Titlebook: Laser Interaction and Related Plasma Phenomena; Proceedings of the F Helmut J. Schwarz (Professor of Physics),Heinrich Conference proceedi

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书目名称Laser Interaction and Related Plasma Phenomena影响因子(影响力)




书目名称Laser Interaction and Related Plasma Phenomena影响因子(影响力)学科排名




书目名称Laser Interaction and Related Plasma Phenomena网络公开度




书目名称Laser Interaction and Related Plasma Phenomena网络公开度学科排名




书目名称Laser Interaction and Related Plasma Phenomena被引频次




书目名称Laser Interaction and Related Plasma Phenomena被引频次学科排名




书目名称Laser Interaction and Related Plasma Phenomena年度引用




书目名称Laser Interaction and Related Plasma Phenomena年度引用学科排名




书目名称Laser Interaction and Related Plasma Phenomena读者反馈




书目名称Laser Interaction and Related Plasma Phenomena读者反馈学科排名

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Nutrient

employor

Scattering of Laser Radiationssible studies of non-linear scattering effects which could not have been undertaken readily, if at all, with conventional sources. In the present paper, an attempt will be made to survey some recent scattering experiments and theory. No attempt at completeness is made.

Spartan

Shock Wave Process and Numerical Calculationsoncluded that a non-transparent layer is formed on the surface of the solid in the very early stages of the irradiation process. Most of the laser energy is absorbed in this layer, and a hot plasma is formed and expands with high velocities. The reaction forces produce a shock wave in the solid.

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效果

Numerical Calculations of Plasma Heating by Means of Subnanosecond Laser Pulsesion of state. The calculation technique is applied to various experimental situations, including the recent lithium deuteride thick target neutron detection experiments, and the results are presented.

BROTH

骚动

Thin Films of Metals and Inorganic Compounds Vacuum Deposited by High Energy Laser kinetic energy equivalent to at least the condensation heat; it is of the order of 5–10 eV or more. By changing the deposition rate with conventional thermal evaporation sources the velocity is not affected so much, since it is only a function of the square root of the temperature, whereas a much g

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