How the Way a Naphthalimide Unit is Implemented Affects the Photophysical and -catalytic Properties of Cu(I) Photosensitizers

GRAPHICAL ABSTRACT

GRAPHICAL ABSTRACT

Introduction

The motivation to resolve the conflict between the world’s increasing energy demand and the depletion of fossil fuels drives the search for more environmentally friendly and renewable energy sources (Detz et al., 2018; Gür, 2018; Stephen Nalley, 2021). One of the most attractive alternatives is the enhanced use of solar energy, which can be realized by its conversion and storage in electric energy and different chemical forms (Armaroli and Balzani, 2016; Hammarström, 2016; Lewis, 2016).

In this context, photosensitizers play an essential role, as they are able to harvest the sunlight to subsequently drive various photocatalytic reactions (Schultz and Yoon, 2014; Lewis, 2016; Capaldo and Ravelli, 2020). One the one hand, the high photostability and non-toxicity of semiconductors and, on the other hand, the wide absorption range and low costs of organic dyes attracted great research interests for decades (Lang et al., 2014; Nalzala Thomas et al., 2021). However, the rapid recombination of photogenerated electron-hole pairs and the resulting low photoefficiency of semiconductors as well as the low photostability of organic dyes limit their applicability (Cao et al., 2015; Penu et al., 2015; Chen et al., 2018; Nalzala Thomas et al., 2021; Dong et al., 2022). Therefore, due to the tunable redox and excited state properties of transition-metal complexes, there is an intensive search for efficient and robust transition-metal based photosensitizers (Eckenhoff and Eisenberg, 2012; Frischmann et al., 2013; Berardi et al., 2014; Yuan et al., 2017). Owing to their long-lived excited states, high absorption coefficients in the visible region and intense luminescence, mainly systems containing noble and expensive 4d/5d metals like Pt (Schultz and Yoon, 2014; Teegardin et al., 2016), Ru (Prier et al., 2013; Hagfeldt et al., 2010), Ir (Chi and Chou, 2010; Yuan et al., 2017) or Re (Yarnell et al., 2011; Wells et al., 2021) have been extensively studied.

In recent years, more cost-efficient and noble-metal-free 3d systems, based on for example Cr (Büldt and Wenger, 2017; Treiling et al., 2019; Reichenauer et al., 2021), Fe (Wenger, 2019; Obermeier et al., 2021; Leis et al., 2022) or Cu (Gernert et al., 2020; Schulz et al., 2020; Forero Cortés et al., 2021; Wegeberg and Wenger, 2021), have attracted increasing attention as suitable alternatives to rare metal complexes (Zhang et al., 2018a; Forero Cortés et al., 2021). In particular, heteroleptic copper (I) complexes with the general formula [(P^∧P)Cu(N^∧N)]⁺ bearing a diphosphine and a diimine ligand have been explored well due to their advantageous properties, such as very long-lived excited states (Armaroli, 2001; Kuang et al., 2002; Hagfeldt et al., 2010; Lazorski and Castellano, 2014; Paria and Reiser, 2014; Tsubomura et al., 2015; Heberle et al., 2017; Leoni et al., 2018; Zhang et al., 2018b). As a result, these complexes succeeded in a wide range of applications, including the photocatalytic production of hydrogen (Luo et al., 2013; Kim et al., 2017; McCullough et al., 2018), the activation of CO₂ (Takeda et al., 2016; Call et al., 2019; Steinlechner et al., 2019; Giereth et al., 2021) or as dyes in organic light-emitting diodes (OLEDs) (Volz et al., 2013; Paria and Reiser, 2018; Au, 2021) and dye-sensitized solar cells (DSSCs) (Dragonetti et al., 2018; Dragonetti et al., 2019; Colombo et al., 2021).

