Abstract:Strontium-doped ZnS nanoparticles (NPs) (1.5, 5 and 9 wt%) were synthesized through a surfactant free hydrothermal method. The structural characterization by X-ray diffraction confirms the synthesis of ZnS, with its two crystalline phases (cubic and hexagonal), without apparition of any peaks related to Sr phases. The crystallite size is affected by Sr doping concentration and was estimated in the range of 2.24-2.51 nm. Furthermore, transmission electron microscopy images show that the NPs have great tendency … Show more
“…We observe a decrease of the phonon energy , see Figure 7 , curves 3 and 4. A similar decrease of is reported in Sr-doped ZnS NPs by Boulkroune et al [ 31 ], where the radius of the Sr ion is larger compared to that of the Zn ion, i.e., there appears a tensile strain similar to the RE ion. Harish et al [ 41 ] have also observed a decrease of the transverse phonon mode with increasing Cu and Ce co-doping concentration.…”
Section: Resultssupporting
confidence: 84%
“…Moreover, there are many published optical studies of different ion-doped (Cu, Mn, Ni, Co, Sr, V, Ag etc.) ZnS nanostructures [ 23 , 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 , 32 , 33 ]. It is reported that the band gap increases with increasing TM doping concentration (Mn, Co, Ni, Cu, Ag, Cd) in ZnS NPs [ 30 ] and decreases with increasing Sr [ 31 ] or RE [ 34 , 35 ] dopants.…”
Section: Introductionmentioning
confidence: 99%
“…ZnS nanostructures [ 23 , 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 , 32 , 33 ]. It is reported that the band gap increases with increasing TM doping concentration (Mn, Co, Ni, Cu, Ag, Cd) in ZnS NPs [ 30 ] and decreases with increasing Sr [ 31 ] or RE [ 34 , 35 ] dopants. It must be noted that there are observed opposite results, for example that decreases with increasing Mn–, Ni– and Co- doping in ZnS thin films [ 29 ] or with increasing Mn doping in ZnS NPs [ 36 ].…”
The surface, size and ion doping effects on the magnetic, phonon and optical properties of ZnS nanoparticles are studied based on the s-d model including spin-phonon and Coulomb interaction, and using a Green’s function theory. The changes of the properties are explained on a microscopic level, due to the different radii between the doping and host ions, which cause different strains—compressive or tensile, and change the exchange interaction constants in our model. The magnetization increases with increasing small transition metal (TM) and rare earth (RE) doping concentration. For larger TM dopants the magnetization decreases. The phonon energies increase with increasing TM, whereas they decrease by RE ions. The phonon damping increases for all doping ions. The changes of the band gap energy with different ion doping concentration is also studied. Band gap changes in doped semiconductors could be due as a result of exchange, s-d, Coulomb and electron-phonon interactions. We have tried to clarify the discrepancies which are reported in the literature in the magnetization and the band gap energy.
“…We observe a decrease of the phonon energy , see Figure 7 , curves 3 and 4. A similar decrease of is reported in Sr-doped ZnS NPs by Boulkroune et al [ 31 ], where the radius of the Sr ion is larger compared to that of the Zn ion, i.e., there appears a tensile strain similar to the RE ion. Harish et al [ 41 ] have also observed a decrease of the transverse phonon mode with increasing Cu and Ce co-doping concentration.…”
Section: Resultssupporting
confidence: 84%
“…Moreover, there are many published optical studies of different ion-doped (Cu, Mn, Ni, Co, Sr, V, Ag etc.) ZnS nanostructures [ 23 , 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 , 32 , 33 ]. It is reported that the band gap increases with increasing TM doping concentration (Mn, Co, Ni, Cu, Ag, Cd) in ZnS NPs [ 30 ] and decreases with increasing Sr [ 31 ] or RE [ 34 , 35 ] dopants.…”
Section: Introductionmentioning
confidence: 99%
“…ZnS nanostructures [ 23 , 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 , 32 , 33 ]. It is reported that the band gap increases with increasing TM doping concentration (Mn, Co, Ni, Cu, Ag, Cd) in ZnS NPs [ 30 ] and decreases with increasing Sr [ 31 ] or RE [ 34 , 35 ] dopants. It must be noted that there are observed opposite results, for example that decreases with increasing Mn–, Ni– and Co- doping in ZnS thin films [ 29 ] or with increasing Mn doping in ZnS NPs [ 36 ].…”
The surface, size and ion doping effects on the magnetic, phonon and optical properties of ZnS nanoparticles are studied based on the s-d model including spin-phonon and Coulomb interaction, and using a Green’s function theory. The changes of the properties are explained on a microscopic level, due to the different radii between the doping and host ions, which cause different strains—compressive or tensile, and change the exchange interaction constants in our model. The magnetization increases with increasing small transition metal (TM) and rare earth (RE) doping concentration. For larger TM dopants the magnetization decreases. The phonon energies increase with increasing TM, whereas they decrease by RE ions. The phonon damping increases for all doping ions. The changes of the band gap energy with different ion doping concentration is also studied. Band gap changes in doped semiconductors could be due as a result of exchange, s-d, Coulomb and electron-phonon interactions. We have tried to clarify the discrepancies which are reported in the literature in the magnetization and the band gap energy.
