Marina V.
Volostnykh
ab,
Gayane A.
Kirakosyan
ac,
Anna A.
Sinelshchikova
ah,
Elizaveta V.
Ermakova
a,
Yulia G.
Gorbunova
ac,
Aslan Yu.
Tsivadze
ac,
Sergey M.
Borisov
d,
Michel
Meyer
b,
Lhoussain
Khrouz
e,
Cyrille
Monnereau
e,
Stephane
Parola
f and
Alla
Bessmertnykh-Lemeune
*bg
aFrumkin Institute of Physical Chemistry and Electrochemistry, Russian Academy of Sciences, Leninsky pr. 31-4, Moscow, 119071, Russia
bInstitut de Chimie Moléculaire de l'Université de Bourgogne (ICMUB), UMR 6302 CNRS, Université de Bourgogne, 9 Avenue Alain Savary, BP 47870, 21078 Dijon Cedex, France. E-mail: alla.lemeune@ens-lyon.fr
cKurnakov Institute of General and Inorganic Chemistry, Russian Academy of Sciences, Leninsky pr. 31, Moscow, 119991, Russia
dInstitute of Analytical Chemistry and Food Chemistry, Graz University of Technology, Stremayrgasse 9, 8010 Graz, Austria
eENS de Lyon, CNRS, LCH, UMR 5182, 69342 Lyon Cedex 07, France
fUCBL, ENS de Lyon, CNRS, LCH, UMR 5182, 69342 Lyon Cedex 07, France
gCNRS, ENS de Lyon, LCH, UMR 5182, 69342 Lyon Cedex 07, France
hBCMaterials, Basque Center for Materials, Applications and Nanostructures, UPV/EHU Science Park, 48940 Leioa, Spain
First published on 16th December 2024
Water-soluble porphyrins have garnered significant attention due to their broad range of applications in biomedicine, catalysis, and material chemistry. In this work, water-soluble platinum(II) and palladium(II) complexes with porphyrins bearing ethyl phosphonate substituents, namely, Pt/Pd 10-(ethoxyhydroxyphosphoryl)-5,15-di(p-carboxyphenyl)porphyrins (M3m, M = Pt(II), Pd(II)) and Pt/Pd 5,10-bis(ethoxyhydroxyphosphoryl)-10,20-diarylporphyrins (M1d–M3d; aryl = p-tolyl (1), mesityl (2), p-carboxyphenyl (3)), were synthesized by alkaline hydrolysis of the corresponding diethyl phosphonates M6m and M4d–M6d. NMR, UV–vis, and fluorescence spectroscopy revealed that the mono-phosphonates M3m tend to form aggregates in aqueous media, while the bis-phosphonates M3d exist predominantly as monomeric species across a wide range of concentrations (10−6–10−3 M), ionic strengths (0–0.81 M), and pH values (4–12). Single-crystal X-ray diffraction studies of the diethyl phosphonates Pt6d and Pd6d revealed that π–π stacking of the aromatic macrocycles is sterically hindered in the crystals, providing a rationale for the low degree of solution aggregation observed for ethyl phosphonate M3d. Photophysical studies of M3m and M1d–M3d demonstrated that these compounds are phosphorescent and generate singlet oxygen in aqueous solutions. Pd(II) complex Pd3d is an excellent photocatalyst for the oxidation of sulfides using di-oxygen in a solvent mixture (MeCN/H2O, 4:
1 v/v). Under these conditions, various alkyl and aryl sulfides were quantitatively converted into the desired sulfoxides. For the oxygenation of mixed alkyl–aryl sulfides, Pd3d outperforms Pd(II) meso-tetrakis(p-carboxyphenyl)porphyrin (PdTCPP). This photocatalyst can be recycled and reused to afford sulfoxides with no loss of product yield.
In material and supramolecular chemistry, these compounds have been extensively explored for preparing functional materials for biomedicine15–17 and fabricating oxygen-sensitive membranes,18,19 sensors for volatile organic compounds,20 and photocatalysts for degradation of environmental pollutants.21 A4-type porphyrins are large molecules with D4h symmetry, bearing four peripheral metal-coordinating groups (such as carboxylate, phosphonate, and sulfonate) that serve as excellent precursors for MOFs.22,23 Their high solubility in polar solvents is a mandatory prerequisite for MOF synthesis, which typically requires homogeneous conditions and must be carried out by using metal salts as reagents. Stable and highly porous porphyrin-based MOFs have already been successfully studied as sensors,24 proton-conducting materials,25,26 and catalysts.27–29
To make the inherently hydrophobic aromatic tetrapyrrolic macrocycles soluble in aqueous environments, numerous strategies have been developed, such as introducing specific hydrophilic substituents like pyridinium, sulfonate, or carboxylate groups.30 However, these negatively or positively charged molecules still tend to aggregate in aqueous media, which adversely affects their light absorption, luminescence, and ability to generate singlet oxygen and interact with guest molecules.31–33 To counteract this aggregation, several approaches have been explored. One strategy involves preparing sterically constrained conjugates with hydrophilic residues like sugar34,35 or polyethylene glycol (PEG) moieties,36 or incorporating them into hydrophilic dendrimers.37 Alternatively, the water solubility of hydrophobic porphyrins can also be enhanced by encapsulating them within cyclodextrin cavities,38 forming micelles,39–41 or using other nanoscale organic or inorganic carriers.42
Functionalization of tetrapyrrolic macrocycles through the covalent attachment of hydrophilic residues is generally more convenient compared to supramolecular strategies, especially for biochemistry and catalysis. This is largely because supramolecular assemblies are sensitive to environmental factors and may result in unexpected dissociation in reaction media and loss of activity. Unfortunately, there are still considerable synthetic challenges in the functionalization of the tetrapyrrolic macrocycle by hydrophilic groups. Most substituents are commonly introduced at the meso-positions of the macrocycle because chemoselective modifications at the β-positions remain difficult to achieve. Additionally, hydrophilic porphyrins are often prepared using hydrophobic 1,4-phenylene linkers since direct sulfonation and carboxylation of the macrocycle itself is not feasible.
