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 bubble structure when the chirped laser pulse propagates through the under-dense plasma (n e = 0.02n c). The evolution of the bubble in the case of the negatively chirped pulse with the chirped parameter of b = –0.08 at the times of: (a1) t = 300 fs, (a2) t = 500 fs, and (a3) t = 600 fs. The evolution of the bubble in the case of the positively chirped pulse with the chirped parameter of b = 0.08 at the times of: (b1) t = 300 fs, (b2) t = 500 fs, and (b3) t = 600 fs. The other laser parameters are the same as the un-chirped case.