Titlebook: Laser Physics at Relativistic Intensities; Andrew V. Borovsky,Andrew L. Galkin,Thierry August Book 2003 Springer-Verlag Berlin Heidelberg

Chipmunk

Relativistic and Charge-Displacement Self-Channeling of Intense Ultrashort Laser Pulses in Plasmas,r beam self-trapping occurs, and the laser pulse propagates into the plasma over dozens of Rayleigh ranges. An additional electromagnetic radiation confinement mechanism emerges due to electron cavitation, namely, the total expulsion of the electron fluid from a certain spatial area. Then, the laser

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繁忙

Andrew V. Borovsky,Andrew L. Galkin,Oleg B. Shiryaev,Thierry Augustees on c- rent and future trends of hardware and software developments. We observe a strong tendency to heterogeneous environments on the hardware level, while at the same time, applications bec978-3-642-44094-6978-3-642-03913-3

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Intense Laser Pulse Solitons in Plasmas,c plasma wavelength. A number of studies are dedicated to the interactions of large aperture intense laser pulses with cold underdense plasmas. In particular, energy transfer from the laser pulse to plasma waves is studied in [106] in the framework of model (6.33)–(6.34).

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,Experiments on Laser—Matter Interaction in the Relativistic Regime,e of interaction which is somewhat artificially defined by . = 0.85 × 10. × (λ[μm]) × (I.[W/cm.]). ≥ 1, where . is the normalized vector potential. Intensities as high as 10. W/cm. were recently reached [179]. Such intensities correspond to a = 8.5 and to electric fields about four decades higher than the electric field atomic unit.

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Fundamentals of Cold Plasma Electrodynamics,tic notation and in spatially three-dimensional form. We also consider the decomposition of plasma momentum into potential and curl parts. This decomposition simplifies the derivation of equations describing laser plasma interactions. The equations presented in this Chapter are used throughout this book.

Obvious

Instabilities of Circularly Polarized Plane Electromagnetic Waves in Plasmas,ample, is met by employing solutions of the Akhiezer—Polovin problem, is to use arbitrary amplitude solutions of the Maxwell and plasma dynamics equations as the ground state for the perturbative analysis.

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Propagation of Laser Radiation in Multiple-Stage Ionized Matter, plasma optical polarization, i.e., the deformation of electron shells resulting in the emergence of oscillating dipole moments of multiply charged ions. Naturally, both of these phenomena contribute to the medium’s dielectric response modification by propagating laser radiation.

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