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Transition metal halide complexes are used as precursors for reductive N 2 activation up to full splitting into nitride complexes. Distinct halide effects on the redox properties and yields are frequently observed yet not well understood. Here, an electrochemical and computational examination of reductive N 2 splitting with the rhenium(III) complexes [ReX 2 (PNP)] (PNP = N(CH 2 CH 2 P t Bu 2 ) 2 and X = Cl, Br, I) is presented. As previously reported for the chloride precursor ( J. Am. Chem. Soc. 2018, 140, 7922), the heavier halides give rhenium(V) nitrides upon (electro-)chemical reduction in good yields yet with significantly anodically shifted electrolysis potentials along the halide series. Dinuclear, end-on N 2 -bridged complexes, [{ReX(PNP)} 2 (μ-N 2 )], were identified as key intermediates in all cases. However, while the chloride complex is exclusively formed via 2-electron reduction and Re III /Re I comproportionation, the iodide system also reacts via an alternative Re II /Re II -dimerization mechanism at less negative potentials. This alternative pathway relies on the absence of the potential inversion after reduction and N 2 activation that was observed for the chloride precursor. Computational analysis of the relevant Re III/II and Re II/I redox couples by energy decomposition analysis attributes the halide-induced trends of the potentials to the dominating electrostatic Re-X bonding interactions over contributions from charge transfer.

The splitting of dinitrogen into nitride complexes emerged as a key reaction for nitrogen fixation strategies at ambient conditions. However, the impact of auxiliary ligands or accessible spin states on the thermodynamics and kinetics of N-N cleavage is yet to be examined in detail. We recently reported N-N bond splitting of a {Mo(μ 2 :η 1 :η 1 -N 2 )Mo}-complex upon protonation of the diphosphinoamide auxiliary ligands. The reactivity was associated with a low-spin to high-spin transition that was induced by the protonation reaction in the coordination periphery, mainly based on computational results. Here, this proposal is evaluated by an XAS study of a series of linearly N 2 bridged Mo pincer complexes. Structural characterization of the transient protonation product by EXAFS spectroscopy confirms the proposed spin transition prior to N-N bond cleavage.

Herein, we describe the redox chemistry of bi- and mononuclear α-diimine-Mn(CO) 3 complexes with an internal proton source in close proximity to the metal centers and their catalytic activity in the electrochemically driven CO 2 reduction reactions. In order to address the impact of the two metal sites and of the proton source, we investigate a binuclear complex with phenol moiety, 1 , a binuclear Mn complex with methoxyphenol unit instead, 2 , and the mononuclear analogue with a phenol unit, 3 . Spectroelectrochemical investigation of the complexes in dmf under a nitrogen atmosphere indicates that 1 and 3 undergo a reductive H 2 formation forming [Mn 2 (H -1 L 1 )(CO) 6 Br] and [Mn(H -1 L 3 )(CO) 3 ], respectively, which is redox neutral for the complex and equivalent to a deprotonation of the phenol unit. The reaction likely proceeds via internal proton transfer from the phenol moiety to the reduced metal center forming a Mn-H species. 2 dimerizes during reduction, forming [Mn 2 (L 2 )(CO) 6 ] 2 , but 1 and 3 do not. Reduction of 1 , 2 , and 3 is accompanied by bromide loss, and the final species represent [Mn 2 (H -1 L 1 )(CO) 6 ] 3- , [Mn 2 (L 2 )(CO) 6 ] 2- , and [Mn(H -1 L 3 )(CO) 3 ] 2- , respectively. 1 and 2 are active catalysts in the electrochemical CO 2 reduction reaction, whereas 3 decomposes quickly under an applied potential. Thus, the second redox active unit is crucial for enhanced stability. The proton relay in 1 alters the kinetics for the 2H + /2e - reduced products of CO 2 in dmf/water mixtures. For 2 , CO is the only product, whereas formate and CO are formed in similar amounts, 40% and 50%, respectively, in the presence of 1 . Thus, the reaction rate for the internal proton transfer from the phenol moiety to the metal center forming the putative Mn-H species and subsequent CO 2 insertion as well as the reaction rate of the reduced metal center with CO 2 forming CO are similar. The overpotential with regard to the standard redox potential of CO 2 to CO and the observed overall rate constant for catalysis at scan rates of 0.1 V s -1 are higher with 1 than with 2 , that is, the OH group is beneficial for catalysis due to the internal proton transfer.

Hydrogenolysis of the chlorosilanes and silyl triflates (triflate = trifluoromethanesulfonate, OTf - ) Me 3- n SiX 1+ n (X = Cl, OTf; n = 0, 1) to hydrosilanes at mild conditions (4 bar of H 2 , room temperature) is reported using low loadings (1 mol %) of the bifunctional catalyst [Ru(H) 2 CO( HPNP iPr )] ( HPNP iPr = HN(CH 2 CH 2 P( iPr) 2 ) 2 ). Endergonic chlorosilane hydrogenolysis can be driven by chloride removal, e.g., with NaBAr F 4 = B(C F 4 - = B(C 6 H 3 -3,5-(CF 3 ) 2 ) 4 - ]. Alternatively, conversion to silyl triflates enables facile hydrogenolysis with NEt 3 as the base, giving Me 3 SiH, Me 2 SiH 2 , and Me 2 SiHOTf, respectively, in high yields. An outer-sphere mechanism for silyl triflate hydrogenolysis is supported by density functional theory computations. These protocols provide key steps for synthesis of the valuable hydrochlorosilane Me 2 SiClH, which can also be directly obtained in yields of over 50% by hydrogenolysis of chlorosilane/silyl triflate mixtures.