As a consequence of their limited absorptivity in the visible region, numerous efforts have been made to modify and to adjust the diimine ligand. For example, several phenanthroline derivatives bearing phenyl and alkynyl substituents (Mejía et al., 2013; Chen et al., 2017; Kim et al., 2017; Zhang et al., 2018a; Doettinger et al., 2021; Forero Cortés et al., 2021) or (diaza)anthracene (Heberle et al., 2017; Soulis et al., 2018; Giereth et al., 2019) moieties were explored, but with limited success. Therefore, in some other studies naphthalene imides were applied as a promising alternative (Tyson et al., 2001; Yarnell et al., 2011; Castellano, 2015; Argüello Cordero et al., 2022). Further, the beneficial features of naphthalimide and diimide derivatives, such as great thermal and oxidative stability, high electron affinity and electron storage capability, are reasons for their widespread use as ligands or building blocks in bichromophoric systems (Castellano, 2015; Georgiev et al., 2016) and in different photocatalytic applications (Suraru and Würthner, 2014; Würthner et al., 2016; Reiß and Wagenknecht, 2019).

Attaching a naphthalimide moiety as an electron acceptor via covalent linkage (i.e., by means of a single bond) to the backbone of an electron donor ligand like phenanthroline can impressively increase the extinction coefficients and excited state lifetimes of the corresponding complexes.(Tyson et al., 2001; Yarnell et al., 2011; Yarnell et al., 2019). As an alternative, recent studies revealed that a direct fusion (e.g., via condensation reactions) of the naphthalene imide moiety to the phenanthroline backbone leads to a fully conjugated system. This resulted in more efficient light absorption far into the visible region and extended lifetimes of up to hundreds of microseconds in the solid state (Yang et al., 2020; Wells et al., 2021; Argüello Cordero et al., 2022).

It is therefore of great interest to test and to compare these two approaches (i.e. covalent linkage vs. directly fusing) using the same type of metal complexes (Scheme 1) and to study the effects on the redox and photophysical behavior as well as on the photoactivity. To this end, we prepared two novel heteroleptic Cu(I) complexes, namely CuNIphen and Cuphen, which are based on the NIphen ligand bearing a covalently linked naphthalimide unit (NIphen = 5-(1,8-naphthalimide)-1,10-phenanthroline) and the mere phen ligand (= 1,10-phenanthroline), respectively (Scheme 1). By comparing these two complexes with the already known Cubiipo, (biipo = 16H-benzo-[4′,5′]-isoquinolino-[2′,1′,:1,2]-imidazo-[4,5-f]-[1,10]-phenanthrolin-16-one) we seek to explore how these three modifications affect the orbital energies of the diimine ligand, and thus, the ³LC and ³MLCT states, as well as the resulting change in redox behavior and charge transfer efficiency. To this end, two novel solid state structures (CuNIphen and Cuphen) are presented and various steady state and time-resolved spectroscopic techniques, electrochemical measurements as well as time-dependent density functional theory (TD-DFT) are applied. Moreover, the new complex was successfully tested over several cycles in the light-driven generation of singlet oxygen (¹O₂). The efficiency of the ¹O₂ generation was examined also considering its continuity and photostability.

SCHEME 1

SCHEME 1. Overview of the chemical structures of the three Cu(I) photosensitizers and the two different design strategies (i.e. covalent linkage vs. directly fusing of a naphthalimide unit) compared in this study. CuNIphen and Cuphen are presented for the first time, whereas Cubiipo was taken from previous studies. (Yang et al., 2020; Argüello Cordero et al., 2022)

Experimental Details

The substituted phenanthroline ligand 5-(1,8-naphthalimide)-1,10-phenanthroline (NIphen) was synthesized following a literature known procedure.Yarnell et al. (2019) 1,10-Phenanthroline (phen) was purchased commercially. The biipo ligand and the corresponding [(xant)Cu(biipo)]PF₆ complex (Cubiipo), where xant corresponds to the xantphos ligand, were required for comparison and taken from previous studies (Yang et al., 2020; Argüello Cordero et al., 2022).

