Two Stages of Impact Fracture of Polycrystalline ZnS and ZnSe Compounds

• Published in: Physics of the solid state Vol. 60; no. 4; pp. 764 - 768
• Main Authors: Shcherbakov, I. P., Dunaev, A. A., Chmel’, A. E.
• Format: Journal Article
• Language: English
• Published: Moscow Pleiades Publishing 01.04.2018; Springer; Springer Nature B.V
• Subjects: AMPLITUDES; CERAMICS; Chemical bonds; CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; COVALENCE; Crack initiation; Crack propagation; CRACKS; Crystal structure; DEFORMATION; Deformation mechanisms; DIFFUSION BARRIERS; Disintegration; DISLOCATIONS; DISTRIBUTION; Ductile fracture; ELECTRONIC STRUCTURE; EXCITATION; Formability; Fracture mechanics; FRACTURES; Grains; Heat treatment; HEAT TREATMENTS; Impact loads; LUMINESCENCE; Mechanical Properties; Mechanoluminescence; Physics; Physics and Astronomy; Physics of Strength; Plastic deformation; PLASTICITY; POLYCRYSTALS; PULSES; Reconfiguration; Solid State Physics; SOLIDS; SYNTHESIS; Tips; ZINC SELENIDES; ZINC SULFIDES
• ISSN: 1063-7834; 1090-6460
• DOI: 10.1134/S1063783418040303

Mechanoluminescence (ML) in ductile solids is caused by the motion of charged dislocations in the deformable material. Interatomic bond ruptures followed by electronic structure reconfiguration are the main source of ML in brittle bodies. We studied ML in ceramics composed of mixed ionic/covalent ZnS and ZnSe compounds, which are generated during impact loading higher than the limit deformation. Depending on synthesis method and thermal treatment, the resulting ceramics had different size and geometry of grains and intergrain boundary structure, which presumably may have a significant effect on the dislocation glide. In both materials, the time sweeps of ML pulses have two well-resolved peaks. The position of the peaks along the time axis is substantially dependent on the size of ceramic-forming grains and, to a smaller extent, on the barrier properties of intergrain boundaries. The first peak is associated with plastic deformation preceding disintegration of the crystal structure. The second peak emerges upon crack nucleation as interatomic bonds are ruptured and the material is undergoing local deformation in tips of propagating cracks. The distributions of ML pulse amplitudes (the dependences between the number of pulses and their amplitude) calculated for both peaks individually follow the power law, which demonstrates that the electronic processes having different excitation mechanisms (dislocation motion vs bond rupture) are correlated.