“…The peaks observe at 290cm -1 , 340cm -1 and 411cm -1 . The peaks around 275cm -1 represents transverse optical (TO) phonon mode as well as peak around 340cm -1 is assigned to longitudinal optical mode (LO) [49][50]. The peaks in between 275cm -1 and 340cm -1 were already reported by previous works and this is the characteristic of the ZnS-NPs [51][52].…”
Zinc Sulphide nanoparticles (ZnS-NPs) are synthesized by microwave assisted chemical precipitation method. The as-synthesized nanoparticles are identified by X ray diffraction and electrical studies to examine the structural transition. The HT-XRD at 1000 C (373 K) and 2000 C (473 K) of ZnS-NPs also confirms structural transition of cubic to hexagonal phase. Thermal properties of the ZnS sample is also studied using thermo gravimetricdifferential thermal analysis (TG-DTA). From D.C. electrical resistance, a discontinuity occurs in the temperature resistance curve of the ZnS-NPs due to phase transition around 450 K. The energy dispersed x-ray analysis and Raman spectra of the ZnS-NPs confirm the presence of zinc and sulphur. The optical studies of the prepared ZnS-NPs are confirmed by its UV-vis and PL spectra. The TEM image of cubic ZnS-NPs reveals the well distribution of spherical shaped particles with mean size of 12.52 nm with standard deviation of 9.326 nm. According to the photocatalytic results of ZnS-NPs for the degradation of methylene blue (MB) have the highest degradation efficiency of 93.24% under UV irradiation within 80 min. Antibacterial effects of ZnS-NPs nanoparticles against some pathogens, like gram-negative, gram-positive, E. coli (Escherichia coli), S. aureus (Staphylococcus aureus) bacteria.
“…The high performance of SrTiO 3 in reaction to heterogeneous photocatalysis requires an effective architecture that maximizes the absorption of photons and reduces electron losses during excitation state (Coleto et al 2019;Ferreira et al 2020).Major efforts are required to further develop heterogeneous photocatalysis of SrTiO 3 under Ultraviolet, visible and solar illumination, in order to further improvement the transfer of charge carriers during excitation state. Actually, interesting and unique features of the binary photocatalyst mechanism have drawn more attention from researchers and have become a favorite subject of research among different groups of scientists across the globe (Ahlem et al 2018;Boulkroune et al 2019;Du et al 2021c, b). It was reported that the properties of the photocatalyst system depend primarily on the nature of the surface properties, the surface morphologies and the role of the optimum amount of doping incorporated in the SrTiO 3 (Hu et al 2020).…”
Understanding the graphene/semiconductor/metal interactions is crucial to design innovative photocatalytic materials with efficient photocatalytic activity for environmental cleanup applications. SrTiO 3 on reduced graphene oxide (rGO) with various graphene contents was successfully synthesized in this study utilizing a simple hydrothermal method, followed by decorating the surface with Ag particles by using the photodeposition process. Under UVvisible light irradiation, the resulting composites were tested for their improved photocatalytic activity to decompose methylene blue (MB). The prepared photocatalysts were characterized by XRD, SEM, EDX, DLS, FT-IR, Raman spectroscopy, and DRS. First-principles density functional theory calculations (DFT) were also carried out by using the generalized gradient approximation (GGA) and PBE functional with the addition of on-site Coulomb correction (GGA + U). The obtained SrTiO 3 /rGO@Ag composites showed great improvement in the photocatalytic performances over pristine SrTiO 3 . For the degradation reaction of MB,SrTiO 3 /rGO 20% @Ag 4% composites yielded the best photocatalytic activity with efficacy reach 94 %, which was also shown that it could be recycled up to four times with nearly unchanged photocatalytic activity.
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