TY - JOUR KW - Energy KW - Target KW - Gas KW - Measurements KW - Acoustics KW - Measurement KW - Transportation KW - Surface KW - Power KW - Copper KW - Experimental KW - Material KW - Ablation KW - Laser KW - Laser ablation KW - Laser ablation KW - Breakdown KW - Intensities KW - Intensity KW - Time KW - Beam KW - Plasma KW - Cu KW - Dependence KW - Lasers KW - Ratio KW - Excimer KW - Nd:yag KW - Ga KW - Ionization KW - Picosecond KW - Nanosecond KW - Pulsed laser KW - Pulsed laser KW - Targets KW - Laser material interaction KW - Energies KW - Nd:yag laser KW - Laser beam KW - M KW - Results KW - Pressure KW - Shock KW - Ar KW - He KW - Plasma shielding KW - Air KW - Pulsed laser ablation (PLA) KW - Media KW - Shock waves KW - Waves KW - Stress KW - Stresses KW - Al KW - Pressure waves AU - Mark A Shannon AU - Richard E Russo AB -
High-power pulsed laser-material interactions are monitored with acoustic measurements of mechanical stress power. At laser intensities above 108 W/cm2, an explosive, plasma forming interaction occurs between the laser beam and the solid target, ablating material away. Stresses in the target caused by the laser ablation can be very large, which for short pulsed laser ablation can make mechanical transport of energy significant. Experimental work is conducted to study the affect of laser intensity on stress power in the target and that carried by pressure waves in the surrounding gas medium. 30 ns excimer and 35 ps Nd:YAG lasers are used to ablate Al and Cu targets, and the resulting stresses are recorded by different types of transducers. The nanosecond results show that gas ionization breakdown can be detected through the stress power, and that the power measured follows a near quadratic dependence on the incident energy. Variations in the ratio of the shock power in air to the stress power in the target shows that plasma shielding of the laser beam can be monitored using the mechanical stress power. Differences in plasma shielding during pico-second ablation of copper in Ar versus He are shown using stress power monitoring.
AD -LAWRENCE BERKELEY LAB,BERKELEY,CA
BT - Applied Surface Science DA - 04/1996 LA - eng LB - Laser N1 -Proceedings of Symposium F: Third International Symposium on Laser Ablation of the 1995 E-MRS Spring Conference
N2 -High-power pulsed laser-material interactions are monitored with acoustic measurements of mechanical stress power. At laser intensities above 108 W/cm2, an explosive, plasma forming interaction occurs between the laser beam and the solid target, ablating material away. Stresses in the target caused by the laser ablation can be very large, which for short pulsed laser ablation can make mechanical transport of energy significant. Experimental work is conducted to study the affect of laser intensity on stress power in the target and that carried by pressure waves in the surrounding gas medium. 30 ns excimer and 35 ps Nd:YAG lasers are used to ablate Al and Cu targets, and the resulting stresses are recorded by different types of transducers. The nanosecond results show that gas ionization breakdown can be detected through the stress power, and that the power measured follows a near quadratic dependence on the incident energy. Variations in the ratio of the shock power in air to the stress power in the target shows that plasma shielding of the laser beam can be monitored using the mechanical stress power. Differences in plasma shielding during pico-second ablation of copper in Ar versus He are shown using stress power monitoring.
PY - 1996 SP - 149 EP - 153 T2 - Applied Surface Science TI - Monitoring stress power during high-power pulsed laser-material interactions VL - 96-98 ER -