| Literature DB >> 35630941 |
Yuriy Gerasymchuk1, Anna Wedzynska1, Anna Lukowiak1.
Abstract
Bioactive glasses are materials which can be used in medicine for regeneration of hard and soft tissues. Their functionalization with active molecules or addition to composites broaden significantly the possible range of glass applications. Hereby, we describe photoactive nanoparticles of CaO-SiO2-P2O5 glass modified with dichlorohafnium (IV) phthalocyanine. The low-temperature, sol-gel based reverse micelle method was proposed for the synthesis, which allowed introduction of metal organic molecules into the glass composition. The morphology, structure, and composition of the material was described showing that spherical but agglomerated glass nanoparticles (size below 100 nm) were obtained in the ternary system. It was also shown that optical properties of the phthalocyanine complex were maintained after immobilization of the dye in the glass. The photoluminescence and generation of singlet oxygen molecules were observed under the light irradiation of the glass.Entities:
Keywords: dichlorometal-phthalocyanine; medical applications; nanoparticles; optical properties; ternary glass
Year: 2022 PMID: 35630941 PMCID: PMC9146838 DOI: 10.3390/nano12101719
Source DB: PubMed Journal: Nanomaterials (Basel) ISSN: 2079-4991 Impact factor: 5.719
Figure 1X-ray diffraction pattern of the obtained BGl@PcHfCl2.
Figure 2Representative SEM images of BGl@PcHfCl2. Insets show histogram of size particle distribution (a) and initial and final (based on EDX analysis) glass composition (b).
Figure 3FTIR spectrum of BGl@PcHfCl2.
FTIR spectrum signal assignment.
| Signal Maximum (Signal Range) cm−1 | Vibration Assignment | Origin |
|---|---|---|
| 3400 (3000–3680) vw | stretching vibration of O–H bond from the silanol (Si–OH) groups and HO–H vibration of adsorbed water molecules | Glass |
| 1631 w | flexural H–OH bond of adsorbed water molecules | Glass |
| 1511 vw | ν(CNC) + ν(φ) + δ(CH) | Pc macrocycle |
| 1220 sh | PO2– asymmetric/P = O stretching | Glass |
| 1090 sh | asymmetric stretching modes of SiO4 tetrahedra | Glass |
| 1076 vs | symmetric stretching modes of SiO4 tetrahedra | Glass |
| 962 (900–980) sh | υ3–Si–O stretching/PO43− groups | Glass |
| 969 vw | δ(CH) + δ(φ) + ρ(MeN4) | Pc macrocycle + coordinated metal |
| 869 vw | γ(CH) + δ(φ) + δ(CNC) + δ(CN) | Pc macrocycle |
| 797 vw | Si–OH group | Glass |
| 611 vw | asymmetric stretching vibrations of PO43− | Glass |
| 564 w | asymmetric stretching vibrations of PO43−/υ4–P–O bending mode | Glass |
| 467 vw | Si–O–Si rocking/Si–O–Si symmetric bending mode | Glass |
| 446 sh | Si–O–Si rocking/Si–O–Si symmetric bending mode | Glass |
Figure 4(a) Absorption spectrum of glass (BGl@PcHfCl2) in DMSO suspension. (b) Photoluminescence spectra of glass in DMSO and water under UV and red-light excitation. (c) Photoluminescence excitation spectra of glass in DMSO and water. (d) Absorption spectra of glass in DMSO in presence of diphenylisobenzofuran after different time of red-light irradiation (inset shows time-dependent decay of absorption band of DPBF monitored at 417 nm).