Recently, it has been shown that diethyl phosphonate groups can be directly attached to the macrocycle in both the meso- and β-positions, affording phosphonate diesters that can be converted into their water-soluble acidic derivatives.43–46 These substituents allow fine-tuning of the hydrophilic–lipophilic balance of the molecules and also significantly impact the electronic structure of the porphyrin macrocycle because of their direct attachment to the aromatic ring. However, the stability of the C–P bond in these sterically bulky compounds is lower compared to that of traditional phosphonic acid diesters, particularly under acidic conditions. This leads to undesirable cleavage of this bond and limits the possibilities for their conversion to the target acids, as dialkyl phosphonates are typically transformed into the corresponding acids under acidic conditions. Our previous research has also demonstrated that porphyrins bearing monoalkyl phosphonate groups, which can be synthesized under basic conditions, are also water-soluble and can be obtained from diesters in high yields.47 To date, only water-soluble Mn(III), In(III), and Ga(III) complexes of this series have been reported.47,48 In this work, the palladium (Pd(II)) and platinum (Pt(II)) complexes M3m and M1d–M3d were obtained and investigated (Fig. 1).
![]() | ||
Fig. 1 Structures of porphyrins M3m and M1d–M3d studied in this work and of the reference compounds M1m, M2m, and MTCPP. |
Robust Pt/Pd porphyrins and related compounds (such as benzoporphyrins, chlorins, bacteriochlorins, and corroles), which incorporate heavy atoms within the macrocyclic cavity, are well known for their ability to produce long-lived triplet states through an excited-state process called intersystem crossing (ISC) when irradiated with visible light.49,50 These triplet states are highly susceptible to dynamic quenching by molecular oxygen, making these complexes highly effective for oxygen sensing.51–54 The generation of reactive oxygen species during this process is used in PDT and photocatalysis.55,56 Additionally, Pt(II) porphyrins have been studied in the development of oxygen microscopy techniques through two-photon-excited phosphorescence.57,58 Pd(II) complexes have also been explored in transition-metal (redox) catalysis.59
In this work, we disclose the efficient synthesis of ethyl phosphonate and bis(ethyl phosphonate) derivatives M3m and M1d–M3d, respectively (Fig. 1), their aggregation behavior in solution, their ability to generate singlet oxygen in aqueous media and their photocatalytic properties. Comparative studies of bis-phosphonates M3d and palladium and platinum meso-tetra(p-carboxyphenyl)porphyrins (MTCPP, M = Pt(II), Pd(II)) revealed that the degree of aggregation in aqueous media is significantly lower for compounds with voluminous phosphonate groups, which are deprotonated over a wide pH range (pH > 4). The metalloporphyrins reported in this work are efficient photosensitizers for generating singlet oxygen and can be used for selective photooxidation of sulfides to sulfoxides.
![]() | ||
Scheme 1 Synthesis of phosphonate esters M3m and M1d–M3d. General conditions and reagents: (i) Pd(OAc)2, CHCl3/MeCN, reflux; (ii) PtCl2, PhCN, reflux, Ar. |
The Pt(II) and Pd(II) complexes M6m and M4d–M6d were obtained using synthetic procedures recently published by us.61 All palladium complexes Pd6m and Pd4d–Pd6d were obtained in high yields (>90%). In contrast, the synthesis of platinum complexes was more challenging, resulting in product yields of 25–57% after chromatographic purification, likely due to the partial decomposition of the porphyrins in boiling benzonitrile.
The hydrolysis of all complexes was carried out using sodium hydroxide in a boiling THF/EtOH/H2O (2:
1
:
1 v/v/v) mixture. Notably, ethanol is more appropriate than methanol to conduct this reaction, as performing the reaction in methanol could lead to partial transesterification of the ethyl phosphonate group, affording an inseparable mixture of products. The reaction course was monitored by MALDI-TOF spectrometry, and heating was stopped immediately after the consumption of the starting compounds. Pure (>90%) complexes M3m and M1d–M3d were isolated by filtration after acidification of the reaction mixtures to a pH below 2.5 with 0.5 M HCl. In the case of methoxycarbonyl-substituted porphyrins M6m and M6d, both the carboxylate ester and the phosphonate diester groups were hydrolyzed under these conditions, yielding three- and tetraanionic complexes M3m and M3d which were isolated in near-quantitative yields.
The structures of the synthesized phosphonate esters M4d–M6d, M3m and M1d–M3d were confirmed by 1H, 13C, and 31P NMR, FT-IR, and HRMS analyses (Fig. S39–S88†). In particular, for the target monoesters M3m and M1d–M3d, a characteristic upfield shift of the phosphorus signal by 3 ppm was observed compared to the diesters M6m and M4d–M6d. This signal was pH-dependent, shifting further upfield by 4 ppm upon the addition of 1 μL of ammonia (25%) to the NMR tube.
![]() | ||
Fig. 2 The asymmetric unit and respective view along the porphyrin plane of Pt6d (A) and Pd6d (B). Thermal ellipsoids are drawn at the 50% probability level. |
Both phosphoryl groups of the porphyrin point in the same direction with respect to the oxygen atoms. However, only one group lies nearly in the mean plane of the porphyrin, forming an intramolecular Cβ–H⋯O hydrogen bond, while the other group is slightly twisted, resulting in a larger distance to the hydrogen Cβ–H and a smaller Cβ–H⋯O angle. The P–O bond distances of 1.454(2)–1.468(2) Å (for PO) and 1.558(4)–1.590(4) Å (for P–O) are typical for diethoxyphosphoryl-substituted porphyrins.44,46 The meso-phenyl substituents exhibit different twist angles (70.5 and 83.5° for Pt6d, 70.7 and 83.6° for Pd6d) with respect to the N4 plane. This difference is attributed to variations of the weak intermolecular interactions in which these substituents are involved in the crystals (Fig. S1†).
