The dc conductivity (σ) along the polar b-axis of ammonium zinc chloride (AZC) crystals in its four hightemperature phases has been measured as a function of temperature. Doping with Mn 2+ in different concentrations changed strongly both values of σ at all temperatures and the dependence of ln σ dc
Laser-induced optical effects in triglycine–zinc chloride single crystals
✍ Scribed by A. Wojciechowski; I.V. Kityk; G. Lakshminarayana; I. Fuks-Janczarek; J. Berdowski; E. Berdowska; Z. Tylczyński
- Publisher
- Elsevier Science
- Year
- 2010
- Tongue
- English
- Weight
- 456 KB
- Volume
- 405
- Category
- Article
- ISSN
- 0921-4526
No coin nor oath required. For personal study only.
✦ Synopsis
The influence of irradiation by a cw 532 nm laser on the behavior of the absorption and optical second harmonic generation of triglicyne-zinc chloride crystal has been studied. Additional absorption bands correlate well with the time of the cw laser exposure. These lines occur at 260 nm, 305 nm, and, with small intensity, at 355 nm. The remaining part of the spectra shows substantially less changes. According to the performed quantum chemical simulations, one may expect that the observed dependences and the stability of the observed photoinduced changes are caused by formation of polarized electron-phonon states and the principal role should belong here to the electron-phonon anharmonicities, which cause the effects described by the non-polar third rank polar tensor like optical second harmonic generation. The increasing optical SHG signal shows a clear correlation with the behavior of the green laser-532 nm. It is important principal that for the blue laser-405 nm, the SHG effect is substantially less. This may reflect that the additional absorption maxima may be responsible for the non-linear optical effects. The effect demonstrates a slow time decay.
📜 SIMILAR VOLUMES
The epitaxially induced strains in thin Cu,O films on the (loo), (11 l), ( 110) and (311) faces of copper single crystals were characterized in terms of changes produced in the optical properties of the films. Oxide on the (110) and (311) exhibited optical anisotropy while that on the (100) and (111