To analyze the mechanism of damage threshold enhancement after laser conditioning, the fluorescent and stimulated Raman scattering properties of unconditioned and laser-conditioned KD2PO4 crystals are compared in detail. It is revealed that the intensity of fluorescence decreases significantly, especially fluorescence <400 nm, after nanosecond laser conditioning, and the change of the stimulated Raman scattering peak at 921 cm − 1 is very weak. Moreover, the intensity of fluorescence further decreases after subnanosecond laser conditioning. A sharp decrease in the fluorescence intensity <400 nm reflects a change in energy levels of the electron defects in a crystal. The Raman scattering proves very weak change of the PO4 vibrational modes. Furthermore, a laser-conditioning mechanism is discussed in combination with electronic transition and thermal processes.
Subwavelength periodic nanostructures on metal, dielectric or metal-dielectric-metal coating were fabricated by femtosecond laser. Circular apertures with diameter of ~0.6μm and a lattice period of 1.0 and 2.0 um were fabricated by single laser pulse irradiation. Surface geometries of nanostructure unit on the three kinds of coatings were compared using the scanning electron microscope and atomic force microscope. Moreover, the nanostructure units fabricated by front-side ablation technique and back-side ablation technique were compared. The minimum diameter of the circular aperture fabricated both by front-side ablation technique and back-side ablation technique could reach approximate 300 nm. By studying mechanisms of femtosecond laser interaction with metal films and dielectric films, it’s found that metal layers dominate femtosecond laser interaction with metal-dielectric-metal sandwich type coatings. It’s also found that the edges of apertures fabricated by back-side ablation technique in metal coatings and metal-dielectric-metal coatings are more regular and round than those fabricated by front-side ablation technique. Femtosecond laser fabrication therefore provides possibilities for maskless and speedy fabrication of fishnet structures which exhibit negative refractive index at optical frequencies.
In order to analyze the mechanism of damage threshold enhancement after laser conditioning, the stimulated Raman scattering and fluorescent properties of un-conditioned and laser conditioned of DKDP crystals were compared in detail. It revealed that the intensity of Raman scattering peak 921cm-1 were slightly lowered, and the intensity of fluorescence was much decreased, especially the fluorescence below 400nm, after nanosecond laser conditioning. Moreover, the intensity of fluorescence could be further decreased after sub-nanosecond laser conditioning. The slightly variation of Raman scattering proved the modification of the PO4 vibrational modes. The sharply decrease of fluorescence intensity below 400 nm reflected the density reduction of electron defects in these crystals. On the basis of the above analysis, laser conditioning mechanism in DKDP crystals was discussed.
We measured the absorption of type I doubler KDP crystal at different laser wavelengths (1064, 532 and 355 nm) by
using laser induced deflection (LID) technique. We also performed the absorption measurements in the cases where
beam polarization was parallel to the principal plane (Pd//Pp) and perpendicular to it (Pd⊥Pp). To account for the
experiment results, a model based on crystal dichroism was developed to calculate the absorption coefficients for O
ray (αo) and E ray (αe) at different laser wavelengths. It is found that the dichroism is manifested especially clearly
at 1064nm, but not clearly at 355nm/532nm. It implies that the absorption at 1064nm is mainly due to lattice
absorption, whereas defects absorption is responsible for the absorption at 355nm/532nm.
Transient transmission and scattering changes was observed to study the dynamics during the laser-induced bulk damage
in fused silica at the wavelength of 532 and 355 nm. Within the nanosecond high power laser irradiation, the
transmittance decreased dramatically, indicating an intense absorption. With fluence increasing, the time required to
form the intense absorption was shortened, and at similar fluence, this time interval at the wavelength of 355 nm is
shorter than that at 532 nm. At times, the intense absorption did not cause the macroscopic damage because no variation
in scattering was observed. While the macroscopic damage occurred, the scattering kept on increasing until the end of
pulse.
Combining high power laser irradiation and emission spectra measurement system, the photoluminescence properties of KDP crystal under high power laser irradiation were studied. Photoluminescence measurement was performed using 532 nm and 355 nm laser excitation at relatively high laser fluence but still under the laser induced damage threshold. Four emission peaks, centered at 559 nm, 586 nm, 609 nm and 621 nm, were observed while irradiated by high power laser at 532 nm. Five emission peaks, centered at 358 nm, 365 nm, 377 nm, 385 nm and 390 nm were observed under high power laser irradiation at 355 nm. Based on the analysis of wave number transformation, these peaks were attributed to the Raman scattering.
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