The new heteroleptic copper (I) complexes CuNIphen and Cuphen were prepared via an one-pot, two-step approach, which is already known in the literature (Heberle et al., 2017; Rentschler et al., 2020). For that purpose, the xantphos ligand was first coordinated to the [Cu(MeCN)₄]⁺ (MeCN = acetonitrile) precursor to form the [(xant)Cu(MeCN)₂]⁺ intermediate in dichloromethane (CH₂Cl₂) solution at 40°C under inert conditions (Luo et al., 2013; Mejía et al., 2013). In a second step the respective diimine ligand (NIphen or phen) was coordinated by slow addition of 1 equivalent of the diimine in CH₂Cl₂ solution at 0°C under exclusion of oxygen. In order to increase the yield and purity while facilitating the synthetic efforts at the same time, the literature known procedure was slightly modified for Cuphen as follows: Instead of adding a CH₂Cl₂ solution of phen dropwise by hand via syringe, an automatic syringe pump was used to precisely control the volume flow rate (i.e., 13 ml/h, for further information see Supplementary Material S2). This guarantees the exclusive formation of the heteroleptic target complex in the absence of the respective thermodynamically favored homoleptic bis-diimine complex (e.g., [Cu(phen)₂]⁺) (Kaeser et al., 2013; Fischer et al., 2014; Lennox et al., 2016) and eases the synthesis. After precipitation from the CH₂Cl₂ solution by carefully adding n-hexane, the final yields of the pure bright yellow target compounds were 38% for CuNIphen (after two additional recrystallization steps) and 80% for Cuphen.

Results and Discussion

Structural Characterization

Both complexes were fully characterized by nuclear magnetic resonance (NMR) spectroscopy (¹H, ¹³C, ³¹P), high resolution mass spectrometry (HRMS) and elemental analysis (EA). CuNIphen was further investigated by 2D-NMR spectroscopy, namely H-H nuclear overhauser effect spectroscopy (H-H-NOESY) and heteronuclear multiple bond correlation (HMBC), which allowed accurate assignment of all proton signals (Supplementary Material S2 and S3). In addition, the solid-state structures of CuNIphen and Cuphen were determined by single crystal X-ray crystallography and are compared with molecular structures that resulted from density functional theory (DFT) calculations.

Nuclear Magnetic Resonance

The asymmetric substitution at the 5-position of the phenanthroline ligand causes two separated signals from the two methyl groups in the xantphos backbone at 1.78 ppm (s, 3H, CH₃) and 1.74 ppm (s, 3H, CH₃) in the ¹H NMR spectrum of CuNIphen (Supplementary Figure S1). Similar observations were made for Cubiipo (Argüello Cordero et al., 2022) and other asymmetrically substituted [(xant)Cu(diimine)]⁺ complexes (Schmid et al., 2018). This in strong contrast to the commonly observed single signal at around 1.7–1.8 ppm for the two methyl groups (s, 6H, CH₃) in related symmetrically substituted Cu(I) complexes (Luo et al., 2013; Mejía et al., 2013; Kim et al., 2017; Doettinger et al., 2021) and is also in contrast to the unsubstituted Cuphen complex (1.76 ppm, s, 6H, CH₃) (Supplementary Figure S7). The same splitting phenomenon can also be seen in the ¹³C NMR spectra of CuNIphen and Cubiipo. There, the chemical shifts of both methyl groups are clearly separated (28.60 and 28.20 ppm for CuNIphen, 27.3 and 27.1 ppm for Cubiipo (Argüello Cordero et al., 2022)), whereas in Cuphen only one signal appears (28.55 ppm) (Supplementary Figures S4, S5, S8). By measuring their mutual interactions through space via NOESY, it has now been confirmed that these signals each correspond to one methyl group within the same xantphos ligand framework and are not caused by two different molecular species (Supplementary Figure S2). This is further supported by the HMBC spectrum, where both sets of protons are coupling to the carbon connecting the two methyl groups (Supplementary Figure S3).

The previously discussed findings are, however, no evidence that the two regioisomers do not occur in solution. The asymmetric substitution causes the signals of the o-protons of the phenyl groups on the phosphorus in Cuphen at 6.92 ppm to split into two different sets at 7.01 ppm (4H) and 6.90 ppm (4H) in CuNIphen — two closer (green) and two distal (blue) from the diimine ligand (cf. Figure 1). Both sets exhibit through-space interactions with the protons at the 2- and the 9-position of the phenanthroline (adjacent to N1 and N2 in Figure 1), which is only reasonable if two regioisomers are present (Supplementary Figure S26 for graphical explanation).

FIGURE 1

FIGURE 1. Solid-state structure (two different ORTEP representations) of CuNIphen with thermal ellipsoids at a probability level of 50%. Hydrogen atoms, counter anions, and solvent molecules are omitted for clarity. For comparison with Cuphen, Supplementary Figure S11.

