Open Access Article
Priya
Saha
a,
Ryunosuke
Tomita‡
b,
Takao
Tsuneda‡
a,
Pingyu
Jiang
a,
Tetsuya
Taketsugu
ac,
Mingoo
Jin
ad and
Dennis Chung-Yang
Huang
*a
aInstitute for Chemical Reaction Design and Discovery (WPI-ICReDD), Hokkaido University, Japan. E-mail: dcyhuang@icredd.hokudai.ac.jp
bGraduate School of Chemical Sciences and Engineering, Hokkaido University, Japan
cDepartment of Chemistry, Faculty of Science, Hokkaido University, Japan
dList Sustainable Digital Transformation Catalyst Collaboration Research Platform, Institute for Chemical Reaction Design and Discovery (ICReDD List-PF), Hokkaido University, Japan
First published on 17th July 2025
Copper photoredox catalysis has emerged as a practical methodology in organic synthesis, with tetracoordinate copper complexes playing a central role. Among these, homoleptic complexes bearing two bisimine ligands (CuN4) and heteroleptic complexes containing one bisimine and one bisphosphine ligand (CuN2P2) are the most utilized. In contrast, homoleptic copper–bisphosphine complexes (CuP4) have received comparatively less attention, despite their recent involvement in novel synthetic transformations. Herein, we report a systematic study of this underexplored family of copper complexes. Representative CuP4 complexes were synthesized, and their photophysical and electrochemical properties were characterized. Their photocatalytic activity was demonstrated in representative coupling reactions. The results provide insights for guiding future ligand design to develop more active copper-based photocatalysts.
To date, tetracoordinate Cu(I) complexes constitute the most widely applied copper photocatalysts (Scheme 1a).2 Specifically, two classes dominate the field: (i) homoleptic complexes bearing two bisimine ligands (CuN4) and (ii) heteroleptic complexes containing one bisimine ligand and another bisphosphine ligand (CuN2P2).3 These photoactive Cu(I) complexes show outstanding responsiveness to visible light and suitable redox properties, allowing them to engage with a broad range of organic substrates. On the contrary, homoleptic Cu(I)-bisphosphine complexes (CuP4) have not received the same level of attention. Although related compounds have been prepared, there exist only scattered reports on their photophysical properties.4 Furthermore, to the best of our knowledge, applications of these complexes as photocatalysts have not been disclosed until 2022, when the Ngai group demonstrated the effectiveness of Cu(BINAP)2+ as the photocatalyst in an olefin carbo–aroylation reaction (Scheme 1b).5 Very recently, our group communicated Cu-catalyzed defluorinative C–O and C–I coupling reactions, where we showed that Cu(dppbz)2+ can serve as the photocatalyst to reduce trifluoromethylarenes (Scheme 1b).6 A general mechanism is depicted in Scheme 2, where upon photoirradiation, the excited-state CuP4 becomes a potent reductant to undergo a single-electron transfer to the substrate (oxidative quenching). Mesolytic cleavage of the resulting substrate radical anion then affords a radical intermediate, which can be captured for further transformations. The Cu(II) intermediate can then be reduced to regenerate CuP4 and close the cycle. The unique role of bisphosphine ligands in enabling these new photocatalytic reactions thus warrants a systematic study of this overlooked class of photoactive complexes.
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2 ratio, the desired CuP4 could be obtained with dppbz, (R)-BINAP, BIPHEP, DPEphos, and XantPhos ligands in excellent efficiency (1–5). A multigram synthesis of [Cu(dppbz)2+]BF4− (1) was also achieved in 97% yield. The crystal structure of complex 1 and 3, which were obtained by single crystal XRD measurement, are shown in Fig. 1 (see ESI† for other structures). Notably, certain complexes can display dynamic equilibrium between distinct ligation forms. As has been reported previously, [Cu(DPEphos)2+] appears as CuP3 in the solid-state structure bearing one uncoordinated phosphorus atom, whereas the solution 31P-NMR gives rise to only a single peak.4d,j Additionally, [Cu((R)-BINAP)2+] (2) exists exclusively as CuP4 form in CDCl3, but in coordinating CD3CN, CuP2 was observed with additional ligated MeCN moieties. In contrast, [Cu(dppbz)2+] (1) remains as CuP4 in both CDCl3 and CD3CN, consistent with its solid-state structure. On the other hand, in the case of (S)-DTBM-SEGPHOS, presumably due to its steric bulkiness, a CuP2 complex (6) bearing one acetonitrile ligand was produced. Furthermore, when dppf was used as the ligand, an intriguing dinuclear copper complex (7) bridged by a dppf motif was observed in its single crystal structure.4i These outcomes showcase how the ligand identity can have a profound influence on the structures of resulting Cu-complexes.