In the crystal, the molecules form a slipped columnar structure along the [010] direction, and these columns are arranged in zig-zag chains in the ab plane as shown in Fig. 3, S1 and S2† for Pt6d. Interestingly, the π–π interactions between molecules in the column are weak. The distance between the porphyrin planes is 4.227 Å and tetrapyrrolic macrocycles are significantly shifted relative to each other, forming an angle of 54° between the centroid–centroid line and the normal to the planes. Most of the C⋯C and C⋯N distances between adjacent tetrapyrrolic macrocycles exceed 4.2 Å, short contacts being mainly observed between the hydrogen atoms of phenyl rings and the metal centers of adjacent molecules (Fig. 3 and Table S6†).
![]() | ||
Fig. 3 The crystal packing of two zig-zag chains of Pt6d along [001]. All hydrogen atoms have been omitted for clarity. |
Such M⋯H interactions have been previously reported in Pt(II) and Pd(II) complexes. Pd/Pt⋯H hydrogen bonding distances of 2.2–2.5 Å have been observed in complexes with ligands bearing acidic hydrogens,66–69 while much longer Pd/Pt⋯H distances (3.5–4.0 Å) are typical for ligands containing only C–H bonds available for coordination to metal centers.65,70 Like other weak interactions, these contacts stabilize the lattice and may even influence ligand conformations in the crystal.70
Interestingly, the crystal packing observed for Pd6d and Pt6d is different from that of the less sterically hindered diesters Pd6m and Pt6m bearing a single phosphonate substituent at the tetrapyrrolic macrocycle.61 In the crystal of these compounds, the phosphonate groups of adjacent molecules have opposite orientations which facilitates strong π–π stacking of the aromatic macrocycles. This difference highlights the importance of the second phosphonate group attached to the porphyrin core on the structural organization of supramolecular assemblies and supports the hypothesis that this substituent could play a crucial role in the solution aggregation of these complexes.
![]() | ||
Fig. 4 Aromatic region of VT 1H NMR spectra of Pd3m in D2O. C = 1.5 × 10−3 M, pD ∼ 12. Proton labeling is presented in Fig. 1. |
As shown in Fig. 4, only four sets of signals are observed at 303 K, two partially resolved doublets and two broadened featureless signals. As the temperature gradually increases to 353 K, three additional signals from Hmeso, Hβ7, and Hβ8 are observed. Further heating to 363 K is accompanied by coalescence of the Hβ7 and Hβ8 signals. The COSY NMR spectrum at 348 K shows cross-peaks between pairs of narrow signals, which enables the unambiguous assignment of four of the eight pyrrole moieties and all phenyl protons (Fig. S4†). We attributed the pyrrole protons already observed at 303 K to the rings oriented toward the phosphonate substituents (Hβ2,3) due to the significant downfield shift of one doublet. The remaining pyrrole protons Hβ7,8 and the Hmeso proton do not show resolved peaks, probably because of the aggregation of molecules in the studied solution. The considerable upfield shift (>0.5 ppm) and changes in signal line shapes of the Hmeso and the Hβ7,8 protons located in the meso-unsubstituted part of the porphyrin ring at room temperature indicate that these protons are more strongly affected by the ring-current effect of the π system of adjacent porphyrin compared to the other protons of the macrocycle. Such spectral behavior suggests that J-aggregates with an offset arrangement of macrocycles predominate in the studied solution, which agrees well with the arrangement observed in the crystal structure of corresponding bis-phosphonate diesters M6d. Similar spectral signatures of self-assembly in aqueous media were reported previously for analogous gallium(III) and indium(III) porphyrinates (In3m and Ga3m).47 However, in contrast to In(III) and Ga(III) complexes, heating to 363 K was insufficient to obtain an entirely resolved spectrum of the monomer species.
It is known that addition of alcohol decreases the aggregation of porphyrins in water (H2O).71,72 Therefore, we recorded 1H NMR spectra of Pt3m at 303 K in D2O/CD3OD mixtures of various compositions (Fig. S5†). Indeed, the 1H NMR spectrum of the complex in neat CD3OD was well resolved and the spectral pattern corresponded to the target structure. 2D NOESY NMR experiments (Fig. S6†) allowed all the signals of Pt3m to be assigned. The signals of the Hmeso and Hβ7,8 pyrrole protons located in the unsubstituted part of the porphyrin experienced the largest shifts upon changing the D2O:
CD3OD ratio from 0
:
100 to 100
:
0 v/v. This confirmed the involvement of these protons in the self-assembly process. Similar results were obtained for the corresponding Pd(II) complex Pd3m, which was investigated over the 278–363 K temperature range (Fig. 4 and S7†).
The 1H NMR spectra of the phosphonate-disubstituted complex M3d in D2O (pD ∼ 12) at various temperatures are shown in Fig. 5, S8 and S9.† In this case, no significant (>0.1 ppm) temperature-induced shifts of the signals were observed over the entire temperature range studied (273–363 K), and the spectra displayed well-resolved patterns of the target compounds above 313 K. At lower temperatures (273–313 K), all signals were slightly broadened and showed more pronounced upfield shifts compared to those appearing in the higher temperature region, particularly the phenyl ortho-H and the pyrrole protons adjacent to the phosphonate substituent. This behavior is likely due to a slowdown in the rotation rate of the anisotropic phenyl and phosphonate groups as the temperature decreases. Based on these data, we concluded that only the monomeric species exist in solution at room temperature and that they are predominant across the entire temperature range, although the aggregation of complex M3d in 10−3 M aqueous media at low temperatures cannot be completely ruled out.
