Pulse chirping effect on controlling the transverse cavity oscillations in nonlinear bubble regime
Vosoughian H1, 3, 4, †, Riazi Z2, Afarideh H3, Sarri G4
       

(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.