Self-focusing and the initial stages of plasma generation by short laser pulses

1978 ◽  
Vol 29 (2) ◽  
pp. 357-357
Author(s):  
J. E. Balmer ◽  
T. P. Donaldson ◽  
J. A. Zimmermann
1978 ◽  
Vol 24 (1) ◽  
pp. 109-112 ◽  
Author(s):  
J.E. Balmer ◽  
T.P. Donaldson ◽  
W. Seka ◽  
J.A. Zimmermann

2004 ◽  
Vol 11 (6) ◽  
pp. 3259-3263 ◽  
Author(s):  
Pallavi Jha ◽  
Navina Wadhwani ◽  
Ajay. K. Upadhyaya ◽  
Gaurav Raj

2007 ◽  
Vol 25 (2) ◽  
pp. 267-275 ◽  
Author(s):  
A.YA. Faenov ◽  
A.I. Magunov ◽  
T.A. Pikuz ◽  
I. YU. Skobelev ◽  
S.V. Gasilov ◽  
...  

X-ray spectra of plasma produced by the interaction of Ti:Sa laser pulses (duration from 60 fs to 1 ps, and energy from 15 mJ to 128 mJ) with foil and solid Teflon and AL targets are investigated. It is shown experimentally and theoretically that the use of low contrast (10−2 – 10−4) short laser pulses, essentially promotes the conditions for generation of fast multi-charged ions. This effect is caused by self-focusing of the main laser pulse in a preplasma produced by intense laser prepulses. Modeling of the observed spectral line shape gives evidence of a considerable (about 3%) amount of multi-charged He-like F ions with energy E ∼ 1 MeV at rather low values of laser intensity IL ≈ 6 × 1016 W cm−2.


2007 ◽  
Vol 21 (03n04) ◽  
pp. 615-625 ◽  
Author(s):  
S. EISENMANN ◽  
Y. KATZIR ◽  
A. ZIGLER ◽  
G. FIBICH ◽  
E. LOUZON ◽  
...  

A study of the propagation of intense short laser pulses in air and the interaction of these pulses with distant targets is described. It is shown that the beam filamentation pattern can be controlled by introducing beam astigmatism. In addition, it is demonstrated that the collapse distance of intense femtosecond laser beams scales as P -1/2 for input powers that are moderately above the critical power for self focusing, and that at higher powers the collapse distance scales as P -1. Related to the interaction of intense short pulses with distant targets, it is measured that the threshold fluence for optical damage in wide gap materials is lower by up to 20% for negatively chirped pulses than for positively chirped, at pulse durations ranging from 60 fs to 1 ps.


1997 ◽  
Vol 33 (11) ◽  
pp. 1879-1914 ◽  
Author(s):  
E. Esarey ◽  
P. Sprangle ◽  
J. Krall ◽  
A. Ting

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