Abstract:This work gives the evidence of the lattice contraction in CdSe nanocrystals (NCs) grown in a glass matrix. The CdSe NCs were investigated by atomic force microscopy (AFM), optical absorption (OA), and Raman spectroscopy. The average size of CdSe NCs can be estimated by AFM images. Using the OA spectra and the effective-mass approximation, it was also possible to estimate the average sizes of CdSe NCs, which agree very well with the AFM data. These results showed that the CdSe NCs grow with increasing time of … Show more
“…Figure 1a shows that the undoped CdS QDs (x = 0.000) exhibit confinement energy ( conf E ) as indicated by the OA band peak at ~3.10 eV. From this value and using a confinement model based on effective mass approximation [12,[15][16][17][18], the mean QD radius R was estimated by the expression: Econf = Eg + (ħ 2 π 2 ⁄ 2 R 2 ) -1.8(e 2 ⁄ εR), where Eg is the bulk material energy gap, is the reduced effective mass, e is the elementary charge, and ε is the dielectric constant. From this, a mean radius of about R~2.0 nm was estimated for the CdS QDs, thus confirming strong size quantum confinement [16].…”
Section: Carrier Dynamicsmentioning
confidence: 99%
“…However, a recent study of thermal treatments on undoped CdSe QDs [12] embedded in this same glass matrix (SNAB) showed a much smaller redshift (~0.03 eV) when annealed for 6 h. Since CdSe and CdS structures display great similarities, as well as Cd1-xMnxS with dilute Mn-concentration, it is reasonable to assume that they have the same growth kinetic in the same glass matrix. Thus, the higher shift (~0.05 eV) observed in Cd0.900Mn0.100S QDs annealed for 6 h provides strong evidences that the observed higher redshift must also be ascribed to a decrease of the effective concentration of Mn 2+ incorporated to the dots, and this decrease takes place during the thermal treatment of the sample.…”
Section: Magneto-optical Propertiesmentioning
confidence: 99%
“…Cd1-xMnxS NPs were successfully synthesized in this glass matrix by adding 2[CdO + S] (wt % of SNAB), and x[Mn] (wt % of Cd), with x = 0.0, 0.5, 5.0, and 10 %. The synthesis method consists in a two sequential melting-nucleation approach, in which it is possible obtain ensembles of nearly spherical nanoparticles embedded in a glass matrix [12]. First, the powder mixture was melted in an alumina crucible at 1200 ºC for 30 minutes.…”
Section: Synthesis Of Cd1-xmnxs Nanoparticles In a Glass Matrixmentioning
confidence: 99%
“…It is well known that the optical properties of NPs can be significantly changed by interactions between nanostructures and their host material, due mainly to the formation of surface defects [11,12]. These surface defects are heavily dependent on NP size and become more important with increasing surface-volume ratio.…”
“…Figure 1a shows that the undoped CdS QDs (x = 0.000) exhibit confinement energy ( conf E ) as indicated by the OA band peak at ~3.10 eV. From this value and using a confinement model based on effective mass approximation [12,[15][16][17][18], the mean QD radius R was estimated by the expression: Econf = Eg + (ħ 2 π 2 ⁄ 2 R 2 ) -1.8(e 2 ⁄ εR), where Eg is the bulk material energy gap, is the reduced effective mass, e is the elementary charge, and ε is the dielectric constant. From this, a mean radius of about R~2.0 nm was estimated for the CdS QDs, thus confirming strong size quantum confinement [16].…”
Section: Carrier Dynamicsmentioning
confidence: 99%
“…However, a recent study of thermal treatments on undoped CdSe QDs [12] embedded in this same glass matrix (SNAB) showed a much smaller redshift (~0.03 eV) when annealed for 6 h. Since CdSe and CdS structures display great similarities, as well as Cd1-xMnxS with dilute Mn-concentration, it is reasonable to assume that they have the same growth kinetic in the same glass matrix. Thus, the higher shift (~0.05 eV) observed in Cd0.900Mn0.100S QDs annealed for 6 h provides strong evidences that the observed higher redshift must also be ascribed to a decrease of the effective concentration of Mn 2+ incorporated to the dots, and this decrease takes place during the thermal treatment of the sample.…”
Section: Magneto-optical Propertiesmentioning
confidence: 99%
“…Cd1-xMnxS NPs were successfully synthesized in this glass matrix by adding 2[CdO + S] (wt % of SNAB), and x[Mn] (wt % of Cd), with x = 0.0, 0.5, 5.0, and 10 %. The synthesis method consists in a two sequential melting-nucleation approach, in which it is possible obtain ensembles of nearly spherical nanoparticles embedded in a glass matrix [12]. First, the powder mixture was melted in an alumina crucible at 1200 ºC for 30 minutes.…”
Section: Synthesis Of Cd1-xmnxs Nanoparticles In a Glass Matrixmentioning
confidence: 99%
“…It is well known that the optical properties of NPs can be significantly changed by interactions between nanostructures and their host material, due mainly to the formation of surface defects [11,12]. These surface defects are heavily dependent on NP size and become more important with increasing surface-volume ratio.…”
“…Finally, as a result of the thermal annealing, dilute Zn 1Àx Mn x Te NCs were formed in the PZABP matrix. Other details on the nanoparticles growth in glass matrices by the fusion method can be found in literature [3,[13][14][15].…”
Optical phonon modes, confined in CdS x Se 1−x nanocrystal (NC) quantum dots (≈2 nm in radius) grown in a glass matrix by the melting-nucleation method, were studied by resonant Raman scattering (RRS) spectroscopy and theoretical modeling. The formation of nanocrystalline quantum dots (QDs) is evidenced by the observation of absorption peaks and theoretically expected resonance bands in the RRS excitation spectra. This system, a ternary alloy, offers the possibility to investigate the interplay between the effects of phonon localization by disorder and phonon confinement by the NC/matrix interface. Based on the concept of propagating optical phonons, which is accepted for two-mode pseudo-binary alloys in their bulk form, we extended the continuous lattice dynamics model, which has successfully been used for nearly spherical NCs of binary materials, to the present case. After determining the alloy composition for NCs (that was evaluated with only 2-3% uncertainty using the bulk longitudinal optical phonon wavenumbers) and the NC size (using atomic force microscopy and optical absorption data), the experimental RRS spectra were described rather well by this theory, including the line shape and polarization dependence of the scattering intensity. Even though the presence of a compressive strain in the NCs (introduced by the matrix) masks the expected downward shift owing to the phonons' spatial quantization, the asymmetric broadening of both Raman peaks is similar to that characteristic of NCs of pure binary materials. Although with some caution, we suggest that both CdSe-like and CdS-like optical phonon modes indeed are propagating within the NC size unless the alloy is considerably heterogeneous.
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