Beam collimation and transport of quasineutral laser-accelerated protons by a solenoid field

ソレノイド磁場による、レーザー駆動陽子線の収束伝送

Harres, K.*; Alber, I.*; Tauschwitz, A.*; Bagnoud, V.*; 大道 博行; Gnther, M.*; Nrnberg, F.*; Otten, A.*; Schollmeier, M.*; Schtrumpf, J.*; 反保 元伸; Roth, M.*

Harres, K.*; Alber, I.*; Tauschwitz, A.*; Bagnoud, V.*; Daido, Hiroyuki; Gnther, M.*; Nrnberg, F.*; Otten, A.*; Schollmeier, M.*; Schtrumpf, J.*; Tampo, Motonobu; Roth, M.*

This article reports about controlling laser-accelerated proton beams with respect to beam divergence and energy. The particles are captured by a pulsed high field solenoid with a magnetic field strength of 8.6 T directly behind a flat target foil that is irradiated by a high intensity laser pulse. Proton beams with energies around 2.3 MeV and particle numbers of 10 could be collimated and transported over a distance of more than 300 mm. In contrast to the protons the comoving electrons are strongly deflected by the solenoid field. They propagate at a submillimeter gyroradius around the solenoid's axis which could be experimentally verified. The originated high flux electron beam produces a high space charge resulting in a stronger focusing of the proton beam than expected by tracking results. Leadoff particle-in-cell simulations show qualitatively that this effect is caused by space charge attraction due to the comoving electrons. The collimation and transport of laser-accelerated protons is the first step to provide these unique beams for further applications such as postacceleration by conventional accelerator structures.