative (K) followed by reductive NN bond splitting process leading to bis‐borylamide N.
DFT Calculations: Reaction Mechanism
To shed light on the reaction mechanism, DFT calculations were carried out. Only the lowest energy pathway leading to N(BCy2)3 is presented here. Not surprisingly, in light of the poor Lewis basic properties of N2, attempts to locate an adduct with Cy2BCl failed. The reactivity between N2 and the reduced radical anion Cy2BCl⋅− (A), generated through one‐electron reduction of Cy2BCl by potassium, was investigated (Figure 3). Two pathways were computed from A: coordination of N2 vs. Cl− elimination. The latter pathway is kinetically unfavorable (ΔΔG ≠=8.9 kcal mol−1), as depicted in Figure 3. A transition state TSA‐B for N2 coordination was located at ΔG ≠=7.9 kcal mol−1 above A. N2 coordination is exoergic (ΔG=−8.2 kcal mol−1) and leads to the radical anion B with a clear nitrogen‐boron interaction (N−B=1.558 Å). Upon dinitrogen coordination to A, the N−N bond elongates from 1.097 Å to 1.174 Å. Analysis of the electronic structure of B indicates that the N−B bond results from the donation of the B‐centered electron into one π* orbital of N2, in agreement with the elongation of the N−N bond upon coordination. Dissociation of Cl− from B to form the radical Cy2BNN⋅ C is computed to be a favorable pathway (ΔG=−5.0 kcal mol−1), resulting in an even shorter N−B bond (1.413 Å). In C, the spin density has significant weight on the terminal nitrogen atom (see Figure S27). Therefore, the creation of a second B−N bond upon interaction with the radical anion A, is computed to be strongly exoergic (ΔG=−44.9 kcal mol−1) to form E. Diazene F, the result of a two‐electron reduction of N2 with concomitant formation of two N−B bonds, is obtained upon chloride dissociation from E. These two electrons have populated one π* orbital on N2 and, due to the unsaturated nature of boron, a two‐electron delocalized π‐type interaction develops between the B−N−N−B atoms. This interaction is illustrated by the linear geometry for the four atoms with rather short B−N bonds, an elongated N−N bond (B−N=1.37 Å and N−N=1.18 Å; N−N=1.25 Å in free H2N2) and the nature of the HOMO (see Figure S30). [36]
Figure 3.
Computed pathway: the energies are relative to “6 A+N2”. Addition of A (Cy2BCl⋅−) to N2 up to the formation of three N−B bonds (compound H, three‐electron reduction of N2). Note that the energy positioning of the various species does not take into account any potential stabilizing interactions developing between K+ and Cl− in the experimental situation.
One‐electron reduction of F by A populates the remaining N2‐centered π* orbital in an exoergic process (ΔG=−23.3 kcal mol−1) to yield the radical anion G featuring a zig‐zag geometry for the B−N−N−B linkage (B−N=1.380 Å, N−N=1.284 Å and B−N−N=136.5°). Coordination of Cy2BCl affords the radical anion H (ΔG=−12.4 kcal mol−1), from which chloride readily dissociates to yield the neutral radical I featuring three N−B bonds. A strongly exoergic (ΔG=−37.6 kcal mol−1) one‐electron reduction of I by A populates the π* orbital between the two nitrogen atoms and yields the anionic system J (Figure 4) featuring an N‐centered lone pair on the nitrogen with only one N−B bond (see Figure S31). Subsequent nucleophilic substitution at Cy2BCl (ΔG=−31.7 kcal mol−1) forms the four boron‐substituted hydrazine K.