A series of square-planar cobalt(II) complexes with pincer ligands {N(CH2CH2PtBu2)2}(-) ({L1(tBu)}(-)), {N(CH2CH2PtBu2)(CHCHPtBu2)}(-) ({L2(tBu)}(-)), and {N(CHCHPtBu2)2}(-) ({L3(tBu)}(-)) was synthesized. Ligand dehydrogenation was accomplished with a new, high-yield protocol that employs the 2,4,6-tri-tert-butylphenoxy radical as hydrogen acceptor. [CoCl{Ln(tBu)}] (n = 1-3) were examined with respect to reduction, protonation, and oxidation, respectively. One-electron oxidations of [CoCl(L1(tBu))] and [CoCl(L2(tBu))] lead to ligand-centered radical reactivity, like amide disproportionation into cobalt(II) amine and imine complexes. In contrast, oxidation of [CoCl{L3(tBu)}] with Ag(+) enabled the isolation of thermally stable, square-planar cobalt(III) complex [CoCl{L3(tBu)}](+), which adopts an intermediate-spin (S = 1) ground state with large magnetic anisotropy. Hence, pincer dehydrogenation gives access to a new platform for high-valent cobalt in square-planar geometry.

The redox series [Ir(n)(NHx)(PNP)] (n = II-IV, x = 3-0; PNP = N(CHCHPtBu2)2) was examined with respect to electron, proton, and hydrogen atom transfer steps. The experimental and computational results suggest that the Ir(III) imido species [Ir(NH)(PNP)] is not stable but undergoes disproportionation to the respective Ir(II) amido and Ir(IV) nitrido species. N-H bond strengths are estimated upon reaction with hydrogen atom transfer reagents to rationalize this observation and are used to discuss the reactivity of these compounds toward E-H bond activation.

The preparation of a number of iron complexes supported by ligands of the type HN{CH2CH2(PR2)}2 [R = isopropyl (((i)Pr)PNP) or cyclohexyl ((Cy)PNP)] is reported. This is the first time this important bifunctional ligand has been coordinated to iron. The iron(II) complexes (((i)Pr)PNP)FeCl2(CO) (1a) and ((Cy)PNP)FeCl2(CO) (1b) were synthesized through the reaction of the appropriate free ligand and FeCl2 in the presence of CO. The iron(0) complex (((i)Pr)PNP)Fe(CO)2 (2a) was prepared through the reaction of Fe(CO)5 with ((i)Pr)PNP, while irradiating with UV light. Compound 2a is unstable in CH2Cl2 and is oxidized to 1a via the intermediate iron(II) complex [(((i)Pr)PNP)FeCl(CO)2]Cl (3a). The reaction of 2a with HCl generated the related complex [(((i)Pr)PNP)FeH(CO)2]Cl (4a), while the neutral iron hydrides (((i)Pr)PNP)FeHCl(CO) (5a) and ((Cy)PNP)FeHCl(CO) (5b) were synthesized through the reaction of 1a or 1b with 1 equiv of (n)Bu4NBH4. The related reaction between 1a and excess NaBH4 generated the unusual η(1)-HBH3 complex (((i)Pr)PNP)FeH(η(1)-HBH3)(CO) (6a). This complex features a bifurcated intramolecular dihydrogen bond between two of the hydrogen atoms associated with the η(1)-HBH3 ligand and the N-H proton of the pincer ligand, as well as intermolecular dihydrogen bonding. The protonation of 6a with 2,6-lutidinium tetraphenylborate resulted in the formation of the dimeric complex [{(((i)Pr)PNP)FeH(CO)}2(μ2,η(1):η(1)-H2BH2)][BPh4] (7a), which features a rare example of a μ2,η(1):η(1)-H2BH2 ligand. Unlike all previous examples of complexes with a μ2,η(1):η(1)-H2BH2 ligand, there is no metal-metal bond and additional bridging ligand supporting the borohydride ligand in 7a; however, it is proposed that two dihydrogen-bonding interactions stabilize the complex. Complexes 1a, 2a, 3a, 4a, 5a, 6a, and 7a were characterized by X-ray crystallography.

A variety of techniques including absorption, magnetic circular dichroism (MCD), variable-temperature, variable-field MCD (VTVH-MCD), and resonance Raman (rR) spectroscopies are combined with density functional theory (DFT) calculations to elucidate the electronic structure of the end-on (η(1)) bound superoxo-Cu(II) complex [TMG(3)trenCuO(2)](+) (where TMG(3)tren is 1,1,1-tris[2-[N(2)-(1,1,3,3-tetramethylguanidino)]ethyl]amine). The spectral features of [TMG(3)trenCuO(2)](+) are assigned, including the first definitive assignment of a superoxo intraligand transition in a metal-superoxo complex, and a detailed description of end-on superoxo-Cu(II) bonding is developed. The lack of overlap between the two magnetic orbitals of [TMG(3)trenCuO(2)](+) eliminates antiferromagnetic coupling between the copper(II) and the superoxide, while the significant superoxo π*(σ) character of the copper dz(2) orbital leads to its ferromagnetically coupled, triplet, ground state.