![]() | ||
Fig. 5 Aromatic region of VT 1H NMR spectra of Pd3d in D2O. C = 1.5 × 10−3 M, pD ∼ 12. Proton labeling is presented in Fig. 1. |
Compound | Solvent | Absorption | Phosphorescence | Ref. | ||
---|---|---|---|---|---|---|
λ abs (nm) (ε × 10−3 (M−1 cm−1)) | λ em (nm) | Φ em (%) | τ (μs) | |||
a In deoxygenated (by N2 bubbling for 15 min) solutions at C = 1 × 10−6 M. Additional data are presented in Fig. S10–18 and S21.†
b The absolute emission quantum yields were determined with an integrating sphere.
c One drop of aqueous ammonia (25%) was added in the cuvette. T = 298 K.
d Buffered water, [MOPS] = 0.01 M, pH = 7.2, C = 1 × 10−6 M (for UV–vis studies).
e Buffered water/DMF (9![]() ![]() |
||||||
Pt3m | MeOHc | 395 (107), 510 (11), 542 (10) | This work | |||
Buffered H2Od | 667, 731 (sh) | 4.2 | 36 | This work | ||
Pd3m | MeOHc | 407 (151), 522 (18), 553 (12) | This work | |||
Buffered H2Od | 695, 762 (sh) | 0.9 | 248 | This work | ||
Pt1d | Buffered H2O/DMFe | 408 (129), 529 (12), 565 (9) | This work | |||
Pd1d | Buffered H2O/DMFe | 415 (132), 533 (8), 571 (10) | This work | |||
Pt2d | Buffered H2O/DMFe | 401 (153), 521 (9), 558 (14) | This work | |||
Pd2d | Buffered H2O/DMFe | 413 (148), 531 (7), 569 (12) | This work | |||
Pt3d | MeOHc | 400 (87), 525 (7), 560 (25) | This work | |||
Buffered H2O/DMFe | 402 (182), 522 (11), 560 (15) | This work | ||||
Buffered H2Od | 720 | 1.4 | 22 | This work | ||
Pd3d | MeOHc | 414 (174), 532 (10), 568 (10) | This work | |||
Buffered H2O/DMFe | 413 (148), 531 (9), 569 (12) | This work | ||||
Buffered H2Od | 746 | 0.4 | 175 | This work | ||
PtTCPP | Buffered H2O/DMFe | 401 (172), 509 (16) | This work | |||
H2O/ethylene glycol (9![]() ![]() |
403 (184), 510 (17), 539 (4) | 651 | 1.7 | 50 | 73 | |
PdTCPP | Buffered H2Of | 413 (270), 523 (21), 554 (sh) | 701 | 0.9 | 300 | 73 |
PdTSPPg | H2O | 412 (127), 520 (11) | 695, 760 | 0.7 | 350 | 74 |
PdTSBPg | H2Oh | 790 | 2.3 | 310 | 75 | |
PtTSPPi | H2O/ethylene glycol (9![]() ![]() |
402 (133), 510 (14), 540 (6) | 645 | 1.3 | 60 | 76 |
PtTMPyP | H2Oj | 401 (164), 513 (17), 545 (11) | 651 | 0.3 | 2.3 | 76 |
All studied phosphonate-substituted complexes exhibit absorption profiles which are similar to those of their non-phosphonated analogues. In short, the spectra display an intense Soret band and two Q bands, with the absorption maxima of the Pt(II) complexes Pt3m and Pt1d–Pt3d being blue shifted by 4–14 nm compared to those of the analogous Pd(II) porphyrins Pd3m and Pd1d–Pd3d, respectively (Table 1, Fig. 6). The introduction of a second electron-withdrawing phosphonate group into the M3m molecules results in bathochromic shifts (5–26 nm) of all absorption maxima for both the Pt(II) and Pd(II) complexes investigated in this work.
Comparative studies of aggregation in the concentration range of 10−6–10−4 M were conducted for complexes Pt3m and Pt3d in MOPS buffer (Fig. S19 and S20†). The strong aggregation of complex Pt3m in the studied solutions was ascertained by deviations from the Beer–Lambert law and bathochromic shifts of all absorption bands with increasing concentration, which are typical signatures for the formation of J-aggregates. These aggregates were also observed in more concentrated solutions (10−3 M, pH ∼ 12) by NMR spectroscopy, as discussed above.
The aggregation of Pt3m was also studied by UV–vis spectrophotometry. In this case, the ionic strength (μeff) of the solutions was gradually increased by addition of sodium chloride (Fig. S20†). Under such conditions, the Soret and Q bands progressively shifted to high and low energy, respectively, suggesting that the molecular organization of the aggregates depends on the environment and is differently influenced by parameters such as concentration and μeff. Notably, the isosbestic points in the spectra of solutions with μeff ranging from 0.01 to 0.11 mol L–1 suggest that probably only monomeric and dimeric species exist in these solutions.77,78
The spectroscopic behavior of the bis-phosphonate derivatives M3d was different, no deviation from the Beer–Lambert law was observed in the concentration range of 10−6–10−4 M (Fig. S21†) and the spectra remained virtually superimposable when μeff was gradually increased up to 0.81 mol L–1 (Fig. S22†). Notably, meso-tetraarylporphyrins with the p-carboxy- and p-sulfonato-substituted phenyl ring (PdTCPP and PdTSPP) form aggregates under the same conditions, while only the positively charged Pt/Pd tetrakis(N-methyl-4-pyridinium)porphyrins (PtTMPyP and PdTMPyP) stay monomeric in pure water up to 1 × 10−3 M.76,79
Next, we compared the aggregation of Pt3d and PtTCPP at different pH values. Below pH ∼ 4, the absorption spectra of freshly prepared 5.4 × 10−6 M aqueous solutions of Pt3d containing 0.1 M NaCl were found to change over time, the spectral modifications monitored over 3 h being the most pronounced at the lowest examined pH value of 2.5 (Fig. S23†). For the three solutions at pH 4.0, 3.5, and 3.0, the intensity of the Soret and Q bands gradually decreased, while the latter also underwent a bathochromic shift, whereas the baseline drift at wavelengths higher than 600 nm clearly pointed out light diffusion and thus the progressive appearance of particles. At pH 2.5, all these phenomena were amplified, but moreover the Soret band broadened and shifted to lower energy, while the intensity of the low-energy Q band increased in this case. Progressive protonation of the p-carboxyphenyl groups below pH 4 lowers the overall charge and thus the water solubility of the protonated species that tend to slowly aggregate and ultimately precipitate. Hence, a spectrophotometric titration of the soluble tetraanionic Pt3d complex with hydrochloric acid was undertaken from pH 10.65 down to pH 3.57 (Fig. S25†). The