Speaker
Prof.
Javier Honrubia
(Polytechnic University of Madrid)
Description
The magnetized liner inertial fusion (MagLIF) scheme has been proposed for cylindrical
implosions of magnetized fuels with lower implosion velocities and convergence ratios, resulting
in an appealing scheme for inertial fusion [1]. Recently, a laser-driven version of MagLIF has
been explored at the Omega facility [2] to study the magnetized implosion physics of MagLIF
targets scaled down by a factor of 10 in linear dimensions. The advantages of using the Omega
laser system are the good illumination symmetry, the higher repetition rate and better diagnostic
access. B-field amplifications through flux compression of about 550 have been measured so far
in cylindrical and spherical implosions on Omega [3].
Here, we analyze the implosion of a magnetized cylindrical target similar to that used in
Omega MagLIF by means of 2-D MHD simulations with the FLASH code [4]. The target is a
plastic (CH) hollow cylinder of 2 mm long, 300μm outer radius and 30μm thick filled with a
CH foam with the density as a parameter. It is driven by 40 laser beams with a total energy of
15.2 kJ in 1.5 ns. The Omega MagLIF illumination scheme was assumed [2]. Simulations show
amplification of the B-field up to 10 kT and higher and magnetic flux conservation around 70%
for a foam density of 20 mg/cm3. As such a B-field is high enough to guide fast electrons and
even protons, we have conducted 3D hybrid simulations of fast electron and proton transport and
energy deposition in the imploded cylindrical target [5,6]. Specifically, we have analyzed if the
intense B-fields achieved at target stagnation are able to guide highly diverging laser-driven fast
electrons and even the less diverging TNSA protons. The first experimental evidence of fast
electron beams guiding by external magnetostatic fields was described in [7]. Here, the B-fields
are increased by roughly one order of magnitude due to magnetic flux conservation in cylindrical
target implosions. Our study will be useful to determine the conditions of the high energy density
matter generated by perfectly collimated electron and ion beams. It may be also relevant for
hydrodynamics of magnetized cylindrical targets.
References
[1] S.A. Slutz et al., Phys. Plasmas 17, 056303 (2010).
[2] J.R. Davies et al., Phys. Plasmas 24, 062701 (2017).
[3] M. Hohenberger et al., Phys. Plasmas 19, 056306 (2012).
[4] B. Fryxell et al., Astrophysical Journal 131, 273 (2000).
[5] J.J. Honrubia and J. Meyer-ter-Vehn, Plasma Phys. and Control. Fusion 51, 014008 (2009).
[6] J.J. Honrubia and M. Murakami, Phys. Plasmas 22, 012703 (2015).
[7] M. Bailly-Grandvaux et al., Nature Comm. 9, 102 (2018).
Primary author
Prof.
Javier Honrubia
(Polytechnic University of Madrid)