Speaker: Juan C. Fernandez

Physics Division, Los Alamos National Laboratory

  

 

Intense laser-driven ion beams:  the science of how they're made and their applications



Laser-plasma interactions in the novel regime of relativistically-induced transparency have been harnessed to generate efficiently intense ion beams with average energies exceeding 10 MeV/nucleon (> 100 MeV for protons) at 'table-top' scales. High-intensity is possible because these beams are  neutralized and therefore immune to the space-charge and current limits of conventional beams. We have discovered and utilized a self-organizing scheme that exploits persisting self-generated plasma electric (~ 0.1 TV/m) and magnetic (~104 Tesla) fields to reduce the ion-energy (Ei) spread after the laser exits the plasma [1], thus separating acceleration from spread reduction. In this way we routinely generate aluminum and carbon beams with narrow spectral peaks at Ei up to 310 MeV and 220 MeV, respectively, with high efficiency (~5%), which at present represents the worldwide state of the art. The experimental demonstration has been done at the LANL Trident laser, irradiating planar foils up to 250 nm thick. Our progress is enabled by massive high-fidelity computer simulations of the experiments. This work advances next-generation compact accelerators suitable for new applications. E.g., a Ei ~400 MeV carbon beam with ~10% energy spread is suitable for fast ignition (FI) of compressed DT [2]. The observed scaling suggests a FI-class ion beam is feasible with existing target fabrication and PW-laser technologies, using a sub-ps laser pulse with ~  2.5 x1021 W/cm2. More near term, these beams have been used on Trident to generate warm-dense matter at solid-densities [3]. They also drive an intense neutron-beam source [4] with great promise for important applications such as bulk thermometry of dynamic materials, active interrogation of shielded nuclear materials, neutron imaging and weapons physics.  In addition, these beams have been used to drive an intense point-like, directed source of ~ 1 MeV gamma-rays, which has been used for imaging thick objects.

[1] S. Palaniyappan, C. Huang, et al., Nature Comm.  6, 10170 (2015)

[2] J. C. Fernandez, et al., Nucl. Fus.  54, 054006 (2014)

[3] W. Bang, et al., Sci. Rep. 5, 14318 (2015)

[4] M. Roth, et al., PRL 110, 044802 (2013)