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Aldo Artímez Peña

Publications and source records attributed to Aldo Artímez Peña.

3 recordsLinked to original sources

Ultrafast X-ray interaction with photovoltaic materials: Thermal and nonthermal responses

Cadmium telluride (CdTe), lead sulfide (PbS), and indium tin oxide (ITO) play crucial roles in various electronic applications where laser treatment enables precise modification of their distinctive electronic characteristics. This study utilizes the XTANT-3 hybrid/multiscale model to investigate the microscopic response of these materials to ultrafast X-ray irradiation. The model simultaneously traces intertwined processes of non-equilibrium dynamics of both electrons and atoms, nonadiabatic coupling, nonthermal melting, and bond breaking due to electronic excitation. Among the materials studied, CdTe exhibits the highest radiation resistance, similar to CdS. At the respective threshold doses, the melting is primarily thermal, driven by electron-phonon coupling, which is accompanied by the band gap closure. Additionally, all materials exhibit nonthermal melting at higher doses. When accounting for energy dissipation pathways and material recrystallization processes, damage thresholds increase substantially. In CdTe and PbS, below 1.5 eV/atom, the band gap returns to its original value upon recrystallization. As the dose increases, the resulting cooled material becomes increasingly amorphous, progressively reducing the band gap until a stable configuration is reached. Notably, in a narrow window of deposited doses, ITO exhibits transient superionic behavior, with the liquid oxygen but solid In and Sn sublattices. At 0.6 eV/atom in CdTe and 0.4 eV/atom in PbS and ITO, material ablation from the surface occurs. These findings indicate that femtosecond laser technology offers promising opportunities for precise band gap engineering in various photovoltaic semiconductor devices.

cond-mat.mtrl-sci↗

Creating mixed-phase states in cadmium sulfide by swift heavy ion irradiation

CdS has broad applications in solar cells and radiation detectors. We study its response to irradiation with swift heavy ions and determine its damage thresholds. We apply a model combining the Monte Carlo code TREKIS-3 to simulate the kinetics of the electronic system and the molecular dynamics code LAMMPS to track the atomic reaction to the energy transfer. It is found that ion tracks in CdS differ between its zincblende and wurtzite phases in morphology and damage thresholds. The anisotropic wurtzite phase displays directional damage formation with transient hexagonal track shapes along the (001) plane. In contrast, zincblende CdS exhibits a more cylindrical damage distribution. High pressures near the ion path drive mass transport away from the melted region, forming cavities within the track core in the wurtzite phase. Although significant recrystallization is observed during post-irradiation relaxation, it does not fully restore the original phase: final tracks consist of the amorphous cores due to the low densities in this region and defect-containing crystalline halos. These findings suggest that ion irradiation could be used to create mixed-phase CdS-based materials.

cond-mat.mtrl-sci↗

Ultrafast X-ray induced damage and nonthermal melting in cadmium sulfide

Cadmium sulfide is a valuable material for solar cells, photovoltaic, and radiation detectors. It is thus important to evaluate the material damage mechanisms and damage threshold in response to irradiation. Here, we simulate the ultrafast XUV/X-ray irradiation of CdS with the combined model, XTANT-3. It accounts for nonequilibrium electronic and atomic dynamics, nonadiabatic coupling between the two systems, nonthermal melting and bond breaking due to electronic excitation. We find that the two phases of CdS, zinc blende and wurtzite, demonstrate very close damage threshold dose of ~0.4-0.5 eV/atom. The damage is mainly thermal, whereas with increase of the dose, nonthermal effects begin to dominate leading to nonthermal melting. The transient disordered state is a high-density liquid, which may be semiconducting or metallic depending on the dose. Later recrystallization may recover the material back to the crystalline phase, or at high doses create an amorphous phase with variable bandgap. The revealed effects may potentially allow for controllable tuning of the band gap via laser irradiation of CdS.

cond-mat.mtrl-sci↗