Literature DB >> 35714100

Photoelectrochemical Conversion of Dinitrogen to Benzonitrile: Selectivity Control by Electrophile- versus Proton-Coupled Electron Transfer.

Maximilian Fritz1, Severine Rupp2, Ciara I Kiene1, Sesha Kisan1, Joshua Telser3, Christian Würtele1, Vera Krewald2, Sven Schneider1.   

Abstract

Nitride complexes are key species in homogeneous nitrogen fixation to NH3 via stepwise proton-coupled electron transfer (PCET). In contrast, direct generation of nitrogenous organic products from N2 -derived nitrides requires new strategies to enable efficient reductive nitride transfer in the presence of organic electrophiles. We here present a 2-step protocol for the conversion of dinitrogen to benzonitrile. Photoelectrochemical, reductive N2 splitting produces a rhenium(V) nitride with unfavorable PCET thermochemistry towards ammonia generation. However, N-benzoylation stabilizes subsequent reduction as a basis for selective nitrogen transfer in the presence of the organic electrophile and Brønsted acid at mild reduction potentials. This work offers a new strategy for photoelectrosynthetic nitrogen fixation beyond ammonia-to yield nitrogenous organic products.
© 2022 The Authors. Angewandte Chemie International Edition published by Wiley-VCH GmbH.

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Keywords:  Electrochemistry; N2 Fixation; Photochemistry; Reaction Mechanisms; Rhenium

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Year:  2022        PMID: 35714100      PMCID: PMC9542086          DOI: 10.1002/anie.202205922

Source DB:  PubMed          Journal:  Angew Chem Int Ed Engl        ISSN: 1433-7851            Impact factor:   16.823


Introduction

Proton‐coupled electron transfer (PCET) is a key concept for the design of efficient redox catalysts. As a prominent example, Nishibayashi reported that Mo pincer catalysts generate over 4000 eq. of NH3 in the nitrogen reduction reaction (NRR) at ambient conditions with the model PCET reductant SmI2/H2O. In fact, most homogeneous NRR catalysts are anticipated to operate via initial PCET to metal‐coordinated N2 as a thermochemically challenging step. An alternative, Haber–Bosch‐like pathway that has been considered commences with full N2 splitting prior to N−H bond formation.[ , ] However, terminal nitride complexes that result from reductive N2 splitting generally exhibit low to moderate hydrogen atom affinities. This is expressed by N−H bond dissociation free energies (BDFE N−H) of the corresponding parent imides that are typically below ≈45 kcal mol−1 (Scheme 1a). In consequence, the first PCET step after N2 splitting defines a thermochemical bottleneck for ammonia‐selective nitrogen reduction vs. competing H2 evolution. PCET‐based strategies will be key to establish efficient, photo‐ and electrochemically driven NRR catalysis that does not rely on sacrificial chemical reductants.
Scheme 1

Computed BDFE N−H for imido complexes relevant to N2 splitting and PCET‐based strategies for selectivity control.

Computed BDFE N−H for imido complexes relevant to N2 splitting and PCET‐based strategies for selectivity control. N2 splitting also provides a potential entry towards nitrogenous products beyond ammonia. This was demonstrated by several stoichiometric (cyclic) reaction sequences,[ , ] as well as the catalytic formation of trisilylamines and recently triborylamines, directly from N2. However, several challenges remain to be addressed to obtain more complex targets, like primary amines or amides. For example, electrolysis of a MoIV alkylimide complex in acidic solution (AcOH) required potentials that are incompatible with most organic electrophiles (−2.3 V vs. Fc+/0).[ , ] One‐pot or even catalytic product formation via reductive N2 splitting in the presence of both electrophiles and Brønsted acid necessitates strategies to reduce the overall overpotential and control the N−C vs. N−H bond formation selectivity. Our groups previously examined N2 splitting and nitride transfer enabled by (electro‐)chemical reduction of rhenium complexes with bulky PNP‐pincer ligands. Light‐driven N2 splitting of the modified platform 1  a (Scheme 1b) gave the more reactive nitride 2  a, which converts benzoyl chloride to benzamide upon PCET from the pincer backbone, but only at elevated temperatures. We here present a PCET‐based synthetic strategy for direct, cathodic product release in the presence of electrophile and acid. This enabled the development of a one‐pot protocol for photoelectrochemical N2 splitting and benzonitrile formation at mild potentials and ambient temperature (Scheme 1c).