absorption spectra were recorded immediately after the addition of the acid aliquots to limit the slow aggregation process occurring below pH 4. The intensity decreases of both the Soret and Q bands together with a concomitant red shift of the latter become significant below pH 5. The isosbestic points at 420, 502, and 541 nm further suggested the formation of a singly protonated porphyrin. Multiwavelength data analysis of the entire dataset (350 ≤ λ ≤ 650 nm; 30 spectra from pH 10.65 to 3.57) using the HypSpec software returned a protonation constant of logK ∼ 3.6. This value has to be taken as approximate, as the spectra between pH 4 and 3.5 might already be slightly off equilibrium, while the protonated fraction reaches only about 50% at the lowest considered pH value. The calculated absorption spectra for [Pt3d]4− and [Pt3dH]3−, the distribution diagram and calculated vs. experimental optical densities at 400 nm are displayed in Fig. S26–28.† Attempts to fit the data with other chemical models ([Pt3d]4− and [Pt3dH2]2−, or [Pt3d]4−, [Pt3dH]3−, and [Pt3dH2]2−) failed as unrealistic electronic spectra were computed for some species. Considering the electron withdrawing effect of the metalloporphyrin ring, the refined log
K value of 3.6 is in rather good agreement with the protonation constant reported for benzoate (log
K = 4.01 at μeff = 0.1 mol L−1, T = 298.2 K) or 4-allylbenzoate (log
K = 4.34 at μeff = 0 mol L–1 or log
K = 4.1 if the value at infinite dilution is extrapolated to μeff = 0.1 mol L−1 using the Davies equation, T = 298.2 K).80
In the case of PtTCPP, broadening of the Soret band and a light-scattering-induced increase of the baseline level were observed in the pH range 3.55–6.37, indicating a high degree of porphyrin aggregation in mild acidic solutions. A well-resolved, pH independent UV–vis absorption spectrum could only be recorded under basic conditions (pH > 8), where the porphyrin exists predominantly as a tetra-anionic species.
Thus, replacement of two p-carboxyphenyl groups of MTCPP by the more acidic and bulky ethyl phosphonate substituents significantly decreases the degree of porphyrin aggregation in aqueous media and enables the concentration, pH, and ionic strength ranges in which porphyrins exist as monomeric species to be widened.
As expected, complexes M3m and M3d are phosphorescent in deoxygenated aqueous solutions (0.01 M MOPS buffer, pH 7.2, RT, Fig. 6). The excitation and ground-state absorption spectra of all the studied compounds are very similar. The maxima of phosphorescence of the Pt(II) complex are shifted to the lower energy regions in comparison with those of the Pd(II) complexes, similar to what was observed for the absorption spectra (Fig. 6 and Table 1). A bathochromic shift of the main emission band by ca. 50 nm and the disappearance of the low energy shoulder typical of only A2B-type porphyrins are observed in the spectra of the bis-phosphonates M3d. No fluorescence is detectable for the Pt(II) complexes and very little fluorescence (Φf < 0.1%), τ = 3.75 ns, for the respective Pd(II) derivatives. Excitation spectra (Fig. S24B†) that were acquired for the fluorescence and phosphorescence bands show the same spectral features as the absorption spectrum (Fig. S24C†) which confirms that the fluorescence indeed originates from the Pd(II) complex and not from an impurity.
The absolute quantum yields (Φem) and luminescence lifetimes (τ) of M3m measured in deaerated MOPS buffer were 2–6.5 times lower (4.2% and 36 μs for Pt3m, 0.9% and 248 μs for Pd3m) compared to the values for dialkyl phosphonates M6m in toluene61 due to water quenching effects.81 The addition of a second phosphonate group at the meso-position of the luminophore molecule decreases Φem by more than 2-fold, and τ decreases by about 1.5-fold. This reduction of both Φem and τ likely reflects the increased probability of non-radiative deactivation processes of the triplet excited state. A similar effect was observed previously for dialkyl phosphonates in toluene.61
Aggregation of M3m at high ionic strength values (0.41 M) is accompanied by a decrease in Φem (Fig. S22†), similarly to Pt(II) and Pd(II) complexes with the H2TCPP ligand.73 In contrast, for the M3d complexes, the intensity of emission was not influenced by ionic strength changes under the same solution conditions, in agreement with the absence of aggregation observed by UV–vis studies.
Comparison of the photophysical properties of the water-soluble complexes reported in this work with those of well-known complexes that have been extensively used in biological experiments (Table 1) enables to conclude that the phosphorylated metalloporphyrins described herein may act as effective PSs for biological applications. Indeed, their photophysical characteristics are comparable to those of other negatively and positively charged water-soluble Pd(II) and Pt(II) complexes. To further validate this, we examined the energy transfer efficiency from the triplet state of M3d to molecular oxygen, resulting in the production of singlet oxygen.
The efficiency of oxygen quenching was investigated by the Stern–Volmer method only for the non-aggregating disubstituted phosphorylated porphyrin Pt3d, because the Pd(II) complex shows low luminescence brightness and a very high sensitivity even at low dioxygen partial pressure (pO2) in solution, making quantitative measurements challenging. A linear dependency of τ0/τ on pO2 in 0.02 M MOPS buffer was observed and the data were treated using the Stern–Volmer equation (Fig. 7). The calculated KSV value for Pt3d was 0.045 hPa−1 (3.66 × 104 M−1), which is comparable to that reported for the water-soluble cationic PtTMPyP(KSV = 2.2 × 104 M−1)82 and anionic PtTCPP (KSV = 7.2 × 104 M−1)83 porphyrins.
