Tamara Potlog*a,
Ion Lungu
a,
Mariana Dirua,
Alexandrina Druta
b and
Marius Dobromirc
aLaboratory of Organic/Inorganic Materials for Optoelectronics, Institute of Applied Physics, Moldova State University, Chisinau, Republic of Moldova. E-mail: tpotlog@gmail.com
bDoctoral School “Natural Sciences”, Moldova State University, Chisinau, Republic of Moldova
cAlexandru Ioan Cuza University of Iasi, Research Centre on Advanced Materials andTechnologies, Department of Exact and Natural Sciences, Institute of Interdisciplinary Research, 11 Carol I Blvd., 700506, Iasi, Romania
First published on 8th April 2025
In this study, a new metal oxide NP/MPc derivative composite as efficient photosensitizer for photodynamic therapy of cancer and photocatalytic activities is developed. The ZnPc(COOH)4/MgO composite consists of the synthesized water soluble tetra-carboxy zinc phthalocyanine derivative and magnesium oxide nanoparticles prepared with different precipitating agents. The ZnPc(COOH)4/MgO composites were investigated by UV-Vis spectroscopy and fluorescence spectrophotometry. The absorption and emission spectra of the self-assembled ZnPc(COOH)4/MgO composite highlight the Stokes shift between them, which is near 119 nm. The composites also exhibited room-temperature phosphorescence with an average triplet state lifetime of 5.01 μs and a quantum yield of 10.63%.
In this paper, tetra carboxy ZnPc derivative and MgO NPs are conjugated to form a new ZnPc(COOH)4/MgO nanocomposite. We study the photophysical behavior of the composite which is essential for photosensitizers aimed for use in PDT.
According to the following procedure, 100 mL of magnesium nitrate solution was prepared by dissolving 5 g of Mg(NO3)2·6H2O in deionized water. Separately, 0.288 g of sodium dodecyl sulfate and 0.8 g of NaOH were each dissolved in deionized water. The sodium dodecyl sulfate solution was gradually added in small portions to the magnesium nitrate solution under continuous stirring. Subsequently, the NaOH solution, which facilitates the precipitation reaction, was added dropwise every 3 minutes with constant stirring at a temperature of 70–80 °C for 2 hours. The formation of a white precipitate was observed. Sodium dodecyl sulfate hydrolyzes in aqueous solutions, creating a basic medium:
NaC12H25SO4 → Na+ + C12H25SO4− | (1) |
NaC12H25SO4− → Na+ + C12H25SO4− | (2) |
Magnesium nitrate, a strong electrolyte, dissociates to form magnesium cations and nitrate anions. In a basic medium, magnesium cations precipitate as magnesium hydroxide, resulting in the formation of a white precipitate.
Mg2+ + 2OH ↔ Mg(OH)2↓ | (3) |
The precipitate was filtered through a blue-banded filter paper and washed with 50 mL of distilled water. The precipitate was dried at room temperature, with a synthesis yield of 65%. The residue was calcined at temperatures of 300 °C, 500 °C, and 700 °C. As a result of calcination at temperatures of 300 °C and 500 °C, the residues were brown and black, respectively. It can be concluded that magnesium oxide, which is white in color, was not formed at these temperatures. Calcination at 700 °C led to the formation of a white residue. At this temperature, magnesium hydroxide decomposes according to the reaction equation:
Mg(OH)2 → MgO + H2O | (4) |
A yielding of 1.161 g of the MgO nanoparticles were obtained via a controlled calcination process.
Chitosan has proven to be a highly versatile and effective multifunctional agent in the production and application of metal nanoparticles.37 Therefore, one thousand milligrams of chitosan were dissolved in 100 mL of aqueous solution at 1% acetic acid. The mixture was continuously agitated for 20 hours at 60 °C to obtain the chitosan solution. Later, the prepared chitosan solution was mixed drop by drop with the MgO NPs. The synthesis of chitosan-functionalized MgO is indicated by the color change in the homogeneous solution after 5 hours of continuous stirring. The mixture was then transferred to a hot plate, dried at 100 °C, and calcined for 5 hours at 700 °C in a muffle furnace to produce chitosan-functionalized magnesium oxide nanoparticles. Structure of a chitosan-MgO nanocomposite is shown in Fig. 1a.