Upon excitation at 390 nm, multiple peaks could be observed in the emission spectra, noticeably including a broad band at >500 nm (Fig. 2b). Analysis of the emission decay curves revealed that, except for 3, these long-wavelength bands have decay lifetimes greater than 10 μs, suggesting a sufficiently persistent excited state for substrate engagement (Fig. 4, see ESI† for detailed analysis). Quenching experiments further corroborated this proposal.7
Given the intriguingly long decay lifetimes of >500 nm bands in the emission spectra of these CuP4 complexes, we were interested in probing the triplet states by theoretical approaches. Taken [Cu(dppbz)2]+ (1) as an example, we performed TD-DFT calculations at wB97XD/cc-pVDZ/LanL2DZ(Cu) + CPCM(dichloroethane) level of theory. According to theoretical calculations, the photoinduced process can be interpreted to proceed via the following mechanism. First, photoexcitation to the S1 state corresponds to an MLCT transition (Scheme 4). This leads to a decrease in electron density at the copper center, causing a substantial structural rearrangement from the S0 geometry to the stable S1 structure. Concurrently, the oscillator strength decreases markedly, leading to a longer excited-state lifetime. The structural change significantly lowers the S1 excitation energy, and consequently, the T1 excitation energy, which involves a similar electronic transition, is also greatly reduced.8 As a result, upon intersystem crossing from the optimized S1 structure to the T1 state, the T1 excitation energy decreases to 2.44 eV (508 nm). This mechanism is consistent with the experimentally observed broad emission peak ranging from 500 to 700 nm and the 26.4 μs lifetime for complex 1 and may be the key characteristic responsible for its photoredox activity. Importantly, by combining the computationally obtained triplet energy and experimentally measured ground-state oxidation potential, the excited state reduction potential E(CuII/CuI*) can be calculated to be −1.35 V (vs. SCE).9 Note that the Ngai group reported a −1.30 V excited state potential for Cu(BINAP)2PF6 in MeCN.5
Next, hydrodeiodination of aryl iodides, a common model reaction for testing new photocatalysts, was performed (Table 1).11 In the presence of tert-amyl alcohol (t-AmOH) and N,N-diisopropylethylamine (DIPEA), all CuP4 catalyzed the dehalogenation reaction, where [Cu(dppbz)2]+ (1) again afforded the highest yield (entries 1–5). Conveniently, the same efficiency can be achieved from the in situ generated catalyst (entry 6). Control experiments suggest that both t-AmOH and DIPEA can potentially serve as the hydrogen source (entries 7 and 8). Reactions performed in the dark or with 440 nm light resulted in no or diminished yields (entries 9 and 10). On the other hand, an uncatalyzed background reaction proceeded with low efficiency in the absence of copper and ligand (entry 11). A brief scope exploration showed that aryl iodides bearing ester (9) or quinazoline (12) reacted with high efficiency, but the electron-rich, structurally complex 13 is a less competent substrate (Scheme 7). This protocol is also applicable to aryl bromides, although an electron-poor arene is necessary for higher yield (10, 11). The observed scope where more readily reducible substrates afford higher yields, hints that the reducing power of CuP4 complexes is the deterministic factor in this transformation.
| Entry | Conditions | Yielda (%) |
|---|---|---|
| a Determined by 19F-NMR analysis of the crude mixture with (trifluoromethoxy)benzene as the standard. | ||
| 1 | CuP4 = [Cu(dppbz)2]BF4 (1) | 98 |
| 2 | CuP4 = [Cu((R)-BINAP)2]BF4 (2) | 47 |
| 3 | CuP4 = [Cu(BIPHEP)2]BF4 (3) | 24 |
| 4 | CuP4 = [Cu(DPEphos)2]BF4 (4) | 17 |
| 5 | CuP4 = [Cu(XantPhos)2]BF4 (5) | 35 |
| 6 | 10 mol% Cu(MeCN)4BF4 + 20 mol% dppbz | >99 |
| 7 | As entry 6, no t-AmOH | 72 |
| 8 | As entry 6, no DIPEA | 24 |
| 9 | As entry 6, no light, rt or 60 °C | <3 |
| 10 | As entry 6, 440 nm instead of 390 nm LED | 15 |
| 11 | No Cu/L | 14 |
Lastly, we explored the applicability of complex 1 in photocatalytic C–S coupling (Scheme 8). This transformation is known to proceed through the strategy of electron donor–acceptor (EDA) complex,12 thus accounting for the significant background reactivity we observed. In the presence of 1, an improved efficiency was achieved, leading to 92% isolated yield in a 0.50 mmol-scale reaction. The protocol was then successfully applied to the coupling with 2-mercaptobenzothiazole (MBT), a compound used as an accelerant in rubber vulcanization process.
Considering the reduction potentials of substrates examined (e.g. Ered: p-cyanotrifluoromethylbenzene = −1.79 V (ref. 13) and p-fluoroiodobenzene = −2.04 V (ref. 14) vs. SCE), they do not seem to be reducible by the excited state CuP4 (Ered = −1.35 V for 1) from the thermodynamic perspective. Substrate preactivation by salt additives as well as the choice of solvent may make up the discrepancy. Coupling the thermodynamically unfavorable electron-transfer step with favorable downstream processes (e.g. capture of radical intermediates) may drive the reaction forward. Alternatively, a reductive quenching process may take place, where instead the excited Cu(I) first oxidizes a sacrificial reagent (e.g. DIPEA in hydrodehalogenation reactions).15 The resultant Cu(0) then carries out the single-electron reduction of substrates. For complex 1, E(CuI/Cu0) = −2.23 V vs. SCE, showing the ability of [Cu(dppbz)2]0 to reduce most substrates discussed in this section.
Footnotes |
| † Electronic supplementary information (ESI) available. CCDC 2445749–2445753. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d5dt01099c |
| ‡ Equal contribution. |
| This journal is © The Royal Society of Chemistry 2025 |