![]() | ||
Fig. 7 Stern–Volmer plot for Pt3d in aqueous media. [MOPS] = 0.02 M, pH 7.2, [NaCl] = 0.1 M, T = 298 K. |
To evaluate the photosensitizing efficiency of Pd3d, the quantum yield of singlet oxygen generation was determined by means of the spin-trapping EPR technique. This method is based on comparing the rate of radical production during the reaction of a singlet-oxygen trap, irradiated in aerated solutions containing the target and a reference PS. The EPR approach is particularly advantageous as it enables measurements across a wide range of solvents and even under operando conditions by irradiating samples directly within the EPR spectrometer cavity. However, EPR remains underutilized for quantitative measurements due to instrumental limitations and the potential contribution of side electron-transfer processes involving the singlet-oxygen trap, which can also lead to the formation of observed radicals.55,84 For our measurements in pure water, we used 4-oxotetramethylpiperidine (4-oxo-TEMP) as the singlet-oxygen trap, which has never been used so far for quantitative measurements to the best of our knowledge. In a first attempt, the classical phenalenone was employed as a reference compound. The buildup of the characteristic 4-oxo-TEMPO radical signal was monitored over time, while irradiating with a 365 nm LED the aqueous solutions of this PS and isoabsorbing solutions of PdTCPP or Pd3d. At the selected wavelength, where only a residual absorbance of the porphyrin Soret band is observed, unrealistically high values of singlet oxygen quantum yields (ΦΔ) were obtained for the porphyrins. Thus, in a subsequent series of experiments, we switched to Rose Bengal as the reference compound and used a green LED (530 nm) for irradiation, as the latter wavelength matches well with the porphyrin Q band. Under these revised conditions, all three studied PSs exhibited similar efficiencies in generating singlet oxygen (Fig. S29†), with ΦΔ values of 0.80 and 0.78 for PdTCPP and Pd3d, respectively, assuming ΦΔ = 0.75 for Rose Bengal.85 These values are in good agreement with those previously reported for PdTCPP in an aqueous solution (0.7) with μeff = 0.15 mol L–1 (NaNO3), considering that an increase in ionic strength generally leads to a decrease in ΦΔ in aqueous solutions.86
Thus, the ΦΔ value obtained for Pd3d is comparable to those reported for porphyrins of interest like those used in PDT.50,84,87,88 These results underscore the high potential of the metalloporphyrins evaluated herein as water-soluble phosphorescent oxygen probes and PSs for PDT, as well as for aqueous photocatalytic oxidation reactions for which molecular oxygen is used as a terminal oxidant.
The photodegradation study of complexes M1d–M3d was conducted in a H2O/DMF mixture (9:
1 v/v), where the complexes showed no spectroscopic signs of aggregation in the 10−6–10−4 M concentration range. Solutions of the porphyrins (5 × 10−6 M) were irradiated using an Osram Powerstar HQI BT 400 W lamp (Fig. S37†), and their photobleaching was monitored by vis–NIR absorption spectrophotometry according to the procedure previously reported by us, which allows for semi-quantitative comparisons within a defined series of analogous chromophores.61
As shown in Fig. 8, the rate of porphyrin bleaching strongly depends on the metal centers, with Pt(II) complexes exhibiting in most case greater stability than their Pd(II) analogues. Furthermore, peripheral substituents influence the peculiar shape of the kinetic traces. Among the Pt(II) phosphonate-substituted complexes, only Pt1d, which bears tolyl groups at the macrocycle, degraded more rapidly than PtTCPP. Surprisingly, PdTCPP demonstrated the highest stability among the Pd(II) complexes studied in this work; however, the kinetic traces of all studied Pd(II) complexes were quite similar, particularly for PdTCPP and Pd3d, during the initial stages of photobleaching.
When Pd(II) complexes were studied under the irradiation conditions used hereafter for photocatalytic experiments (425 nm LED, 18 W) in a MeCN/H2O (4:
1 v/v) mixture, the photobleaching exhibited an inverse trend: Pd2d and Pd3d were significantly more stable than PdTCPP, as shown in Fig. S38.† Interestingly, Pd3d demonstrated greater photostability than mesityl-substituted Pd2d, despite the presence of ortho-hydrogen atoms in the aryl substituents of this compound. Overall, these results were encouraging for the practical use of metalloporphyrins synthesized herein, which prompted us to test them as photocatalysts in oxidation reactions.
Among the Pd(II) complexes prepared in this work, tetraanionic Pd3d is particularly interesting due to its high solubility in aqueous media and its efficiency in generating singlet oxygen. Complex Pd2d, featuring two mesityl substituents, also stood out as a photocatalyst of practical interest within the studied series. Previous investigations have shown that porphyrins with perfluorinated or sterically hindered ortho-disubstituted aryl groups at the meso-positions of the macrocycle exhibit superior catalytic activity in oxidation reactions (so-called second-generation catalysts),92,97–99 because of restricted intermolecular processes (such as μ-oxo bridge formation) involved in the photodegradation of the catalyst.
The photocatalytic properties of Pd3d were investigated by oxidizing various sulfides in a MeCN/H2O mixture (4:
1 v/v) under a pure oxygen atmosphere and irradiation with a 425 nm LED (18 W). As shown in Scheme 2, most of the aryl methyl sulfides were transformed to sulfoxides almost quantitively, although with various reaction times, and less than 2% of sulfone overoxidation products were observed in these reactions.
Electron-rich 4-methoxythioanisole and electron-deficient 4-halophenyl- or 4-cyanophenyl methyl sulfides exhibited high reactivity and their oxidation was complete in 1–1.5 h. Bulky ortho-bromothioanisole was oxidized in 2.5 h, which is only 2.5 times longer than the reaction time for para-bromo- and chloro-substituted analogues. 4-Aminophenyl methyl sulfide, which contains an amino group capable of participating in electro-transfer side reactions, also gave excellent results, although the time needed to reach complete conversion was longer (3.5 h) compared to that required for thioanisole oxidation. In contrast, 4-nitrothioanisole, known for its inertness in EnT reactions,100 exhibited a significantly slower oxidation rate, with only 33% conversion after 24 h of irradiation. Dibutyl sulfide also reacted smoothly under these conditions, producing sulfoxide in almost quantitative yields within 3.5 h. Another dialkyl sulfide, cyclic thian-4-one, exhibited lower reactivity but was successfully oxygenated by increasing the photocatalyst loading to 0.09 mol%. Methionine sulfoxide, which has pharmaceutical applications, was obtained in nearly quantitative yield after 3 h of irradiation. Notably, high selectivity in oxidation was observed in the oxygenation of benzyl methyl sulfide, a substrate known to produce by-products due to undesired cleavage of the S–C bond during photocatalytic oxidation in acetonitrile.101 Remarkably, diphenyl sulfide, known102 for its resistance to photooxidation in the presence of PSs due to its low nucleophilicity and steric hindrance, was efficiently oxidized to sulfoxide in 3.5 h. Most of the sulfoxides thus obtained can be easily isolated in pure form (>98%) without additional purification by column chromatography.
