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Titlebook: Ion acceleration and extreme light field generation based on ultra-short and ultra–intense lasers; Liangliang Ji Book 2014 Springer-Verlag

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Extreme Light Field Generation I: Quasi-Single-Cycle Relativistic Laser Pulse,se to interact with a solid-density foil before the latter is damaged by the prepulse of the laser. Very hard diamond-like foils of ultrasmall, say 4.5 nm, thickness comparing with the skin depth of the light are now available. All these offer a good condition for studying relativistic laser–foil interaction.
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Ion acceleration and extreme light field generation based on ultra-short and ultra–intense lasers978-3-642-54007-3Series ISSN 2190-5053 Series E-ISSN 2190-5061
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Springer Theseshttp://image.papertrans.cn/i/image/475189.jpg
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https://doi.org/10.1007/978-3-642-54007-3Circularly-polarized Laser Pulse; Extreme Light Field; Ion Acceleration; Laser Ion Accelaration; Laser P
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Ion Acceleration I: Efficient Heavy Ion Acceleration by ESA,udes higher than that of conventional methods. A number of novel mechanisms have been proposed for accelerating protons or heavier ions to high energies using the recently available high-intensity short-pulse lasers. With target-normal sheath acceleration, protons up to 58 MeV have been obtained with 3 × 10. W/cm. lasers [2].
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Extreme Light Field Generation II: Short-Wavelength Single-Cycle Ultra-Intense Laser Pulse,ressure and moves at an ultra-high velocity. With another counter-propagating CP pulse named the scattered pulse (SC pulse) impinging on this high-speed double layer, the SC pulse would be reflected and hence its frequency is strongly Doppler shifted.
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