Author/Authors :
Batani، نويسنده , , D. and Jafer، نويسنده , , R. and Redaelli، نويسنده , , R. and Dezulian، نويسنده , , R. and Lundh، نويسنده , , O. and Lindau، نويسنده , , F. and Persson، نويسنده , , A. and Osvay، نويسنده , , K. and Wahlstrِm، نويسنده , , C.-G. and Carroll، نويسنده , , D.C. and McKenna، نويسنده , , P. and Flacco، نويسنده , , A. and Malka، نويسنده , , V. and Veltcheva، نويسنده , , M.، نويسنده ,
Abstract :
Low-intensity laser prepulse (<1013 W/cm2, ns duration) are a major issue in experiments on laser-generation of protons, often limiting the performances of proton sources produced by high-intensity lasers (≈1019 W/cm2, ps or fs duration)
l effects are associated to the prepulse and are discussed in this contribution:i)
ction of thin foil targets by the shock generated by the laser prepulse
on of preplasma on target front side affecting laser absorption
ation of target rear side
displacement of thin foil targets affecting focusing condition
ticular, we show that under oblique high-intensity irradiation and for low prepulse intensities, the proton beam is directed away from the target normal. Deviation is towards the laser forward direction, with an angle that increases with the level and duration of the ASE pedestal. Also, for a given laser pulse, beam deviation increases with proton energy.
servations are discussed in terms of Target Normal Sheath Acceleration, in combination with a laser-controllable shock wave locally deforming the target surface.
Keywords :
Proton generation , Shock , laser absorption , Prepulse , High-pressure phase diagram