Mirjam R.
Schreier
,
Björn
Pfund
,
Xingwei
Guo‡
* and
Oliver S.
Wenger
*
Department of Chemistry, University of Basel, St. Johanns-Ring 19, 4056 Basel, Switzerland. E-mail: xingwei_guo@mail.tsinghua.edu.cn; oliver.wenger@unibas.ch
First published on 6th August 2020
Many photoactive metal complexes can act as electron donors or acceptors upon photoexcitation, but hydrogen atom transfer (HAT) reactivity is rare. We discovered that a typical representative of a widely used class of iridium hydride complexes acts as an H-atom donor to unactivated olefins upon irradiation at 470 nm in the presence of tertiary alkyl amines as sacrificial electron and proton sources. The catalytic hydrogenation of simple olefins served as a test ground to establish this new photo-reactivity of iridium hydrides. Substrates that are very difficult to activate by photoinduced electron transfer were readily hydrogenated, and structure–reactivity relationships established with 12 different olefins are in line with typical HAT reactivity, reflecting the relative stabilities of radical intermediates formed by HAT. Radical clock, H/D isotope labeling, and transient absorption experiments provide further mechanistic insight and corroborate the interpretation of the overall reactivity in terms of photo-triggered hydrogen atom transfer (photo-HAT). The catalytically active species is identified as an Ir(II) hydride with an IrII–H bond dissociation free energy around 44 kcal mol−1, which is formed after reductive 3MLCT excited-state quenching of the corresponding Ir(III) hydride, i.e. the actual HAT step occurs on the ground-state potential energy surface. The photo-HAT reactivity presented here represents a conceptually novel approach to photocatalysis with metal complexes, which is fundamentally different from the many prior studies relying on photoinduced electron transfer.
We hypothesized that the photochemical hydrogenation of olefins would be an ideal test ground for exploring the photo-HAT reactivity of a metal complex. Whilst alkene hydrogenation is of course an extremely well-developed field, photochemical methods are very scarce and largely limited to substrates with strongly electron-withdrawing substituents to permit typical PET chemistry,28 or to the reduction with solvated electrons.29,30 For the present work, we chose olefins that do not contain electron-withdrawing groups and which therefore cannot be activated by PET due to their very negative reduction potentials (Ered < −2.7 V vs. SCE31). From the perspective of PET, these olefins are unactivated.
HAT is a key process in many photochemical reactions,32,33 but usually requires auxiliary reagents such as thiols or ascorbate which act as H-atom donors in a secondary, light-independent step that does not involve the photosensitizer.34–37 Photoreactions, in which a metal complex donates or accepts an H-atom in an electronically excited state, are rare.33,38–43 For the conceptually related proton-coupled electron transfer (PCET) reactions, there exist numerous compounds which exhibit PCET reactivity from electronically excited states, but these systems typically rely on polar O–H or N–H groups which can form hydrogen bonds.44–47
The HAT reactions considered herein do not proceed directly from an electronically excited state, but instead occur after an initial reductive excited-state quenching process with a tertiary amine. The sequence of reductive excited-state quenching followed by single-electron transfer to the substrate is rather common in organic photoredox catalysis as well as energy-related photochemical research, but here, the situation is conceptually different: reductive quenching leads to an H-atom donor, which can then undergo HAT with olefins. Thermal HAT from metal complexes in their electronic ground state has attracted significant attention48,49 and homolytic splitting of metal-hydride bonds upon excitation with visible light is known