Results and Discussion

We first aimed at replacing BzCl by benzoylation reagents of the higher halides as being better nucleofuge. For that purpose, N2 splitting with [ReX3(HPNP)] (1  b: X=Br, 1  c: X=I; Scheme 2) was examined to avoid complications from halide scrambling during subsequent benzoylation. The bromide and iodide complexes were synthesized from [ReBr3(PPh3)2(MeCN)] and by halide metathesis for 1  c, respectively. Spectroscopic and crystallographic characterization of 1  b/c support rhenium(III) in meridional octahedral coordination. As a typical trend for the halide precursors,[ , ] cyclic voltammetry (CV) showed that the first reduction of 1  b (E 1/2=−1.70 V vs. FeCp2 +/0) and 1  c (E 1/2=−1.52 V) are at significantly less negative potentials with respect to 1  a (E 1/2=−1.84 V). At lower scan rate, the ReIII/II couple becomes irreversible for all three halides, which is attributed to X− loss from [ReX3(HPNP)]− as a prerequisite to N2 activation. Scan rate dependent data allowed for estimating first order halide dissociation rate constants. The increase by almost two orders of magnitude along the halide series (k diss=0.05 s−1 (1  a), 0.33 s−1 (1  b), 1.97 s−1 (1  c); Figures S67–S69) correlates with increasing halide ionic radii and polarizability, viz leaving group properties.[ , ] Accordingly, the higher halides allowed for photoelectrochemical N2 splitting by controlled potential electrolysis (CPE) at less negative potentials (Scheme 2). Furthermore, the productive photolysis window favourably extends further into the visible range. CPE of the halide series (E app=−1.73 V (1  b), −1.53 V (1  c)) under N2 with irradiation by a blue LED (λ=456±10 nm) gave increased yields of the nitride complexes 2  b (37 %; Faradaic Efficiency (FE)=22 %) and 2  c (53 %; FE=53 %) with respect to the parent chloride (1  b). Complexes 2  b and 2  c were fully characterized, including crystallography (Figures S98 and S99), which confirmed cis‐configurations in the solid state as was found for 2  a.
Scheme 2

Photoelectroreductive N2 splitting with precursors 1  a–c (FE=Faradaic Efficiency).

Photoelectroreductive N2 splitting with precursors 1  a–c (FE=Faradaic Efficiency). In contrast to 2  a/PhC(O)Cl, benzoylimide formation is directly observed upon addition of excess PhC(O)Br to 2  b in THF. Crystallization gave [Re(NBz)(HPNP)]Br (3) in high yield (Scheme 3). While isolated 3 is stable in CH2Cl2 over several days, re‐dissolving in THF leads to rapid dissociation of benzoyl bromide and a small equilibrium constant was obtained in a titration experiment monitored by 31P NMR spectroscopy (K THF=1.1×10−5 M−1; Figure S31). However, benzoylimide formation can be driven by halide exchange with NaBArF 24 (BArF 24 −=B{3,5‐(CF3)2C6H3}4 −), giving 3 in 90 % yield (Scheme 3). In the solid state, the rhenium(V) benzoyl imido complexes 3 and 3 (Figure 1 and Figure S101) exhibit a structural reorganization with respect to the parent nitride 2  b (see above). The trans‐dibromide configuration of the cation of 3 and 3 reflects the decreased trans‐influence of the multiply bonded nitrogen ligand, as expressed by the significantly longer Re−N multiple bond length (3: 1.724(3) Å (exp), 1.734 Å (DFT); 2  b: 1.663(5) Å (exp), 1.677 Å (DFT); Table S3/S5). 1H NOESY characterization (Figure S30/S37) confirmed the trans configuration also in solution and computations favoured trans‐3 over the cis isomer by ΔG 0 DFT=3.8 kcal mol−1.
Scheme 3

Benzoylation equilibrium of 2  b and benzoyl bromide.