Also, it is well known,38,39 that substituted MPcs exhibit promising photosensitizing properties for photodynamic therapy (PDT) of cancer, demonstrating higher photodynamic properties. Solubility is a major challenge for MPcs. The solubility of unsubstituted MPcs is extremely low. Aqueous solutions suitable for spectroscopic and photochemical studies, with concentrations of about 10−6 mol L−1, can only be obtained in DMSO or DMF. The developed tetra carboxy ZnPc derivatives (ZnPc(COOH)4), displayed reasonable photo physicochemical behavior and photodynamic activity in DMSO/H2O.40 The conjugation of ZnPc(COOH)4 to MgO NPs has not been reported in the literature. The current paper employed a method where chitosan was linked to MgO NPs before conjugating to ZnPc(COOH)4.
Finally, 3 mg of (ZnPc(COOH)4), solubilized in 3 mL of deionized water, was added to 0.2 mL of chitosan-surface-modified MgO nanoparticle solution and stirred for 2 hours in the dark. The product was centrifuged at 4500 rpm for 30 minutes, forming the MgO/Ch/ZnPc(COOH)4 assembled system, as illustrated in Fig. 1b and Scheme 1.
Fortunately, peripheral carboxy (–COO−) substituted ZnPcs can be easily prepared to dissolve in aqueous media and form homogeneous solutions.
A Bruker Alpha FTIR spectrometer with a Diamond Crystal ATR accessory was used for rapid compound identification. The chemical composition of the ZnPc(COOH)4/Ch/MgO compounds was further analyzed using an FT-IR 4600 spectrometer (Spectrum Research Systems Co.) in the mid-infrared region, ranging from 4000 to 400 cm−1. X-ray photoelectron spectroscopy (XPS) measurements were performed using a Physical Electronics PHI 5000 Versa Probe instrument, equipped with a mono-chromated AlKα X-ray source (hν = 1486.7 eV).
To enhance the efficacy of photodynamic therapy, we conjugated ZnPc(COOH)4 to MgO/chitosan nanoparticles through the free –OH and –NH2 groups of chitosan.
According to Fig. 1, the conjugation of ZnPc(COOH)4 to MgO/chitosan nanoparticles does not result in change in the position of the bands observed in tetracarboxy ZnPc, except for a modification in the intensity of both bands. The “shoulder” peak is likely an unresolved vibrational-electronic (additional) transition. The splitting of the Q-band results from the overlap of the electronic transitions corresponding to the first two excited states and their associated vibrational levels. The typical assignment for the spectral bands in ZnPc is that the lower-energy peak corresponds to the S1 state (n → π*) and the higher-energy peak to the S2 state (π → π*).
The ZnPc(COOH)4/Ch/MgO solutions, when excited at 360 nm (Fig. 2a), emit electromagnetic radiation (light) as a result of the transition from a higher to a lower electronic energy level.
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Fig. 2 Fluorescence spectra of ZnPc(COOH)4 and ZnPc(COOH)4/Ch/MgO systems excited with λ = 360 nm (a) and λ = 640 nm (b) in water. |
The substitution of ZnPc with COOH groups causes a shift in the emission wavelength compared to pure ZnPc. The emission spectrum of ZnPc(COOH)4 in water shows a broad, high-intensity emission band at 465 nm. According to the Franck-Condon principle, if a particular transition probability between the fundamental and 1st vibrational levels is the highest in absorption, the reverse transition is also most probable in emission.41
The emission and absorption transitions appear as mirror images if they correspond to electronic transitions between the same two states and if no significant molecular configuration changes occur in the excited state. The generally symmetric nature of these spectra results from the involvement of the same transitions in both absorption and emission and the similar vibrational energy levels of the S0 and S1 states.
For the ZnPc(COOH)4/Ch/MgO self-assembled system, the primary emission band shifts to 479 nm, and an additional, weaker band appears at 707 nm. The fluorescence spectrum occurs at longer wavelengths than the absorption, a shift caused by energy losses due to the vibrational relaxation in the excited state. The difference between the absorption and the fluorescence maxima, known as the Stokes shift, is 105 nm for ZnPc(COOH)4 and 119 nm for the ZnPc(COOH)4/Ch/MgO system.
For the conjugated system excited at 640 nm, presented in Fig. 2b, additional lower-intensity bands also appear at 708 nm and 782 nm. When excited at 640 nm, only the ZnPc(COOH)4/Ch/MgO systems exhibit the same emission bands at 708 nm and 782 nm, as observed with 360 nm excitation. The fluorescence intensity of ZnPc(COOH)4/Ch/MgO increases significantly due to the intramolecular proton transfer between the ZnPc(COO−)4 and the NH3+ groups of the MgO/chitosan nanoparticles.
Another notable feature in all prepared solutions is the emission band at 828 nm, likely resulting from excited-state reactions, complex formation, and/or charge-transfer complexes involving amines.