for a few selected examples,50,51 but we are unaware of prior reports of photo-triggered HAT from metal complexes to unactivated olefins. The reductive excited-state quenching step involved in our photo-triggered HAT gives access to a particularly reactive metal hydride with a very low M–H bond dissociation free energy (BDFE), and this enables uncommon photochemistry that goes beyond the well-established single electron transfer (SET) reactivity. From the synthetic viewpoint, our approach offers the possibility to form C–H bonds, complementing recent work on photo-triggered PCET that focused on the cleavage of C–H bonds.52,53
Metal hydride complexes play important roles for proton and CO2 reduction,54,55 and recently tungsten hydrides provided fundamental insight into multi-site PCET reactions.56–58 To some extent their reactivity can be regarded as HAT-like, but with coupled proton and electron transfer reactions occurring to separate base and oxidant molecules.22 Iridium cyclopentadienyl hydride complexes are a particularly well investigated class of compounds,59 which have been shown to function as photoacids60 (Fig. 1). Furthermore, they are able to form H2 upon irradiation with visible light61,65 or when used in photo-electrocatalytic settings in water or CH3CN.66 “Self-quenching” reactions, in which an electron is transferred from an excited [Cp*Ir(α-diimine)H]+ complex (Cp* = pentamethylcyclopentadienyl) to an iridium hydride in the ground state, are responsible for photochemical H2 formation in water and CH3CN.67 By contrast, in neat CH2Cl2 the “self-quenching” products (comprised of one oxidized iridium hydride complex and one reduced iridium hydride complex) undergo sequential hydride transfer and HAT, enabling the hydrodechlorination of two equivalents of CH2Cl2 to CH3Cl.64
Fig. 1 Different photo-reactivities: iridium hydrides can undergo excited-state proton transfer60 or photodriven dihydrogen formation.61,65,67 Herein we demonstrate that photo-HAT represents an additional reaction pathway for iridium hydride complexes, complementing recent work demonstrating sequential hydride and HAT transfer.64 |
In the present work, [Cp*Ir(phen)(H)]+ (phen = 1,10-phenanthroline) was formed in situ via photo-irradiation of [Cp*Ir(phen)Cl]+ in CH3CN in presence of excess triethylamine (TEA), which served as a combined electron and proton source. Continued irradiation then promoted [Cp*Ir(phen)(H)]+ to its (relatively long-lived) 3MLCT state. In presence of 250 mM TEA, reductive excited-state quenching to form [Cp*Ir(phen)(H)]0 rather than “self-quenching” is the dominant reaction pathway. For the closely related [Cp*Ir(bpy)(H)]0 complex (bpy = 2,2′-bipyridine), an IrII–H bond dissociation free energy (BDFE) of 43.9 kcal mol−1 was reported previously.67
We anticipated that such a low IrII–H BDFE would make [IrII–H] complexes suitable for olefin hydrogenation via photo-triggered HAT. Activation of olefins by thermal (i.e., not light-driven) metal-hydride catalyzed hydrogen atom transfer (MHAT)48,68 is typically performed with metal-hydrides that have BDFEs ranging from ≈50 to 60 kcal mol−1.70,71 Our results presented below indicate that the key-step in our photoinduced hydrogenation of olefins (Fig. 2) is indeed an initial HAT from the [IrII–H] species to the substrate. After successful activation of the olefin starting material (SM) via photo-triggered HAT, a radical intermediate (RI˙) is formed. The latter can undergo two different onward reactions: (i) either RI˙ can accept a second H-atom to form the hydrogenation product H, or (ii) an H-atom can be abstracted from a different position of radical intermediate RI˙ to give the rearranged products (E)-R or (Z)-R.69,72 In this work, we attempted to maximize the hydrogenation and to minimize the rearrangement yield, but the main point of the study was to establish a new type of photo-reactivity of metal complexes, as noted above.
