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Titlebook: High-Field Science; Toshiki Tajima,Kunioki Mima,Hector Baldis Book 2000 Springer Science+Business Media New York 2000 Absorption.X-ray.ast

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41#
發(fā)表于 2025-3-28 18:02:26 | 只看該作者
42#
發(fā)表于 2025-3-28 18:48:48 | 只看該作者
43#
發(fā)表于 2025-3-29 01:11:58 | 只看該作者
E. Esarey,C. B. Schroeder,W. P. Leemanslgorithm involves the construction of a Hamiltonian that describes the behavior of the quantum system. This Hamiltonian is expressed as a linear interpolation of an initial Hamiltonian whose ground state is easy to compute, and a final Hamiltonian whose ground state corresponds to the solution of a
44#
發(fā)表于 2025-3-29 03:16:51 | 只看該作者
45#
發(fā)表于 2025-3-29 11:01:33 | 只看該作者
46#
發(fā)表于 2025-3-29 12:02:20 | 只看該作者
Equation of State Measurements at Extreme Pressures Using Laser-Driven Shockspose has been limited. Direct irradiation of a solid by even a tabletop laser focused to a small spot can produce a multi-Mbar shock. Although this has been known for several decades, during that time most laser-driven shock experiments have been demonstrations of high velocity shock waves, not the
47#
發(fā)表于 2025-3-29 16:51:24 | 只看該作者
Dusty Plasmas and Coulomb Crystalsmb crystals) when its kinetic energy becomes sufficiently small compared with its potential energy. Employing Yukawa potential to model the interparticle potential between dust particles, we have performed molecular dynamics (MD) simulation to obtain the phase diagram of such charged dust systems.
48#
發(fā)表于 2025-3-29 23:32:08 | 只看該作者
49#
發(fā)表于 2025-3-30 00:42:57 | 只看該作者
Second-Harmonic Generation and Non-Resonant Absorption in Sub-Picosecond Laser-Solid Interactionsce near 20°, the specular second harmonic is blue shifted when the laser intensity exceeds 1 × 10. W/cm.. This effect is also observed in PIC simulations of the experiment. Several absorption mechanisms are examined for their consistency with the data.
50#
發(fā)表于 2025-3-30 05:25:02 | 只看該作者
Strong Coupling between Clusters and Radiationf laser with clustered matter over conventional unclustered one arises first from the uncancelled transverse polarization induced on clusters by the laser and further in a nonlinear regime from the nonharmonic orbits of electrons that are detached from their original cluster. In the nonlinear regime
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