This strongly suggests that indeed both possible regioisomers are formed during complexation and occur in solution. Furthermore, it should be noted that during synthesis (where the diimine ligand is coordinated to the preformed intermediate complex) a differentiation between both possible orientations is unlikely. This conclusion is also supported by DFT calculations, as they predict only a small thermodynamic energy difference of 1.39 kJ/mol between both isomers (Supplementary Figure S26).

X-ray Characterization

To further analyze the structure of the new compounds, single crystals of CuNIphen and Cuphen suitable for X-ray crystallography were obtained by slow diffusion of n-heptane into a concentrated CH₂Cl₂ solution of the respective complex (Supplementary Material S3.3 for further details). CuNIphen (Figure 1) exhibits an intramolecular π-stacking interaction between one phenyl group (green) of the xantphos ligand and the phenanthroline ligand (grey). More precisely, the phenyl ring directly overlays the pyridine moiety opposite to the substituted 5-position due to steric effects (cf. Figure 1, right). Interestingly, a comparable π-stacking interaction is not present in Cuphen, although the unsubstituted 1,10-phenanthroline does not carry a sterically demanding substituent (Supplementary Figure S12). This is most probably due to competing intermolecular interactions in the solid state.

It should be mentioned, that for CuNIphen only one regioisomer was detected in the X-ray crystallographic measurements. In contrast, two regioisomers were found for Cubiipo, which also has an asymmetric structure (Argüello Cordero et al., 2022). However, the structural difference between the two possible regioisomers of CuNIphen is larger than for Cubiipo. This means that Cubiipo possesses a high overall planarity due to the biipo ligand, (Argüello Cordero et al., 2022) whereas in CuNIphen the torsion angle of the substituent is almost 90° as a result of the covalently linked naphthalimide (Table 1), inducing a greater steric bulk. It is therefore likely that one isomer is preferred during the crystallization process. DFT calculations (B3LYP-D3(BJ)/def2-TZVP) were used to predict the structures of CuNIphen and Cuphen (Supplementary Figures S26, S27) simulated in acetonitrile solution. For CuNIphen both possible regioisomers were evaluated and only a small thermodynamic energy difference of 1.39 kJ/mol was predicted, with the structure also observed in the solid state (Figure 1) being energetically favored. The structural parameters obtained from DFT were compared to those from X-ray studies and are in good agreement (Table 1).

TABLE 1

TABLE 1. Selected bond lengths, bond angles and interplanar angles (N-Cu-N vs. P-Cu-P) of Cuphen (top) and CuNIphen (bottom) including the substituent torsion angle (phen vs. naphthalimide). The interplanar angle corresponds to the angle between the two N-Cu-N and P-Cu-P planes, respectively. The bond length C*-N3 describes C-N bond from the phenanthroline to the naphthalimide. The table also compares the experimentally determined parameters (exp.) with those calculated by DFT (denoted italicized as calc.). Further information can be found in the Supplementary Material S3.3).

Concerning the geometry proximal to the copper center, it can be deduced from Table 1 and Figure 1 that Cuphen and CuNIphen both exhibit a distorted tetrahedral geometry (described as interplanar angles) which is common for this class of copper complexes (Leoni et al., 2018; Keller et al., 2020; Doettinger et al., 2021) including Cubiipo (Argüello Cordero et al., 2022). The bond angles (e.g., P1-Cu-P2 and N1-Cu-N2) and bond lengths (Cu-P1 and Cu-N1) are very similar to each other and are in the same dimension as described earlier. Further, also the bond length between the carbon and the nitrogen atoms linking the naphthalimide substituent (C*-N3 = 144.8 p.m., Table 1) is in good agreement with a comparable structure in the literature (144.4 p.m. (Zhang and Ma, 2019). This renders both complexes CuNIphen and Cuphen as structurally closely related compared to similar Cu(I) compounds.

Electrochemical Properties

The electrochemical properties of Cuphen, CuNIphen and the corresponding NIphen ligand were determined by cyclic and differential pulse voltammetry (Figure 2) in acetonitrile solution containing 0.1 M [Bu₄N][PF₆] as electrolyte. The electrochemical data of Cubiipo and biipo are also given for comparison and are summarized in Table 2.