Figure 1

Molecular structures of 3, 4, 5 and 6 in the solid state drawn at the 50 % probability level. Hydrogen atoms except N−H are omitted for clarity. Selected bond lengths [Å] and angles [°]: 3: N1‐Re1 2.278(3), Re1‐N2 1.724(3), N2‐C17 1.425(4), C17‐O1 1.206(4); Br1‐Re1‐Br2 165.462(12), N1‐Re1‐N2 176.37(12). 4: N1‐Re1 2.168(7), Re1‐N2 1.788(8), N2‐C17 1.343(12), C17‐O1 1.251(10); N1‐Re1‐Br1 170.9(2), Br2‐Re1‐N2 170.3, P1‐Re1‐P2 163.70(8). 5: N1‐Re1 1.901(2), N2‐C23 1.325(4), C23‐O1 1.275(4); Br1‐Re1‐C17 109.35(8), N1‐Re1‐O1 166.92(9), P1‐Re1‐P2 166.1481). 6: N1‐Re1 2.161(5), Re1‐N2 2.113(4), N2‐C17 1.289(7), C17‐O1 1.259(7); N1‐Re1‐Br2 177.47(13), Br1‐Re1‐N2 176.63(12), P1‐Re1‐P2 163.19(5).

Benzoylation equilibrium of 2  b and benzoyl bromide. Molecular structures of 3, 4, 5 and 6 in the solid state drawn at the 50 % probability level. Hydrogen atoms except N−H are omitted for clarity. Selected bond lengths [Å] and angles [°]: 3: N1‐Re1 2.278(3), Re1‐N2 1.724(3), N2‐C17 1.425(4), C17‐O1 1.206(4); Br1‐Re1‐Br2 165.462(12), N1‐Re1‐N2 176.37(12). 4: N1‐Re1 2.168(7), Re1‐N2 1.788(8), N2‐C17 1.343(12), C17‐O1 1.251(10); N1‐Re1‐Br1 170.9(2), Br2‐Re1‐N2 170.3, P1‐Re1‐P2 163.70(8). 5: N1‐Re1 1.901(2), N2‐C23 1.325(4), C23‐O1 1.275(4); Br1‐Re1‐C17 109.35(8), N1‐Re1‐O1 166.92(9), P1‐Re1‐P2 166.1481). 6: N1‐Re1 2.161(5), Re1‐N2 2.113(4), N2‐C17 1.289(7), C17‐O1 1.259(7); N1‐Re1‐Br2 177.47(13), Br1‐Re1‐N2 176.63(12), P1‐Re1‐P2 163.19(5). Starting from 3, reduction was examined first in the absence of acid. The CV of 3 in THF shows a reversible reduction at E 1/2=−0.71 V (v=1.0 V s−1; Scheme 4) and a reduction at E p,c=−1.63 V (v=0.1 V s−1), which was irreversible at all scan rates (Figure S61). Notably, at lower scan rates, the first reduction also becomes increasingly irreversible and a new feature at E p,a=−0.42 V grows in the reverse oxidative scan, while the ratio of the cathodic and the sum of the anodic peak currents stays close to unity (Figure S62). These observations are in line with an ECE mechanism, namely a chemical step that follows reduction within the CV timescale, which can be attributed to trans to cis isomerization (see below). Chemical reduction of 3 with cobaltocene enabled the isolation of the rhenium(IV) benzoylimido complex [Re(NBz)Br2(HPNP)] (4) in 85 % yield (Scheme 4). Notably, only five‐coordinate ReIV oxo and imido complexes were previously reported, and ReIV oxo species have been proposed as reactive intermediates in C−H activation.
Scheme 4

Top: Synthesis of 4, 5, and 6 by reduction of 3 including protonolysis of 5 and 6 obtaining 1  b and benzamide. Bottom left: Cyclic voltammetry of the ReV/IV couple of 3 (1 mM in THF, 0.1 M N Bu4PF6) at varied scan rate (currents are normalized to v1/2). Bottom right: Cyclic voltammetry of 3 in presence of 10 eq. [LutH]OTf/Lutidine (1 mM in THF, 0.1 M N Bu4PF6) at varied scan rate. * Isolated yield.