A very recent study reported on the photoenzymatic hydrogenation of vinyl pyridines, using “ene” reductases in combination with Ru(bpy)3Cl2 as a catalytic system (with some modest product yields also observable in absence of the enzyme).73 Mechanistically, this formal hydrogenation proceeded via a sequence of reduction, protonation and HAT steps. Such combined enzyme-photoredox catalysis approaches hold much promise for enantioselective conversions, but they are not straightforward to implement.74–76
Our iridium complex serves both as photosensitizer and as catalyst of HAT. Due to this dual role, no fine tuning of different catalytic cycles is needed,77 as is sometimes necessary when merging photoredox chemistry with traditional transition metal catalysis or with enzyme catalysts. The hydride complex is formed in situ from a robust Ir(III) precursor complex, and HAT occurs to stable olefin substrates and does not require highly reactive radicals as reaction partners. Thus, alongside the abovementioned very recent study by Miller, Dempsey, and coworkers,64 our work opens a conceptually new avenue to photoredox chemistry, exploiting visible-light excitation of a simple metal complex for inducing H-atom rather than electron transfer.
Entrya | Catalyst | Sacrificial donor | Additive (mol%) | Conversionb [%] | 1-H/1-Rb |
---|---|---|---|---|---|
a Reaction conditions: 1-SM (50 mM), [Cp*Ir(phen)Cl]Cl (2.5 mM), sacrificial donor (250 mM) and 1,10-phenanthroline (0 or 15 mM) in 0.5 mL degassed CD3CN. Irradiation of the sample occurred at 470 nm (7.5 W) for 44 h, while the temperature was kept at 50 °C. See ESI Section 1 for details regarding the photoreactor and ESI Section 3.1 for experimental details. b Conversions and H/R product ratios were determined by 1H-NMR spectroscopy. See ESI Section 3.1.1 for details. c Product formation was confirmed by GC/MS spectrometry. See ESI Section 3.1.2 for details. d Reaction was performed in the dark. | |||||
1 | [Cp*Ir(phen)Cl]Cl | DIPEA | — | 85 | 2.8:1 |
2 | [Cp*Ir(phen)Cl]Cl | TEA | — | 90 | 3.2:1 |
3 | [Cp*Ir(phen)Cl]Cl | TEA | phen (30) | 94 | 14.7:1 |
4 | [Cp*Ir(phen)Cl]Cl | TEA | — | 0 | n.d. |
5 | — | TEA | — | 0 | n.d. |
6 | [Cp*Ir(phen)Cl]Cl | — | — | 0 | n.d. |
Fig. 3 Substrate scope for the photo-triggered hydrogenation of olefins promoted by an iridium hydride. For simplicity, only one isomer of the rearranged products (R) is shown. Reaction conditions: substrate (50 mM), [Cp*Ir(phen)Cl]Cl (2.5 mM), TEA (250 mM) and 1,10-phenanthroline (15 mM) in 0.5 mL degassed CD3CN. Irradiation of the sample occurred at 470 nm (7.5 W) for 44 h, while the temperature was kept at 50 °C, see Section 1 of the ESI† for details regarding the photoreactor. Yields and conversions were determined by 1H-NMR spectroscopy and the yields of the hydrogenation products (1-H to 5-H, 8-H, 9-H and 11-H) were likewise confirmed by GC-MS spectrometry. See ESI Section 3.2† for details. In the case of product 8-R, R means isomerization to cis-1-phenyl-1-propene. In the case of products 6-H/6-R, 10-H/10-R, and 12-H/12-R the product conversion could not be determined by GC-MS spectrometry. Therefore, the yields for these substrates were determined based on 1H-NMR spectroscopy exclusively. |
The conversion of substrate 6-SM with its free hydroxyl-group was considerably lower, affording the hydrogenation product in only 40% yield. This observation suggests that the catalytic turnover is slowed down by coordinating substituents on the substrate, even if the substrate coordinates only weakly and reversibly, as expected for 6-SM. When using the mesityl-substituted substrate 7-SM the reaction was completely shut down. The combined observations made for substrates 6-SM and 7-SM suggest that coordination to the Ir center is undesirable, but sterically very demanding substituents can impede HAT completely.