The bond‐dissociation energy of the N−N bond in hydrazine K is 46.1 kcal mol−1; reduction is required for subsequent N−N bond breaking. Thus, one‐electron reduction of K by A is computed also to be endoergic but by only ΔG=8.0 kcal mol−1 to yield L. The transition state TSL −M+N associated with N−N bond cleavage is computed with a very small activation barrier (ΔG ≠=1.5 kcal mol−1) to form the radical (Cy2B)2N⋅ M and the anion (Cy2B)2N− (N) with ΔG=−47.0 kcal mol−1. The one‐electron reduction of M by A to form N and Cy2BCl is computed to be strongly exoergic (ΔG=−49.7 kcal mol−1). This step concludes the six‐electron reduction of N2 to form two equivalents of the anion N. This boron‐substituted amide features a linear geometry with two perpendicular B−N π‐orbitals similar to the allene structure. Finally, tris‐borylamine N(BCy2)3 P is formed by a nucleophilic substitution between N and Cy2BCl (Figure S32).
In summary, these computations highlight the facile and favorable coordination of N2 to the Cy2BCl radical anion A obtained by one‐electron reduction by K, as the first and crucial step in the functionalization process. Notably, coordination of N2 to this radical anion prior to chloride elimination appears to be kinetically preferred over the reverse process. The overall transformation is strongly exoergic because of the high reactivity of the radical anion A, Cy2BCl⋅−.
Having rationalized the formation of N(BCy2)3, as well as NH(BCy2)2 (Figure S34), the competing formation of BH‐containing byproducts required investigation. The intramolecular H migration from the cyclohexyl to B was thus computed (Figure S33). In accordance with the literature, [28] this migration proved both facile and thermodynamically favorable. The lowest energy pathway was found via the generation of the radical Cy2B⋅ D. The transition state was found to be only 13.3 kcal mol−1 higher than Cy2B⋅, and thus 22.2 kcal mol−1 above A, readily accessible at room temperature. The resulting C‐centered radical is computed at −18.5 kcal mol−1 relative to D (−9.6 kcal mol−1 vs. A). Most importantly, the addition of N2 to the in situ generated R2BCl radical anion A to form the first BN bond is lower in energy than the competing HAT from the neighboring Cy to B that creates the BH bond leading to side‐product formation. This kinetic preference is crucial in the successful N2 functionalization.
Conclusion
In conclusion, we present the first successful functionalization of N2 using boron‐centered radicals, at room temperature and low pressures (from one atmosphere). These radicals are efficiently generated in situ by reduction of the corresponding, readily available chloroborane derivatives. We believe that these results open new avenues to N2 functionalization notably different from the high‐energy heterogeneous HB process and the bio‐inspired homogeneous transformations. These findings could drastically affect the carbon footprint of ammonia production and pave the way for new applications for ammonia, particularly in renewable energy storage and the hydrogen economy. [37]
Supporting Information
See Supporting Information for experimental section, characterization data, spectra, as well as EPR measurements and DFT calculations (details of computations, mechanisms leading to NH and BH bond formations).
Conflict of interest
A patent based on the present work has been filed on May 20, 2021 under the number: FR2105295, with inventors S. Bennaamane and N. Mézailles. (mentioned in our article as ref [37]) The patent has been licensed to SWAN‐H. N.M. is co‐founder and president of SWAN‐H.
1.
Supporting information
As a service to our authors and readers, this journal provides supporting information supplied by the authors. Such materials are peer reviewed and may be re‐organized for online delivery, but are not copy‐edited or typeset. Technical support issues arising from supporting information (other than missing files) should be addressed to the authors.
Supporting Information
Acknowledgments
Financial support from CNRS and Université de Toulouse is acknowledged. CALMIP is gratefully acknowledged for access to supercomputing facilities. C.B. wishes to thank the “région Auvergne‐Rhône‐Alpes” for financial support. The NMR service of the ICT is gratefully acknowledged, as well as Mrs. C. Absalon for LIFDI MS analysis. We thank T. Personeni for preparing samples for EPR experiments and Dr. W. Schipper from SWAN‐H for insightful discussions.
In memory of Pascal Le Floch
Bennaamane S., Rialland B., Khrouz L., Fustier-Boutignon M., Bucher C., Clot E., Mézailles N., Angew. Chem. Int. Ed. 2023, 62, e202209102; Angew. Chem. 2023, 135, e202209102.
Data Availability Statement
The data that support the findings of this study are available in the Supporting Information of this article.
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Data Availability Statement
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