Once the oxidation reaction was complete, catalyst recycling was carried out by extracting Pd3d into an aqueous solution at pH 7–8. The photooxidation was performed in MeCN/H2O mixtures with a higher water content (1:
1 v/v) to facilitate the phase separation and avoid the evaporation of the aqueous solution during the work-up process. Five consecutive oxidation reactions of 4-chloroanisole were conducted, yielding the target product almost quantitatively. However, full conversion in the final cycle required 4 h of irradiation, likely due to partial photodegradation of the catalyst during the reaction and some loss of catalyst in each work-up procedure.
Comparative studies of Pd3d and its mesityl analogue Pd2d were performed using diphenyl sulfide, 4-cyanophenyl, and 4-aminophenyl methyl sulfides. Diphenyl sulfide and 4-cyanophenyl methyl sulfide yielded sulfoxides in 3.5 h and 1.5 h, respectively, with both photocatalysts. The oxidation of the electron-rich 4-aminophenyl methyl sulfide proceeded more rapidly with Pd3d, taking only 3.5 h, but required 5 h with Pd2d. Additionally, extraction of Pd2d into an aqueous phase after completion of the reaction was only possible using 0.1 M aqueous sodium hydroxide. Consequently, this preliminary study revealed that Pd3d exhibited more advantageous catalytic features over Pd2d in photooxidation reactions, despite the presence of ortho-H on aryl residues of this compound.
Finally, the photocatalytic properties of Pd3d and PdTCPP were compared using the same series of aryl methyl sulfides (Table S7†). Both photocatalysts demonstrated comparable efficiency in the oxidation of most reactive sulfides; however, electron-poor sulfides systematically reacted more rapidly with Pd3d. For instance, the oxidation of 4-chlorophenyl methyl sulfide proceeded in 1 h with Pd3d, requiring 3.5 h of irradiation with PdTCPP. The irradiation time for diphenyl sulfide was reduced from 8 h to 3.5 h when PdTCPP was replaced by Pd3d.
Comparing the reactivity of different types of sulfides in the presence of Pd3d and PdTCPP, we hypothesized that the sulfoxidation reaction primarily proceeds through the EnT mechanism when PdTCPP is used as a photocatalyst. However, both the EnT and ET mechanisms may be involved when Pd3d is used (Scheme S1†).103–105 To gain a deeper insight into the reaction pathway, the abilities of Pd2d, Pd3d, and PdTCPP to generate singlet oxygen in a MeCN/H2O mixture (4:
1 v/v) were compared. This was a challenging issue to tackle, since no reference compound has been reported for this solvent mixture. We chose phenalenone (PH) as the reference, as its singlet oxygen quantum yield remains in the range of ΦΔ = 0.95–1.00 regardless of the solvent, including pure MeCN and water. Since our EPR experiments with PH were dubious, as discussed above, we employed the fluorescence chemical trapping method using 1,9-anthracenedipropanoic acid (ADPA). Upon irradiation at 395–405 nm of air-saturated solutions containing each complex, the compound selectively reacts with singlet oxygen, forming the corresponding endoperoxide. Monitoring the time course of luminescence decay upon prolonged irradiation gives indirect access to the quantum yield of singlet oxygen generation, as established in our previous work.106
In order to reinforce the validity of the measurements in MeCN/H2O, we used tris(bipyridyl)dichlororuthenium(II) as a model compound, which shares a similar range of excitation wavelengths, and for which the quantum yields of singlet oxygen generation in several solvents are available (ΦΔ = 0.57 in pure acetonitrile107). In this preliminary experiment, we demonstrated that the decrease in ADPA fluorescence, plotted as ln(I0/I) over time, is linear (R2 < 0.995) for both phenalenone and [Ru(bpy)3]Cl2 (Fig. S31†) and yields ΦΔ = 0.51 considering ΦΔ = 0.97 for PH.
UV–vis studies of Pd1d–Pd3d in a MeCN/H2O mixture (4:
1 v/v) at concentrations approximately 2–3 times lower than those used in photocatalytic experiments (Amax < 0.25) demonstrated that these complexes tend to aggregate in this solvent mixture (Fig. S30†). The broadening of the Soret band was most pronounced for Pd1d, but aggregate formation could not be entirely ruled out even for the most hydrophilic Pd3d.
This was evident as the spectrum of the solution prepared from a powdered sample obtained by ultrasonic treatment (trace Pd3d(1) in Fig. 9 and S30†) differed slightly from that of the diluted solution prepared from the aqueous stock solution (trace Pd3d(2) in Fig. 9 and S30†), the former showing less broadening of the Soret band as compared to the latter. Consequently, the ΦΔ values measured for these two solutions of Pd3d were 0.88 and 0.76, respectively (Fig. S32 and S33†). Pd1d and Pd2d were also efficient in generating singlet oxygen, with ΦΔ values of 0.77 and 0.76, respectively (Fig. S34 and S35†), which are both higher than that found for classical PdTCPP (0.58) in the same solvent (Fig. S36†).
Thus, the high efficiency of phosphonate-substituted porphyrins in the sulfide photooxidation can likely be attributed to their superior ability to generate singlet oxygen and high photostability in a MeCN/H2O mixture. However, both Pd2d and Pd3d are efficient in the oxygenation of diphenyl sulfide, a compound known for its negligible reactivity with singlet oxygen. In this particular case, the main reaction pathway likely involves electron transfer. The triplet state of Pd2d and Pd3d may exhibit a higher oxidation potential than PdTCPP due to the electron-withdrawing nature of the phosphonate substituent. If so, these new phosphonate-substituted porphyrins could prove to be more effective photoredox catalysts than PdTCPP.