To explore whether our method can also be applied to internal olefins, trans-1-phenyl-1-propene (8-SM) was tested as substrate, affording propylbenzene (8-H) in 38% yield. The lower conversion of this internal olefin in comparison to terminal olefins is in line with prior studies, which found that an additional methyl substituent at the terminal carbon of 1,1-diphenylethylene slows down the thermal HAT from CpCr(CO)3H to various olefins by about 800 times.78 Furthermore, with 8-SM the formation of the hydrogenation product was less favored than for 1-SM–6-SM. Significant isomerization to cis-1-phenyl-1-propene was observed, whereas no isomerization to the thermodynamically less favored terminal olefin (allylbenzene) was detected.
To gain insight into how the stability of the presumed radical intermediates influences the outcome of the overall reaction, a series of terminal olefins (9-SM–12-SM) with different non-aromatic substituents at the disubstituted olefinic carbon atom was investigated. The hydrogenation yield decreases along the series 1-SM > 9-SM > 11-SM > 12-SM, reflecting the stability of the different radicals formed after initial HAT to these substrates along the substituent series Ph > COOMe > CH3 > H (Fig. 4A).78 Furthermore, the chemoselectivity of the reaction is highly dependent on the stability of the formed radical intermediate. While the hydrogenation product is the major product for all investigated aromatic substrates (1-SM–6-SM), the formation of the rearranged product becomes increasingly important for aliphatic olefins. Specifically, H/R ratios decrease from ca. 15:1 for 1-SM to roughly 2:1 for 9-SM, and finally about 1:3 for 12-SM. This observation reflects the fact that for aliphatic substrates, the newly formed C–H bond in the radical intermediate (RI˙ in Fig. 2) is roughly 10 kcal mol−1 (ref. 82 and 83) weaker compared to aromatic substrates (see ESI Section 4.1† for details). Consequently, H-atom abstraction to yield rearranged products is faster for aliphatic (e.g., 11-SM or 12-SM) than for aromatic substrates (e.g., 1-SM).
Fig. 4 Influence of radical stability and sterics on reactivity of the substrates and product distribution: (A) the conversion of the substrate decreases with decreasing radical stability (reference value: methyl radical = 0 kcal mol−1).84 The chemo-selectivity changes towards the rearranged product when aliphatic substrates are used instead of aromatic substrates. (B) Introducing sterics on the substrates hinders the initial HAT and lowers the reactivity of the substrate, see text for details. |
The very good correlation between the reactivity (and chemoselectivity) of the different substrates and the stability of the formed radical intermediates RI˙ (Fig. 4A) is fully in line with hydrogenation via an initial photo-HAT. The investigated olefin substrates have very negative reduction potentials (below −2.7 V vs. SCE)31 and photoexcited [Cp*Ir(α-diimine)X] species (X = Cl−, H−) do not have this much reducing power (see ESI Section 4.1† for details),67 hence PET is not a viable reaction pathway.
Fig. 6 Role of iridium hydride in the reaction mixture. (A) Comparison of the different reaction time profiles when using [Cp*Ir(phen)Cl]+ (yellow trace) or [Cp*Ir(phen)(H)]+ (green trace). (B) Olefin hydrogenation with [Cp*Ir(phen)(H)](PF6), yields determined by 1H-NMR spectroscopy. The yellow trace in panel A is the same data set as the blue trace in Fig. 5B. |
The electrochemical and chemical conversion of [Cp*Ir(bpy)Cl]+ to [Cp*Ir(bpy)(H)]+ is well established,66,85 but so far does not seem to have been studied in photochemical settings. For related rhodium complexes, the photochemical conversion of chloro- to hydride complexes has been explored to some extent.86–88 When irradiating a 80 μM solution of [Cp*Ir(phen)Cl]+ in CH3CN in presence of 1.0 mM TEA with an LED at 455 nm, the UV-Vis absorption spectrum of [Cp*Ir(phen)Cl]+ converts slowly but steadily to the spectral signature of [Cp*Ir(phen)(H)]+. The series of spectra shown in Fig. S33† were recorded after different irradiation times and have an isosbestic point at 375 nm, in line with expectation based on the UV-Vis spectra of neat [Cp*Ir(phen)Cl]+ and [Cp*Ir(phen)(H)]+.
