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Ativistic. The many 2-D complex interaction. laser PIC and light (>50%) absorbed by of very absorption dence the that there is efficient arise into absorption Most of the energy is primarily in the energetic electrons and ions. Spheres," of The generated by The dorni- temperature this mechanism can due laser to the large impinges light on the pressure target, of the laser. the central of be As the ripple past enhanced the critical because surface. the laser The electric absorption field is further can now Falcone, "Multiterawatt, (_.

Kirala, K. B. Mitchell, D. Van 1-1ulsteyn, and A. 6-urn Laser-Illuminated in this resulting mechanism electrons insight that surface, is J x B heating hot processes the plasma. at the critical generation nant nonlinear We find extremely rel- [am2/cm 2 is provides valuable code I...... in 2(1. Relativistic K. (;. stabrtulk, E. ]. Valeo, and W. I.. Kruer, "Two-dimensional SJmulaliiuls (ii Resollailct' Absorption," I>lnls. I-'luids, 18, I1_1 (ItU_,). 21. W. I.. tvmnĀ¢ifls c,nPhtsmal_Inl,_ics and Conlnqh'd lusion, IX, [_3(I_851.

Kruer A. B. Langdon Introduction One of the most exciting frontiers in physics today is the interaction of ultrashort, ultra-intense (I > 1017 W/cre 2) laser pulses with dense plasmas, Short pulse lasers open up new avenues of research which enable experimenters to access a strongly nonlinear regime of laser-plasma interactions. This regime is characterized by relativistic effects and large light pressures. For many years, there was only incremental progress towards achieving peak powers and focused irradiances for pulses less than or equal to a picosecond (10 q2 s).

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Aircraft Manual - Hurricane I - Merlin II Engine [Air Pub 1564A Vol I] (Air Ministry


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