The complexes thus obtained are quite soluble in basic aqueous media, although their aggregation propensity in solution depends on the number of phosphonate groups appended to the macrocycle. While mono-phosphonates M3m tend to form aggregates similarly to PdTCPP, the bulky bis-phosphonates M3d exist predominantly as monomeric species across a wide range of concentrations, ionic strengths, and pH values (4–12).
Structural studies of the diethyl phosphonate derivatives Pt6d and Pd6d demonstrated that the introduction of a second phosphonate group indeed plays a decisive role in reducing the π–π stacking of adjacent porphyrin molecules in the crystals. This reduction in stacking interactions likely contributes to the decrease in solution aggregation of M3d. Another important structural factor of these compounds is their lower molecular symmetry compared to typical water-soluble porphyrin derivatives bearing four identical meso-aryl substituents, such as aryl-4-carboxylates and aryl-4-sulfonates, which are structurally predisposed to form aggregates in aqueous media due to the formation of multiple electrostatic interactions.
We also demonstrated that the Pd/Pt porphyrins with phosphonate ester groups are phosphorescent in aqueous media, which is an important feature for biomedical or photocatalytic applications. Complexes Pd1d–Pd3d produce singlet oxygen with high efficiency in both MeCN/H2O mixtures and pure water. The platinum complex Pt3d turned out to be an efficient singlet oxygen sensitizer in buffered aqueous solution, comparable to previously reported cationic PtTMPyP4+ and anionic PtTCPP complexes. Therefore, this new family of Pd/Pt porphyrins holds promises for a wide range of practical applications.
In this work, we demonstrated that Pd3d is a more efficient catalyst than PdTCPP for the selective photooxidation of sulfides to sulfoxides. This complex enables faster oxidation reactions under environmentally friendly conditions, utilizing dioxygen as the terminal oxidant and non-chlorinated solvents. Furthermore, this photocatalyst can be easily separated from the products and reused in consecutive catalytic cycles.
Beyond their use as photosensitizers and photoredox catalysts, these compounds are also of interest as precursors of functional materials, because both carboxylic and phosphonic groups are widely used in material chemistry, each serving as an anchor for specific inorganic supports. These compounds are also intriguing linkers for MOF synthesis, which could potentially increase the structural diversity of porous frameworks that have so far been primarily derived from PdTCPP in applied chemistry.
X-ray diffraction experiments were performed at the Center for Shared Use of Physical Methods of Investigation at the Frumkin Institute of Physical Chemistry and Electrochemistry, RAS.
Atomic coordinates have been deposited in the Cambridge Crystallographic Data Centre (the CCDC deposition codes are 2027752 for Pt6d and 2027753 for Pd6d).†
The UV–vis spectra were recorded with a Helios Alpha (Thermo Electron), CARY 50 (Varian), or Jasco V-550 spectrophotometer, using rectangular quartz cells of either 1 or 10 mm optical path length. The ionic strength was adjusted by addition of sodium chloride (NaCl). All solutions were prepared in doubly distilled or deionized water.
Luminescence spectra were recorded on a FluoroLog® 3 spectrofluorometer (Horiba Scientific) equipped with a NIR-sensitive R2658 photomultiplier from Hamamatsu (300–1050 nm). All dye solutions were deoxygenated in a screw-cap cuvette (Hellma) by bubbling high purity nitrogen (99.9999%, Linde Gas, Austria) through the solution for at least 15 min. Absolute quantum yields at room temperature were measured with an integrating sphere from Horiba. The luminescence decay half-times were acquired in the time domain on a FluoroLog® 3 spectrofluorometer equipped with a DeltaHub module (Horiba Scientific) controlling a SpectraLED-392 (λ = 392 nm), using the FluorEssence and the DAS-6 Analysis software for data analysis. Luminescence quenching by molecular oxygen was studied in the same screw-cap cuvette by bubbling gas mixtures through a solution of porphyrin. The composition of the gas mixtures was adjusted with a custom-build gas-mixing device based on mass-flow controllers from Voegtlin (https://www.red-y.com) by mixing the test gas (2% of O2 in N2) and nitrogen (99.9999% purity, both from Linde Gas).
The second set of three solutions, each with an equal absorption value (A = 0.4) at 530 nm, was prepared by dissolving metalloporphyrins and Rose Bengal in water. The measurements were conducted using the same procedure but using a 530 nm LED (Thorlab). The temporal change in 4-oxo-TEMP concentration with time was plotted (Fig. S29†) and the singlet oxygen quantum yields (ΦΔ) were determined using the reported values for Rose Bengal (ΦΔ = 0.75).85
Photostability measurements in MeCN/H2O were performed using a Jasco V-550 spectrophotometer in a rectangular quartz cell (Hellma, 100-QS, 45 × 12.5 × 12.5 mm, 10 mm optical path length, chamber volume 3.5 mL). Isoabsorbing solutions of the studied compounds were prepared, placed in closed vials, and irradiated in the EvoluChem Photoredox box using a blue LED (425 nm, 18 W). The spectra recorded after 3 h of irradiation are presented in Fig. S38.†
This catalyst loading was also used in the kinetic studies (Table S7†) which were performed using the same procedure. The reactions were periodically monitored by NMR spectroscopy after withdrawing aliquot samples.
The experiments with the recycled photocatalyst were performed using the same procedure in a MeCN/H2O mixture (2.5 mL, 1:
1 v/v) using 0.05 mol% of Pd3d. After completion of the reaction, the product was extracted with CH2Cl2 (3 × 5 mL) and the aqueous phase (pH 7–8) containing the photocatalyst was introduced in the next catalytic cycle.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 2027752 and 2027753. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d4dt03068k |
This journal is © The Royal Society of Chemistry 2025 |