FIGURE 2

FIGURE 2. Cyclic voltammograms (top) and differential pulse voltammograms (bottom) of CuNIphen (dark red, solid, 1 mM), NIphen (red, dashed, 1 mM) and Cuphen (grey, dotted, 1 mM) in acetonitrile solution referenced vs. the ferrocene/ferricenium (Fc/Fc⁺) couple. Conditions: scan rate of 100 mVs⁻¹, [Bu₄N][PF₆] (0.1 M) as supporting electrolyte.

TABLE 2

TABLE 2. | Summary of the photophysical and electrochemical properties of NIphen, CuNIphen, Cuphen and of selected reference compounds in acetonitrile and dichloromethane solution at room temperature. The absorption measurements were carried out in MeCN solution. The electrochemical data were obtained from deaerated acetonitrile solution at room temperature and are referenced vs. the ferrocene/ferricenium (Fc/Fc⁺) couple.

CuNIphen features two reversible reduction waves at −1.62 V and −2.01 V and an irreversible oxidation wave at 0.82 V (dark red, solid). In contrast, Cuphen shows only one reversible reduction at −2.00 V and one irreversible oxidation wave at 0.72 V (grey, dotted). Both oxidation waves are assigned to the Cu(I)/Cu(II) oxidation and the literature-known cleavage of the Cu-P bond (Zhang et al., 2019; Forero Cortés et al., 2021). The NIphen ligand possesses one reversible reduction event at -1.62 V (red, dashed). Hence, the reversible reduction events of CuNIphen can be assigned to the stepwise reduction of 1) the naphthalimide substituent at -1.62 V and 2) the phenanthroline moiety at −2.01 V. This means that, analogous to Cubiipo (Yang et al., 2020; Argüello Cordero et al., 2022), CuNIphen can also be reduced twice and that the covalent linkage of the naphthalimide moiety to the phenanthroline core enables an additional second reduction. The fact that the first reduction event occurs at the distal substituent could also be confirmed by DFT calculations of the spin density of the singly reduced species of CuNIphen ([(xant)Cu(NIphen)]^±0). Identical calculations for Cuphen predicted an increase in electron density at the phenanthroline, which is also in accordance with the experiment (Supplementary Figure S34 for spin density plots and further details).

It should be noted that the differences in the first reduction between the NIphen ligand and the respective Cu(I) complex are very small. In strong contrast, much larger potential differences (∆ = 100 mV) were observed between biipo and Cubiipo (Table 2). This indicates a more pronounced electronic communication between the phenanthroline moiety and the directly fused naphthalimide unit within the biipo system. For the second reduction a much stronger anodic shift was observed for Cubiipo (−2.17 V) compared to CuNIphen (−2.01V). Hence, the twofold reduction of the CuNIphen complex is much easier to perform than of Cubiipo (∆ = 160 mV). All in all, the covalent linkage of a naphthalimide substituent leads to a weaker electronic interaction between the phenanthroline and the naphthalimide moiety, but facilitates access to the doubly reduced species.

Absorption and Steady State Emission Spectroscopy

The UV/vis absorption spectra of CuNIphen, NIphen, and Cuphen show strong features between 250 and 300 nm in acetonitrile solution (Figure 3 and Table 2) originating from ligand centered (LC) π-π* transitions within the phenanthroline ligand, which is also in agreement with the literature (Accorsi et al., 2009; Zhang et al., 2016). The low-energy absorption bands of NIphen between 311 and 365 nm are predominantly due to LC transitions inside the naphthalimide unit (Xiao et al., 2010; Szakács et al., 2019; Yarnell et al., 2019). Cuphen has a broad absorption band centered at 380 nm, which is assigned via TD-DFT calculations to d_Cu→π∗_phen metal-to-ligand charge transfer (MLCT) transitions (Supplementary Figure S29 and Supplementary Table S5). Interestingly, the spectrum of CuNIphen agrees well with the sum of the spectra of NIphen and Cuphen. This confirms the conclusion from the electrochemical measurements, that the electronic communication between both building blocks (i.e., naphthalimide and phenanthroline) is comparatively small. Nevertheless, CuNIphen possesses remarkably increased attenuation coefficients compared to the pure NIphen ligand and the reference compound Cuphen (cf. grey and red spectrum in Figure 3) in both the UV and especially the important visible range.

