Table-top laser–plasma ion accelerators have many exciting applications, many of which require ion beams with simultaneous narrow energy spread and high conversion efficiency. However, achieving these requirements has been elusive. Here we report the experimental demonstration of laser-driven ion beams with narrow energy spread and energies up to 18 MeV per nucleon and ∼5% conversion efficiency (that is 4 J out of 80-J laser). Using computer simulations we identify a self-organizing scheme that reduces the ion energy spread after the laser exits the plasma through persisting self-generated plasma electric (∼1012 V m−1) and magnetic (∼104 T) fields. These results contribute to the development of next generation compact accelerators suitable for many applications such as isochoric heating for ion-fast ignition and producing warm dense matter for basic science.
Traveling convection vortices TCV are studied using a theoretical ideal MHD model for the equilibrium and perturbed plasma. In this rst approach, we do not consider the viscosity and the ow of the plasma column in the equilibrium. The linearized equations are solved using normal mode analysis. The solutions show a n m = 1 kink instability which is in good agreement with the experimental data. It is calculated numerically a growth rate of 28 minutes to be compared with experimental data, indicating a quite good result with our model. Clearly, the results indicate the behaviour of the TCV as a kind of kink instability as supported by the agreement b e t ween theoretical and experimental values for the growth rate. Also the lamentation currents calculated through the theoretical model agree quite well with the experimental observations by satellites.
We have derived the viscous MHD equilibrium and perturbed equations
for current carrying cylindrical plasmas. We have considered
compressible plasmas and, when the viscosity is introduced in the
equation of motion it leads to a linearized vector second order
perturbed equation for the fluid displacement, showing the appearance
of non Hermitian operators. The Lagrangian representation is used to
investigate the stability and we used the normal mode analysis to
study the linearized equation. We applied our model for the problem of
the coronal loop heating and solved the eigenmode equation, which is
nonlinear in the eigenvalue, using a numerical code based on the
software “Mathematica”, with appropriate
boundary conditions. We have confirmed that viscosity is relevant as
the dominant mechanism for the coronal loop heating in our
self-consistent calculation as indicated by previous non
self-consistent work of De Azevedo et al (1991 Solar Phys.
136 295). In the limit of zero viscosity, we obtain the
discrete and the continuous spectra and some unstable
points.
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