To probe this conversion under conditions resembling more closely those of the reactions in Section 2.2, 3.5 mM [Cp*Ir(phen)Cl]+ in CD3CN containing 350 mM TEA (but no olefin substrate) was irradiated at 470 nm. The 1H-NMR spectra recorded (in the dark) after photo-irradiation for 2 hours provide clear evidence for the formation of [Cp*Ir(phen)(H)]+ (ESI, Section 4.2†). This set of experiments furthermore demonstrates that prolonged photo-irradiation leads to dissociation of the phen ligand, which explains why the photochemical hydrogenation proceeds better in the presence of excess phen (Table 1).
Presumably, this photoreaction proceeds via an initial reductive dissociation of the chloro-ligand, thereby leading to [Cp*Ir(phen)]0. Protonation of that species (with TEA˙+ as proton source) can then in principle lead directly to the formation of [Cp*Ir(phen)(H)]+, but this is speculative and our data does not provide insight into the individual elementary steps involved in this conversion. Whilst TEA is principally an electron donor, its one-electron oxidized form TEA˙+ is competent to act either as acid or H-atom donor.89
Having established that [Cp*Ir(phen)(H)]+ forms from [Cp*Ir(phen)Cl]+ in the course of continuous photo-irradiation in presence of excess TEA, the next logical step is to elucidate possible onward photochemical reactions of that iridium(III) hydride species. [Cp*Ir(phen)(H)]+ exhibits 3MLCT photoluminescence with a lifetime (τ) of 148 ns in deaerated CH3CN at a [Cp*Ir(phen)(H)]+ concentration of 0.2 mM with 0.6 mM NBu4PF6 at room temperature (Fig. S36†). TEA induces reductive 3MLCT quenching with a rate constant of 4.5 × 108 M−1 s−1 according to Stern–Volmer luminescence quenching experiments (inset of Fig. S36†), thereby leading to the respective iridium(II) hydride, [Cp*Ir(phen)(H)]0.
That iridium(II) hydride species cannot be observed directly by transient absorption spectroscopy, because this is a highly reactive species that does not accumulate in detectable concentrations. However, UV-Vis transient absorption spectroscopy provides unambiguous evidence for a follow-up transient species, namely the iridium(I) complex [Cp*Ir(phen)]0, which forms from the iridium(II) hydride [Cp*Ir(phen)(H)]0 after H-atom release. This iridium(I) species exhibits diagnostic absorption bands near 600 and 640 nm (Fig. 7C, vertical black lines), which are observable after pulsed 445 nm excitation of [Cp*Ir(phen)(H)]+ in presence of excess TEA in CH3CN (Fig. 7A). An analogous experiment with a triarylamine electron donor (TAA-OMe) instead of TEA provides clear evidence for the triarylamine radical cation (absorption band at 720 nm in Fig. 7B/D) superimposed with the spectroscopic signature of the iridium(I) species. Thus, it is clear that both TEA and the triarylamine act as electron donors to the 3MLCT-excited [Cp*Ir(phen)(H)]+ complex.
