Pulse chirping effect on controlling the transverse cavity oscillations in nonlinear bubble regime |
(color online) The evolution of THE bubble structure when the un-chirped laser pulse propagates through the under-dense plasma (n e = 0.02n c) at the times of: (a) t = 300 fs, (b) t = 500 fs, and (c) t = 600 fs. The laser pulse with the normalized amplitude of a 0 = 10, the longitudinal size of σ x = 10 µm, and the spot size of σ y = 8 µm enters the simulation box from the left boundary. |
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