Top: Synthesis of 4, 5, and 6 by reduction of 3 including protonolysis of 5 and 6 obtaining 1  b and benzamide. Bottom left: Cyclic voltammetry of the ReV/IV couple of 3 (1 mM in THF, 0.1 M N Bu4PF6) at varied scan rate (currents are normalized to v1/2). Bottom right: Cyclic voltammetry of 3 in presence of 10 eq. [LutH]OTf/Lutidine (1 mM in THF, 0.1 M N Bu4PF6) at varied scan rate. * Isolated yield. The X‐band EPR signal of 4 in toluene at room temperature exhibits large 187Re hyperfine interaction (g=1.92, a iso=700 MHz; Figure S40), supporting a low‐spin ReIV complex. Structural characterization in the solid state (Figure 1) indicates isomerization to the cis‐dibromide configuration. Comparison of the molecular structures of 3 and 4 shows a significant elongation of the Re=N bond by 0.09 Å upon reduction despite reduced trans‐influence in the cis‐configuration. Isolated 4 exhibits a reversible oxidation at E 1/2=−0.48 V (Figure S64). We therefore attribute the ECE signature of the reduction of 3 to slow isomerization of trans‐4 to cis‐4 with an estimated rate constant of k iso≈0.04 s−1 (Figure S70). The potential shift (ΔE 1/2=0.23 V; ΔΔG°=5.3 kcal mol−1) arises from the difference between the cis/trans‐isomerization equilibria in the oxidized (cis/trans‐3) and reduced (cis/trans‐4) states, respectively, which is well reproduced by DFT (ΔΔG°DFT=6.7 kcal mol−1, Figure S94). Isomerization of trans‐4 to the more stable cis‐configuration was computed exergonic by ΔG°DFT=2.9 kcal mol−1. The irreversible ReIV/III redox couple was examined by chemical reduction of 3 with CoCp*2 (2 eq.). Two‐electron reduction is associated with a substantial structural reorganization. Bromide loss, ortho‐metalation, tautomerization and κN‐to‐κO isomerization gives diamagnetic [ReIII{C6H4C(O)NH2}Br(PNP)] (5; Scheme 4) in 68 % isolated yield. Bromide ion dissociation after the second reduction is probably a prerequisite to cyclometalation. Conceivable pathways to cyclometallation are C−H oxidative addition to rhenium(III) or addition across the Re=NBz bond.[ , ] Protonolysis of 5 with diphenyl ammonium bromide (pK a THF=0.6) restores parent 1  b and gives free benzamide in over 70 % yield (Scheme 4, top), closing a synthetic cycle from N2 to benzamide, yet at high overpotential. The electrochemical data of 3 reveals a remarkable anodic shift of the first reduction potential (E 1/2=−0.71 V) with respect to parent nitride 2  b (ΔE >2.2 V). For comparison, much smaller effects were reported for borylation of a MoIV nitride (ΔE≈350 mV) or alkylation of a MoVI nitride (ΔE≈1 V), respectively. The benzoyl‐induced potential shift of 3/4 becomes apparent upon comparison with the respective parent imide [Re(NH)Br2(HPNP)]+/0 (8/7). For this purpose, the thermochemistry of electron cross transfer of the ReV/ReIV pairs 3/4 and 8/7 was calculated as an isodesmic reaction to avoid difficulties for computing absolute potentials (Scheme 5). The reaction free energy (Δr G°=−17.9 kcal mol−1) indicates that the reduction of the parent rhenium(V) imide should be around 0.8 V more negative (E 1/2(8/7)≈−1.5 V) than the benzoylimide trans‐3 (E 1/2=−0.71 V). The computations further confirm a low N−H bond strength of the parent rhenium(IV) imide trans‐7 (BDFE N−H=33.2 kcal mol−1), which is very close to that of the related complex [Re(NH)Cl{N(CH2CH2PtBu2)2}] (Scheme 1), rendering 7 thermodynamically unstable with respect to hydrogen evolution (BDFE H−H=52 kcal mol−1 in THF). Furthermore, as judged from a thermochemical cycle, the protonation of 2  b requires strong acids (pK a THF(trans‐8)≈5).
Scheme 5

Top: Frontier Kohn–Sham MOs of trans‐3 (left) and cis‐4 (right). Bottom: Thermochemistry of electron cross equilibrium of trans‐3/4 with trans‐7/8. For simplicity, the trans‐configurations were used for all states. Note that the cis‐configuration is slightly more stable for 4 (ΔG=2.9 kcal mol−1). See Supporting Information for the cis‐isomers.