FIGURE 3

FIGURE 3. Experimental (top, solid lines) and calculated (bottom, dashed lines, B3LYP-D3(BJ)/def2-tzvp) UV/vis absorption spectra of NIphen (light red), CuNIphen (dark red) and Cuphen (grey) in acetonitrile. The inset shows an enlarged region of the absorption from 365 to 480 nm.

In addition, the UV/vis absorption spectra of NIphen and CuNIphen exhibit quite different features when compared to those of biipo and Cubiipo. In the biipo ligand, ligand centered (LC) π-π* transitions from the phenanthroline/imidazole part to the naphthaloylenebenzene moiety were observed in the 360–460 nm range (Yang et al., 2020). The MLCT transitions of Cubiipo overlap with these, resulting in a broad absorption band and high attenuation coefficients (Argüello Cordero et al., 2022). In contrast, the decreased electronic interaction in the covalently linked CuNIphen complex leads to two separated absorption areas at about 310–370 nm (the LC region) and at 370–470 nm (the MLCT region), and thus, lower attenuation coefficients. As a direct consequence of the missing overlap, CuNIphen generally absorbs weaker in the visible range than Cubiipo (Table 2).

In a next step, the steady state emission was studied, where NIphen exhibits a similar behavior in MeCN and CH₂Cl₂ solution with emission quantum yields of 0.057 and 0.034, respectively (Supplementary Figure S17). The moderate emission intensity of NIphen in both solvents indicates efficient intersystem crossing (ISC) from a bright ¹LC to a dark ³LC state (Yarnell et al., 2019). In contrast to NIphen, the emission performance of CuNIphen is strongly solvent dependent. No emission of CuNIphen was observed in MeCN under inert conditions, whereas significant emission was found in deaerated CH₂Cl₂ with a maximum at 669 nm. Similarly, Cuphen displays no emission in MeCN, but a bright emission in CH₂Cl₂. In contrast, Cubiipo is not emissive in both solvents as previously studied. However, some emission is detected in solution due to uncoordinated ligand (Argüello Cordero et al., 2022).

Excited State Properties

The excited states characteristics of NIphen, CuNIphen, Cuphen, and Cubiipo were further studied by time-resolved emission and transient absorption (TA) spectroscopy with an excitation at 355 nm in MeCN and CH₂Cl₂ (Supplementary Material S6).

The emission lifetimes of NIphen in MeCN and CH₂Cl₂ were below the detection limit of our instruments (<10 ns), supporting that the emission of NIphen occurs from a ¹LC state. However, TA spectroscopy revealed much longer lifetimes of the dark excited states of NIphen in MeCN and CH₂Cl₂ (8.40 and 11.04 µs, respectively). The fact that both lifetimes are fairly similar suggests the presence of a ³LC state of the ligand. This is further supported by theoretical calculations via TD-DFT which predicted that the lowest triplet state of NIphen is entirely located on the naphthalimide moiety and should therefore have no charge transfer character (Supplementary Figure S35). (Yarnell et al., 2019) Considering also the moderate quantum yield of NIphen (see above), a population of the lower lying ³LC state is evident.

Next, transient signals could be obtained for the CuNIphen complex which is not emissive in deaerated MeCN. Kinetic analysis of these signals at 462, 468, 474 and 480 nm (Supplementary Figure S24) yielded an averaged exponential time constant of about 19.24 µs, consistent with the results obtained by Yarnell and co-workers (Yarnell et al., 2019). Therefore, in agreement with the results obtained for the NIphen ligand, the final occupied excited state in CuNIphen can be assigned to a dark ³LC state. Remarkably, the introduction of the Cu(I) center more than doubles the lifetime of the ³LC state in CuNIphen (19.24 µs) compared to NIphen (8.40 µs). Interestingly, the excited state lifetime decreases significantly from 19.24 µs in MeCN to 0.37 µs in CH₂Cl₂ (Figure 4), while the latter time is in the same range as for the structurally related Cuphen with 0.50 µs (Table 2). This process occurring in CH₂Cl₂ can therefore most probably be assigned to the depopulation of a ³MLCT state.

