(b) HRTEM image of a

single CdS NP. (c) XRD patterns obtained from the laser-irradiated zone for different doping concentrations selleck chemicals llc and (d) the particle size evolution deduced from the width of the reflex (110). (a, b, and c) adapted from [37]. Lead sulfide nanoparticles Lead acetate and thiourea in aqueous solution have been used to impregnate a xerogel. Then, irradiation of this sample with fs pulses at 800 nm led to the rapid formation of PbS NP [40], which could be recognized not only by the brown coloration in Figure 8a but also by various characterization techniques (HRTEM, EDX analysis, electron diffraction, photoluminescence). Since the sample is initially transparent at 800 nm, the photogrowth Panobinostat molecular weight process probably involves multiphoton absorption, but as soon as the first NP appear in the beam waist volume, one-photon absorption can occur

and even becomes predominant. The TEM images (inset of Figure 8a) give particle sizes comprised between 5 and 12 nm for a given laser power of 40 mW, which is corroborated by XRD experiments. The evolution of the NP size with the laser power (Figure 8c, blue curve) shows that the crystal growth is not limited by the porosity, as it is always the case if the growth process is very efficient. The reason why photogrowth of PbS is found more efficient than in the case of CdS under fs irradiation at low repetition rate lies in the thermal origin of this process. In effect, the thermal energy liberated by one-photon absorption is fully sufficient for the precursor breakdown and for atom diffusion, whereas multiphoton absorption only acts as a starter. Figure 8 Local growth of PbS NP in a xerogel impregnated with PbS precursors. The doping solution had a GW4869 mw concentration of 0.37 M in lead acetate. (a) Photograph of a sample fs irradiated at 10 mW and TEM image of NPs obtained after fs irradiation at 40 mW. (b) TEM and HRTEM images after CW irradiation at 140 mW. (c) Average particle size against Ketotifen the laser power in both regimes. The power threshold has been measured for the CW laser. Dotted lines are extrapolations. (a and b) adapted from [40] and [41], respectively. An even darker and stronger

coloration could be obtained by using a visible CW laser [41]. In this latter case, the high concentration of NP observed in the TEM image of Figure 8b is an indication of the process efficiency, as well as the particle size that overpasses the mean pore size. For the highest doping concentration (precursor solution 0.37 M), the mean NP diameter, estimated using PbS peaks in XRD pattern and Debye-Scherrer equation, seems to reach a maximum around 11 nm, namely about twice the pore size diameter. However, the particle size can be tuned down to 2 or 3 nm by decreasing the doping concentration. One unfortunate feature of PbS NP is their affinity with oxygen to form PbO and PbSO4 compounds, leading to a poor stability of their optical properties [42].