Top: Frontier Kohn–Sham MOs of trans‐3 (left) and cis‐4 (right). Bottom: Thermochemistry of electron cross equilibrium of trans‐3/4 with trans‐7/8. For simplicity, the trans‐configurations were used for all states. Note that the cis‐configuration is slightly more stable for 4 (ΔG=2.9 kcal mol−1). See Supporting Information for the cis‐isomers. The thermochemical bias in favour of benzoyl‐ vs. proton‐coupled reduction can be rationalized by π‐bonding within the {Re≡N−R} core (R=Bz, H). While the ReV imides 3 and 8 as well as the ReIV imide 4 are nearly linear, 7 was computed to be distinctly bent (∠Re−N−H: 120°). This conformational reorganization can be attributed to population of a molecular orbital (MO) with π*Re−N character. Bending of the Re−N−H moiety reduces the 3‐electron interaction of the d Re and p N atomic orbitals. In contrast to hydrogen, the benzoyl substituent is a moderate π‐acceptor. In fact, Nielson et al. previously described the acylimido ligand (NC(O)H)2− as a single faced π‐donor. The population of a molecular orbital with {Re≡NBz} π* character in 4 (Scheme 5) is in line with the significant elongation of the Re−N bond with respect to 3 (see above). In turn, πN−C and π*C−O character of the SOMO of 4 leads to contraction of the N−C (Δd=0.08 Å) and elongation of the C−O (Δd=0.07 Å) bonds. Hence, charge delocalization into the benzoyl substituent contributes to the remarkable anodic shift of the reduction potential with respect to the nitride and parent imide complexes. This thermochemical framework emphasizes that ammonia formation will be hampered by the unfavourable first PCET to 2  b. We therefore aimed at utilizing the preference in favour of Bz+/e− transfer to control the selectivity of nitride transfer. Full release of organic products requires further reduction and addition of electrophiles. For this purpose, PCET of the benzoylimido complex was examined. Addition of 2,6‐dichlorphenol (11 eq.; pK a THF=25.1) to 3 leads to a significant anodic shift of the irreversible, second reduction by around +400 mV, suggesting PCET (Figure S63). In the presence of the stronger acid lutidinium triflate ([LutH]OTf; 10 eq.; pK a THF=7.2), the first wave retains the reversible reduction, yet with anodically shifted potential (E 1/2=−0.66 V; ΔE=50 mV) and significantly higher peak current, supporting a multi‐electron process (Scheme 4). Accordingly, chemical reduction of 3 with CoCp2 and lutidinium bromide (2 eq. each) gives rhenium(III) carboxamide complex 6 in 87 % spectroscopic yield (Scheme 4) and traces of 1  b (3 %). Crystallographic characterization of 6 confirms single bond character of the Re−NHBz bond (d Re1−N2=2.113(4) Å) after 2e−/H+ reduction (Figure 1). The full, chemically driven nitrogen transfer can be obtained upon addition of the strong acid [Ph2NH2]Br (pK a THF=0.6), giving free benzamide and 1  b in yields of 56 % and 80 %, respectively (Scheme 4). Motivated by these results, we developed protocols for direct, one‐pot (electro‐)chemically driven nitride transfer from 2  b. Addition of benzoyl bromide (3 eq.), [LutH]BArF 24 (3 eq.), and the mild chemical reductant FeCp2* (3 eq.; E 1/2=−0.43 V) to 2  b in THF‐d 8 (Scheme 6, Entry 1 and Figure S74) gives parent 1  b as the only detectable product by 31P NMR spectroscopy in 55 % yield, together with an equimolar amount of benzonitrile (56 %). The use of the 15N labelled nitride complex from photoelectrochemical splitting of 15N2 confirmed nitride transfer to the organic product (Figure S76). Ammonium as a potential product is not detected. Besides PhCN, benzoyl anhydride (43 %) and benzoic acid (23 %) are observed. This is in line with initial formation of benzamide, which subsequently reacts with additional BzBr to benzonitrile and the anhydride/acid. The formation of some 4‐bromobutyl benzoate (26 %) is attributed to electrophilic ring opening of THF with benzoyl bromide, which is catalysed by Lewis acids. Increased yields for both benzonitrile (77 %) and 1  b (82 %) are obtained with the weaker acid [Et3NH]BArF 24 (Scheme 6, Entry 2). Without additional acid, benzonitrile yields are strongly reduced (10 %; Scheme 6, Entry 3). Furthermore, instead of 1  b the rhenium(III) imine complex [ReBr3{N(CHCH2P Pr2)(CH2CH2P Pr2)}] (9) is spectroscopically observed in 9 % yield as the only identified rhenium product upon comparison with an original sample. Complex 9 is most conveniently obtained from reaction of 1 with 2,4,6‐tri‐tert‐butylphenoxyl radical and was fully characterized including X‐ray crystallography. The dehydrogenation of the PNP ligand during reductive nitride transfer underlines the necessity of acid for full nitrogen release, presumably via PCET after N‐benzoylation.
Scheme 6

Reaction conditions for one‐pot (electro‐)chemical nitride transfer from N2 derived nitride 2  b to give 1  b and benzonitrile. All yields refer to rhenium nitride complex 2  b; FE=Faradaic Efficiency. [a] The yield in BzOH defines an upper limit; it was indirectly estimated by 1H‐NMR spectroscopy from integration of the signals of BzO(CH2)4Br, which are superimposed with those of BzOH (see Supporting Information pp. S54–S58).