Fig. 7 (A) Transient absorption spectrum of a solution containing [Cp*Ir(phen)(H)](PF6) (0.5 mM) and TEA (10 mM). The spectrum was measured at a time delay of 60 ns after excitation at 445 nm (9 mJ) and was time-integrated over 100 ns. (B) Transient absorption spectrum of a solution containing [Cp*Ir(phen)(H)](PF6) (0.5 mM) and TAA-OMe (10 mM) in deaerated CH3CN. The spectrum was measured at a time delay of 10 ns after excitation at 445 nm (9 mJ) and was time-integrated over 100 ns. See ESI Section 2.6† for the molecular structure of TAA-OMe. (C) Absorption spectrum of [Cp*Ir(phen)]0 in deaerated CH3CN at room temperature obtained after deprotonation of [Cp*Ir(phen)(H)]+ with KOtBu (1.3 eq.). (D) Absorption spectrum of TAA-OMe˙+ in deaerated CH3CN after chemical oxidation of a TAA-OMe solution (31 μM) with NOBF4 (3.0 eq.). |
In the presence of the olefin substrates, we expect that [Cp*Ir(phen)(H)]0 acts as H-atom donor, leading to the [Cp*Ir(phen)]0 complex and the radical intermediates (RI˙ in Fig. 2). In the transient absorption experiments of Fig. 7, where there is no olefin substrate present, [Cp*Ir(phen)]0 is expected to form via H2 evolution from two equivalents of [Cp*Ir(phen)(H)]0 as illustrated in Fig. S37.† This reaction is exergonic by ca. 16 kcal mol−1.67
When the deuterated substrate (1-SM-d4) was subjected to the standard conditions (see Fig. 3) and the reaction mixture was irradiated for 44 h, both hydrogenation (1-H-d4, 87%) and isomerization (1-R-d3, 6%) products were observed. No formation of 1-SM-d3 was detectable throughout the irradiation process (ESI Section 4.6†). Thus, H-atom abstraction from the radical intermediate (1-RI˙-d4) to form 1-SM-d3 can be neglected. Evidently, secondary HAT (kHAT2) yielding the final hydrogenation product 1-H-d4 as well as isomerization (kR) leading to the rearranged product 1-R-d3 are both faster than reverse HAT (k−HAT1). The fast onward reaction to give preferably the hydrogenation product 1-H-d4 is likely due to the presence of TEA oxidation products such as TEA˙+ or TEA˙.89,92 These highly reactive species presumably serve as the H-atom sources for a secondary HAT to yield the final hydrogenation product.
As noted previously for thermal MHAT, the chemoselectivity of the overall reaction strongly depends on the concentration of the H-atom donor.72 When the concentration of the H-atom donor is relatively high, such as for a system where CpCr(CO)3H was readily regenerated under H2 pressure,78 hydrogenation products are formed preferably. With lower H˙ concentrations, however, which was the case in a previously investigated Co–H/H2 system,72 the rearranged products (1-R-d3) are formed preferably. The preferential formation of hydrogenation products in our study therefore indicates an elevated (local) H-atom donor concentration, presumably due to the presence of iridium hydrides and TEA oxidation products in sufficiently close proximity.
Fig. 10 Proposed reaction mechanism. For simplicity, only the (E)-isomer of the rearranged product is shown. |
Photoexcitation of [Cp*Ir(phen)(H)]+ populates a long-lived 3MLCT excited state (τ of 148 ns at a [Cp*Ir(phen)(H)]+ concentration of 0.2 mM),59,67 which is quenched reductively by TEA with a rate constant of kq = 4.5 × 108 M−1 s−1 to form [Cp*Ir(phen)(H)]0 (ESI Section 4.3†). This iridium(II) hydride is likely the key catalytic intermediate, acting as H-atom donor vis-à-vis the olefin substrates. At the relevant TEA concentrations for our olefin hydrogenations (250 mM), the rate for reductive 3MLCT excited state quenching exceeds the rate for “self-quenching” by at least one order of magnitude.
Direct detection of [Cp*Ir(phen)(H)]0 by transient absorption spectroscopy is not possible, because this is a highly reactive and short-lived species, which does not accumulate in detectable concentrations. Instead, [Cp*Ir(phen)]0, which is formed from [Cp*Ir(phen)(H)]0 after H-atom release, is readily detected (Section 2.4).
