scholarly journals Status of and prospects for the fast ignition inertial fusion concept

2007 ◽  
Vol 14 (5) ◽  
pp. 055502 ◽  
Author(s):  
M. H. Key
2015 ◽  
Vol 41 (9) ◽  
pp. 725-736 ◽  
Author(s):  
S. Yu. Gus’kov ◽  
N. V. Zmitrenko ◽  
D. V. Il’in ◽  
V. E. Sherman

2006 ◽  
Vol 24 (2) ◽  
pp. 269-273 ◽  
Author(s):  
ANTOINE BRET ◽  
CLAUDE DEUTSCH

In the fast ignition scenario for inertial fusion, a relativistic electron beam is supposed to travel from the side of the fusion pellet to its core. One one hand, a relativistic electron beam passing through a plasma is a highly unstable system. On the other hand, the pellet core is denser than its side by four orders of magnitude so that the beam makes its way through a important density gradient. We here investigate the effect of this gradient on the instabilities. It is found that they should develop so early that gradient effects are negligible in the linear phase.


2013 ◽  
Author(s):  
Richard Burnite Stephens ◽  
◽  
Mark N. Foord ◽  
Mingsheng Wei ◽  
Farhat N. Beg ◽  
...  

2014 ◽  
Vol 32 (3) ◽  
pp. 419-427 ◽  
Author(s):  
J.J. Honrubia ◽  
J.C. Fernández ◽  
B.M. Hegelich ◽  
M. Murakami ◽  
C.D. Enriquez

AbstractFast ignition of inertial fusion targets driven by quasi-monoenergetic ion beams is investigated by means of numerical simulations. Light and intermediate ions such as lithium, carbon, aluminum and vanadium have been considered. Simulations show that the minimum ignition energies of an ideal configuration of compressed Deuterium-Tritium are almost independent on the ion atomic number. However, they are obtained for increasing ion energies, which scale, approximately, as Z2, where Z is the ion atomic number. Assuming that the ion beam can be focused into 10 µm spots, a new irradiation scheme is proposed to reduce the ignition energies. The combination of intermediate Z ions, such as 5.5 GeV vanadium, and the new irradiation scheme allows a reduction of the number of ions required for ignition by, roughly, three orders of magnitude when compared with the standard proton fast ignition scheme.


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