The fluorescence lifetime of the ZnPc(COOH)4 and ZnPc(COOH)4/Ch/MgO systems is presented in Fig. 3. The excitation wavelength was λex = 365 nm, and the emission wavelength was set at 338 nm. ZnPc(COOH)4 in an H2O solution displays a bi-exponential decay, clearly indicating the presence of two distinct species populations. Lifetimes were estimated to use the least squares fitting technique with a bi-exponential decay model. The fluorescence decay for each sample was fitted to the following bi-exponential function:
![]() | (5) |
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Fig. 3 Fluorescence lifetime spectra of the ZnPc(COOH)4 and ZnPc(COOH)4/Ch/MgO self-assembled systems in water. |
The quality of the fit was evaluated using the reduced chi-square (χ2) test and deviation function criteria. After fitting the intensity decay curves, the extracted lifetime values are presented in Table 1.
Samples | Fluorescence | |||||
---|---|---|---|---|---|---|
τ1, ns | τ2, ns | τav, ns | Relτ1, % | Relτ2, % | Φ, % | |
ZnPc(COOH)4 | 1.50 | 4.44 | 2.97 | 25.22 | 74.78 | 21.17 |
ZnPc(COOH)4/Ch/MgO (LS-2-4) | 1.31 | 4.21 | 2.76 | 24.08 | 75.92 | 4.21 |
ZnPc(COOH)4/Ch/MgO (AV-2-1) | 1.59 | 4.21 | 2.90 | 25.85 | 74.15 | 4.24 |
ZnPc(COOH)4/Ch/MgO (AV-3-1) | 1.31 | 4.06 | 2.66 | 18.11 | 81.89 | 3.99 |
As summarized in Table 1, both the ZnPc(COOH)4 and ZnPc(COOH)4/Ch/MgO systems in water exhibit two characteristic fluorescence lifetimes with an average lifetime of approximately 3 ns, slightly higher for the self-assembled system. The concentration of ZnPc(COOH)4 in water and in all ZnPc(COOH)4/MgO/Ch/systems is 2 mg mL−1. The absolute quantum yield of fluorescence of ZnPc(COOH)4 reaches 21.17%, while for ZnPc(COOH)4/Ch/MgO systems, it decreases to approximately 4%.
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Fig. 4 Phosphorescence spectra of the ZnPc(COOH)4 and ZnPc(COOH)4/Ch/MgO self-assembled systems in water and the triplet excited state lifetimes of these systems. |
The triplet excited state lifetime of the ZnPc(COOH)4 and ZnPc(COOH)4/MgO/Ch systems, under 355 nm excitation, displays a bi-exponential decay. The corresponding lifetime values are presented in Table 2. For the ZnPc(COOH)4/MgO/Ch system, the highest lifetime value of approximately 5 μs was recorded. The phosphorescence quantum yield of this system reaches 10.63%.
Samples | Phosphorescence | |||||
---|---|---|---|---|---|---|
τ1, μs | τ2, μs | τav, μs | Relτ1, % | Relτ2, % | Φ, % | |
ZnPc(COOH)4 | 1.04 | 8.47 | 4.76 | 57.67 | 42.33 | 3.20 |
ZnPc(COOH)4/Ch/MgO (LS-2-4) | 1.16 | 8.89 | 5.03 | 63.01 | 36.99 | 10.63 |
ZnPc(COOH)4/Ch/MgO (AV-2-1) | 1.13 | 8.83 | 4.98 | 61.39 | 38.61 | 0.01 |
ZnPc(COOH)4/Ch/MgO (AV-3-1) | 1.06 | 8.53 | 4.76 | 59.65 | 40.35 | 2.27 |
To summarize, the present study facilitates the development of new sustainable room-temperature phosphorescent materials. This result indicates that the interaction between ZnPc(COOH)4 and MgO/Ch was strong, which was beneficial for restricting the molecular vibrations of MgO/Ch and promoting room-temperature phosphorescence emission. Room-temperature phosphorescence offers several significant advantages for optical detection, including enhanced selectivity and sensitivity, longer emission lifetimes, and a greater spectral shift between excitation and emission spectra. The extended lifetime of the triplet excited state facilitates the development of relatively inexpensive detection systems based on decay time measurements.
It is shown that the triplet energies can be determined based on the strong spin–orbit coupling of Zn2+ ions: the first triplet energy can be evaluated by observing spin-forbidden singlet–triplet (S0–T1) absorption, whereas the second triplet energy was determined by intersystem crossing.
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