Based on previously determined electrochemical potentials for analogous bpy-based (instead of phen-based) iridium complexes, neither the 3MLCT-excited [Cp*Ir(phen)(H)]+ (E0′(IV/III*) ≈ −1.3 vs. SCE,67 ESI Section 4.1†) nor the [Cp*Ir(phen)(H)]0 complex (E0′(III/II) ≈ −1.4 V vs. SCE,67 ESI Section 4.1†) have the reducing power to permit electron transfer to the olefin substrates (Ered < −2.7 V vs. SCE).31 Consequently, olefin hydrogenation cannot occur via a PET pathway (ESI Section 4.1†).
However, [Cp*Ir(phen)(H)]0 exhibits an IrII–H BDFE of approximately 44 kcal mol−1,67 considerably lower than the M–H BDFEs of common MHAT-catalysts, which are typically in the range of 50–60 kcal mol−1.70,71 This very weak IrII–H bond permits an initial HAT to the olefin substrates (ESI Section 4.1†). The achievable hydrogenation yields for the various substrates 1-SM–12-SM reflect the relative stabilities of the involved (charge-neutral) radical intermediates RI˙ (Fig. 4), as expected for HAT. Furthermore, the radical clock experiment (Fig. 8) underpins the radical pathway and speaks against a mechanism involving olefin insertion into the Ir–H bond.
No conversion at all is observed with the sterically demanding mesityl-substituted olefin 7-SM (Fig. 3), suggesting that the catalyst and 7-SM cannot approach sufficiently closely to undergo HAT. The formation of sufficiently intimate contacts, different however from actual substrate ligation to the metal center or olefin insertion into the M–H bond, seems to be a key requirement for successful reaction.
For substrates undergoing successful photo-HAT, the formed radical intermediate (RI˙) can either react via secondary HAT to yield the hydrogenation product (H, top right in Fig. 10) or rearrange to the isomerization product (R, top left in Fig. 10). TEA oxidation products such as TEA˙+ or TEA˙ likely serve as H-atom sources for secondary HAT. Whilst the hydrogenation products (H) are inert and do not react onwards, the rearranged products (R) can be activated via HAT from [Cp*Ir(phen)(H)]0 to re-form radical intermediate (RI˙). Thus, irradiation over extended time periods drives the overall reaction towards the hydrogenation product (Fig. 5B). Excess phen ligand (30 mol%) in the reaction mixture enhances that H/R chemoselectivity by decelerating catalyst degradation and enabling photo-reactions over longer irradiation periods (Section 2.4).
We focused on the photoinduced hydrogenation of relatively simple olefins as a test ground to explore the reactivity patterns of photo-HAT, but prior studies on thermal (i.e., light-independent) reactions established that metal-catalyzed HAT has numerous applications in organic synthetic chemistry.68 Compared to thermal HAT, the photo-HAT with [Cp*Ir(phen)(H)]+ has the advantage that even lower M–H BDFEs (ca. 44 kcal mol−1 for the reductive quenching product [Cp*Ir(phen)(H)]0) are reachable, which stands in contrast to the traditional thermal manner, where most M–H BDFEs are above 50 kcal mol−1.70 This gain in driving force of around ΔΔG ≈ 6 kcal mol−1 can in principle translate to an approximately 104 times faster reaction rate. Very low M–H BDFEs are typically unstable to bimolecular H2 evolution,65–67 but in the presence of 50 mM olefin substrate our hydrogenation reactions proceeded well and exhibited the typical reactivity patterns of HAT.
In our reactions, even aliphatic substrates yielding highly reactive radical intermediates were activated successfully. The investigated olefin substrates have strongly negative reduction potentials (<−2.7 V vs. SCE)31 and therefore cannot be activated easily by the traditional path of photoinduced electron transfer.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0sc01820a |
‡ Current address: Center of Basic Molecular Science (CBMS), Department of Chemistry, Tsinghua University, Beijing 100084, China. |
This journal is © The Royal Society of Chemistry 2020 |