Reaction conditions for one‐pot (electro‐)chemical nitride transfer from N2 derived nitride 2  b to give 1  b and benzonitrile. All yields refer to rhenium nitride complex 2  b; FE=Faradaic Efficiency. [a] The yield in BzOH defines an upper limit; it was indirectly estimated by 1H‐NMR spectroscopy from integration of the signals of BzO(CH2)4Br, which are superimposed with those of BzOH (see Supporting Information pp. S54–S58). One‐pot electrochemical nitride transfer is accomplished upon CPE of 2  b at the potential of the first reduction (E app=−0.68 V) in the presence of BzBr (5 eq.) and [LutH]BArF 24 (3 eq.) for 22 h (Scheme 6, Entry 4). Similar yields in benzonitrile (51 %; FE=63 %) and 1  b (66 %; FE=81 %) could be obtained compared to chemical reduction (Scheme 6, Entry 1). The spectroscopic yield in 1  b is in line with the transfer of 1.62e− per Re during electrolysis. With [Et3NH]BArF 24 (Scheme 6, Entry 5), slightly increased yields in benzonitrile (66 %; FE=70 %) and 1  b (69 %; FE=73 %) are obtained, whereas 1.88e− per Re are transferred. For the electrochemical protocols, slightly higher amounts of BzBr (5 eq.) are required to compensate for an increased formation of the side product from THF ring opening, 4‐bromobutyl benzoate (117 % and 133 %), as compared with the use of chemical reductants. A control electrolysis experiment without 2  b confirmed the absence of PhCN, Bz2O, and BzOH, yet indicated formation of the THF ring‐opening product. The electrochemical protocol closes a 2‐step electrosynthetic cycle for benzonitrile generation from N2 after photoelectrochemical N2 splitting (Scheme 7).
Scheme 7

2‐Step photoelectrosynthetic cycle for the conversion of N2 to benzonitrile at ambient conditions.

2‐Step photoelectrosynthetic cycle for the conversion of N2 to benzonitrile at ambient conditions.

Conclusion

In summary, we have demonstrated a two‐step photoelectrochemical cycle for the fixation of dinitrogen with benzoyl bromide to yield benzonitrile. Moving to the higher halide precursors significantly shifts both reductive N2 activation to less negative potentials and photolytic N−N splitting deeper into the visible range. The unfavourable first PCET step renders the resulting nitride (X=Br) unsuitable for efficient ammonia generation. PCET cannot compete with benzoylation/reduction, which can at least in part be attributed to π‐stabilization of the unusual rhenium(IV) imido state by the benzoyl substituent. This thermochemical bias provides a PCET‐based, conceptual basis to enable selective, electrochemical formation of nitrogenous organic products over ammonia production. We have demonstrated this by the development of an electrochemical one‐pot protocol for nitride transfer upon reduction at mild potential (E appl=−0.74 V), which is compatible with the organic electrophile (BzBr) and acid (Et3NH+), to restore parent 1  b. The release of benzonitrile in 66 % yield is attributed to two PCET steps that follow benzoylation of the nitride with increased driving force and subsequent trapping of benzamide. Our results provide a new, PCET‐based N2 fixation strategy for the selective formation of organic, nitrogenous products.

Conflict of interest

The authors declare no conflict of interest. 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 Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file. Supporting Information Click here for additional data file.
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Authors:  Isabel Klopsch; Markus Kinauer; Markus Finger; Christian Würtele; Sven Schneider
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Authors:  Thomas Kupfer; Richard R Schrock
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7.  Dinitrogen Reduction to Ammonium at Rhenium Utilizing Light and Proton-Coupled Electron Transfer.

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1.  Photoelectrochemical Conversion of Dinitrogen to Benzonitrile: Selectivity Control by Electrophile- versus Proton-Coupled Electron Transfer.

Authors:  Maximilian Fritz; Severine Rupp; Ciara I Kiene; Sesha Kisan; Joshua Telser; Christian Würtele; Vera Krewald; Sven Schneider
Journal:  Angew Chem Int Ed Engl       Date:  2022-07-18       Impact factor: 16.823

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