Physics of Plasmas · 2008 · 13 citations · 20 references
Natural SciencesPhysicsOpticsPlasma PhysicsRadiation PhysicsHigh-temperature PlasmasLaser PhysicsLaser-plasma InteractionsNonlinear Plasma DynamicsPlasma OscillationsPlasma SimulationHarmonic GenerationHarmonic Generation In PlasmasHigh-harmonic GenerationMetallic Thin FilmsNonlinear Plasma OscillationsNonlinear Plasma WavesThird-harmonic GenerationWave Number
An analytical model is developed for third harmonic generation (THG) efficiency from a high-density inhomogeneous plasma produced by laser irradiation of a thin metallic film. The laser suffers strong reflection from the critical layer. The superposition of forward and backward waves creates a quasistatic density ripple of wave number 2k and a second harmonic density ripple at 2ω, 4k, where ω and k are the frequency and wave number of the laser. The density ripple couples with the oscillatory electron velocity at ω, k to produce a nonlinear current at 3ω, 5k driving a resonant third harmonic radiation in the region where 5k=k3 and k3 is the wave number at 3ω frequency. As the density scale length of the plasma is increased, the efficiency of THG increases. The same behavior is reproduced in two particle in cell simulation by launching a laser in a rippled density underdense plasma of phase-matched density and a ripple period of half-laser wavelength.
20
Not-so-resonant, resonant absorption
F. Brunel · Physical Review Letters · 1987 · 1K citations
Natural Sciences, Physics, Optics +14
Generation of Coherent Soft X Rays at 2.7 nm Using High Harmonics
Zenghu Chang, Andy Rundquist, Haiwen Wang et al. · Physical Review Letters · 1997 · 742 citations
Relativistic laser plasma interactions
D. Umstadter · Journal of Physics D Applied Physics · 2003 · 327 citations · Full text