FIGURE 4

FIGURE 4. Left: Transient absorption spectra of CuNIphen at 480 nm in MeCN (dark red) and in CH₂Cl₂ (purple) solution under inert conditions excited at 355 nm. Right: Calculated spin density of the optimized lowest triplet state of CuNIphen simulated in CH₂Cl₂ (B3LYP-D3(BJ)/def2-tzvp, CPCM, isosurface value: 0.01). Please note that the identical calculation simulating MeCN (CPCM) yielded similar results (Supplementary Figure S35).

Similar to CuNIphen in MeCN, the long-lived non-emissive component of Cubiipo is attributed to the ³LC state of the biipo ligand with an excited state lifetime of 2.6 µs (Argüello Cordero et al., 2022). However, in CH₂Cl₂ solution Cubiipo still shows no emission and conversely reveals an increase of the time constant to 128.39 µs, which is in strong contrast to the here obtained results for CuNIphen.

Singlet Oxygen Measurements

As known from our previous work, Cubiipo causes a weak ¹O₂ emission in aerated MeCN solution (Argüello Cordero et al., 2022). As evidenced by the TA measurements above, the lifetime of the long-lived component of Cubiipo increases dramatically from 2.6 µs in MeCN to 128.39 µs in CH₂Cl₂. Therefore, it is of great interest to evaluate the singlet oxygen (¹O₂) productivity of Cubiipo and CuNIphen in MeCN and also in CH₂Cl₂. To test the ¹O₂ productivity, the emission quantum yield of ¹O₂ can be observed at about 1276 nm (Schmid et al., 2022; Chettri et al., 2021). For this purpose, phenalenone (PN) is a universal reference compound which can be used in various solvents (Flors and Nonell, 2006; Silva et al., 2013; Trivella et al., 2014; Godard et al., 2020; Kaye et al., 2021; Payne et al., 2022). As expected, the much longer triplet state lifetime of Cubiipo in CH₂Cl₂ greatly enhances the generation of ¹O₂ with singlet oxygen quantum yields of 0.98 with respect to PN (QY_PN(CH₂Cl₂) = 0.98).(Schmidt et al., 1994; Gallavardin et al., 2012; Epelde-Elezcano et al., 2016; Godard et al., 2020). For both CuNIphen and Cuphen, ¹O₂ emission quantum yields of 0.32 and 0.38 were obtained in aerated CH₂Cl₂, which are intriguingly similar (Supplementary Figure S22). These ¹O₂ quantum yields of CuNIphen and Cuphen are in very good agreement with the corresponding ³MLCT lifetimes of 0.37 and 0.50 µs in CH₂Cl₂ (Table 2). This strongly suggests that in the case of CuNIphen and Cuphen the ¹O₂ generation originates from the respective ³MLCT excited state. In addition, CuNIphen was also tested in MeCN, but no singlet oxygen emission was observed under these conditions. One possible reason for this could be that the energy of the excited state does not match with the energy required to convert ³O₂ to ¹O₂ (DeRosa and Crutchley, 2002).

Apart from a high activity, a high photostability is another crucial feature of a photosensitizer, not only for efficient ¹O₂ production, but also for continuous reuse without significant loss of activity (DeRosa and Crutchley, 2002). In this regard, CuNIphen exhibits an outstanding photostability over a period of 8.5 h in inert MeCN and of at least 1 h in aerated CH₂Cl₂ (Supplementary Figures S19, S20). These excellent properties motivated us to investigate the feasibility of continuous ¹O₂ production using CuNIphen in more detail. It is well known, that the use of deuterated solvents leads to much longer ¹O₂ lifetimes and more intense emissions compared to non-deuterated solvents (Bregnhøj et al., 2016), which we have also confirmed for our system (Supplementary Figure S22). Therefore, aerated CD₂Cl₂ was used to study the continuous ¹O₂ generation of CuNIphen. As indicated in Figure 5, CuNIphen produces ¹O₂ with almost constant activity over the course of 12 measurements. Moreover, only an insignificant decrease of the MLCT band (Δ = 1.4%, Figure 5) is observed, possibly due to photo bleaching by in-situ generated singlet oxygen or literature-known photo-induced ligand exchange processes (Kaeser et al., 2013; Fischer et al., 2014; Lennox et al., 2016). As described above, the high photostability of CuNIphen enables an efficient and continuous generation of ¹O₂. These properties of CuNIphen might open the door towards many different applications, such as in photoredoxcatalysis and photodynamic therapy (PDT).

