scholarly journals Ion beam requirements for fast ignition of inertial fusion targets

2015 ◽  
Vol 22 (1) ◽  
pp. 012703 ◽  
Author(s):  
J. J. Honrubia ◽  
M. Murakami
2015 ◽  
Vol 41 (9) ◽  
pp. 725-736 ◽  
Author(s):  
S. Yu. Gus’kov ◽  
N. V. Zmitrenko ◽  
D. V. Il’in ◽  
V. E. Sherman

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.


2010 ◽  
Vol 36 (6) ◽  
pp. 473-481 ◽  
Author(s):  
S. Yu. Gus’kov ◽  
D. V. Il’in ◽  
J. Limpouch ◽  
O. Klimo ◽  
V. E. Sherman

2002 ◽  
Vol 20 (3) ◽  
pp. 415-418 ◽  
Author(s):  
V.V. VATULIN ◽  
O.A. VINOKUROV

The so-called fast ignition mode is one way to ignite the thermonuclear fuel in systems of inertial fusion and decrease of the necessary energy of the driver. In the present work the second stage of the process—the heating, the thermonuclear burning initiation under the influence of a powerful ion pulse, and distribution of the burning all over the rest of the cylindrical system—is studied. The main purpose of the presented calculations was to determine the threshold of the fast ignition of the cylindrical DT cord by a heavy ion beam.


1999 ◽  
Vol 75 (2) ◽  
pp. 121-125
Author(s):  
Masao OGAWA ◽  
Kazuhiko HORIOKA ◽  
Toshiyuki HATTORI

2017 ◽  
Vol 35 (2) ◽  
pp. 373-378 ◽  
Author(s):  
P.A. Seidl ◽  
J.J. Barnard ◽  
E. Feinberg ◽  
A. Friedman ◽  
E.P. Gilson ◽  
...  

AbstractWe present an overview of the performance of the Neutralized Drift Compression Experiment-II (NDCX-II) accelerator at Berkeley Lab, and report on recent target experiments on beam-driven melting and transmission ion energy loss measurements with nanosecond and millimeter-scale ion beam pulses and thin tin foils. Bunches with around 1011 ions, 1 mm radius, and 2–30 ns full width at half maximum duration have been created with corresponding fluences in the range of 0.1–0.7 J/cm2. To achieve these short pulse durations and mm-scale focal spot radii, the 1.1 MeV [megaelectronvolt (106 eV)] He+ ion beam is neutralized in a drift compression section, which removes the space charge defocusing effect during final compression and focusing. The beam space charge and drift compression techniques resemble necessary beam conditions and manipulations in heavy ion inertial fusion accelerators. Quantitative comparison of detailed particle-in-cell simulations with the experiment plays an important role in optimizing accelerator performance.


Author(s):  
Tetsuo Someya ◽  
Aleksandar I. Ogoyski ◽  
Shigeo Kawata ◽  
Toru Sasaki

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