FIGURE 5

FIGURE 5. Left Top: Near-infrared emission spectra of CuNIphen in aerated deuterated dichloromethane solution (CD₂Cl₂) after excitation at 387 nm, showing the characteristic ¹O₂ emission at 1276 nm. The covered cuvette was shaken vigorously three times between each measurement. Left Bottom: Relative integral differences of the recorded ¹O₂ emission. Right Top: UV/vis absorption spectra of the same sample after every second emission measurement. Right Bottom: Relative differences in the absorbance of CuNIphen monitored at 270 (red), 336 (blue) and 400 nm (green), respectively.

Conclusion

In this study, a systematic comparison between two different design strategies, namely between covalently linking and direct fusing of a naphthalimide unit, was performed. To this end, the heteroleptic Cu(I) photosensitizer CuNIphen, bearing a covalently linked naphthalimide substituent, and the unsubstituted reference complex Cuphen were prepared and fully characterized for the first time. The electrochemical, photophysical and catalytic properties were then evaluated in contrast to Cubiipo, which contains a directly fused naphthalimide unit. Analogous to Cubiipo, CuNIphen can be reversibly reduced twice, which means that the naphthalimide unit can accept a second electron. Nevertheless, the electronic communication between the phenanthroline moiety and the covalently attached naphtalimide unit is less pronounced in CuNIphen compared to fused π-system in Cubiipo. With respect to the mere NIphen ligand and the reference complex Cuphen, CuNIphen exhibits a much stronger absorption and increased attenuation coefficients over the whole spectrum.

The excited state features and associated kinetics were systematically investigated by a combination of emission and transient absorption spectroscopy in different solvents. In MeCN solution, CuNIphen exhibits a long-lived excited ³LC state with an excited state lifetime of 19.24 µs. In CH₂Cl₂, however, the lifetime drastically shortens to 0.37 µs, with the corresponding exited state most likely being ³MLCT in nature. In strong contrast to CuNIphen, the corresponding excited state lifetime of Cubiipo increases from 2.6 µs in MeCN to 128.39 µs in CH₂Cl₂, which causes significant changes in the catalytic behavior.

All three Cu(I) complexes were successfully applied in the light-driven formation of singlet oxygen (¹O₂) and the efficiency of ¹O₂ generation was directly evaluated by NIR emission spectroscopy. The resulting ¹O₂ quantum yields are consistent with the different excited state lifetimes from the TA measurements. More importantly, the exceptionally high photostability of CuNIphen enables a continuous ¹O₂ production. Over the course of 12 measurements, only a negligible decrease of the MLCT band (1.4%) of CuNIphen was detected. This renders CuNIphen as a promising candidate for further applications in the conversion of solar energy.

Data Availability Statement

The datasets presented in this study can be found in online repositories. CCDC 2165289 and CCDC 2165279 contain the supplementary crystallographic data for this paper. These data can be obtained free of charge by the Cambridge Crystallographic Data Centre via www.ccdc.cam.ac.uk/structures.

Author Contributions

MK and ST have designed and guided this project. FD prepared and purified the Cu(I) complexes including their structural characterization. YY performed the electrochemical, photophysical and photocatalytic experiments. FD conducted the (TD)-DFT calculations. CK and WF performed the X-ray measurements and solved the structures. YY, FD, MK, and ST analyzed and discussed the data. All authors discussed the scientific results, participated in the preparation of the paper and approved the final version of the manuscript.

Funding

This work was supported by the Deutsche Forschungsgemeinschaft (DFG) within the Priority Program SPP 2102 “Light-controlled reactivity of metal complexes” (KA 4671/2-1 and TS 330/4-1).

Conflict of Interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s Note

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.

Acknowledgments

We thank the analytical service at the Technische Universität Braunschweig for NMR measurements and fruitful discussions. We also like to express our thanks to Bernd Maier for help and initial support with the syntheses of NIphen und CuNIphen. We also greatly acknowledge the group of Prof. Christoph Jacob (Braunschweig) for helpful discussions and access to their compute cluster. We also thank the RWTH Aachen Compute Cluster (project No. 4706) for granting us access to their computation facility. We acknowledge support by the Open Access Publication Funds of Technische Universität Braunschweig.

Supplementary Material

The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/fchem.2022.936863/full#supplementary-material

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