Fusion Energy with Krypton Fluoride Lasers and Direct Drive Targets

2012 ◽  
Vol 61 (1T) ◽  
pp. 41-46
Author(s):  
John D. Sethian ◽  
Steve Obenschain
2001 ◽  
Vol 19 (4) ◽  
pp. 609-622 ◽  
Author(s):  
V.D. ZVORYKIN ◽  
S.V. ARLANTSEV ◽  
V.G. BAKAEV ◽  
O.V. RANTSEV ◽  
P.B. SERGEEV ◽  
...  

Two of the key issues of a krypton fluoride (KrF) laser driver for inertial fusion energy are the development of long life, high transparency pressure foils (to isolate vacuum in the electron beam diode from a working gas in the laser chamber), and the development of durable, stable, optical windows. Both of these problems have been studied on the single-pulse e-beam-pumped KrF laser installation GARPUN. We have measured the transport of electron beams (300 keV, 50 kA, 100 ns, 10 × 100 cm) through aluminum-beryllium and titanium foils and compared them with Monte Carlo numerical calculations. It was shown that 50-μm thickness Al-Be and 20-μm Ti foils had equal transmittance. However, in contrast to Ti foil, whose surface was strongly etched by fluorine, no surface modification nor fatal damages were observed for Al-Be foils after ∼1000 laser shots and protracted fluorine exposure. We also measured the 8% reduction in the transmission of CaF2 windows under irradiation by scattered electrons when they were set at 8.5 cm apart from the e-beam-pumped region. However an applied magnetic field of ∼0.1 T significantly reduced electron scattering both across and along the laser cell at typical pumping conditions with 1.5 atm pressure working gas. Thus the e-beam-induced absorption of laser radiation in optical windows might be fully eliminated in an e-beam-pumping scheme with magnetic field guiding.


2004 ◽  
Vol 92 (7) ◽  
pp. 1043-1056 ◽  
Author(s):  
J.D. Sethian ◽  
R.V. Smilgys ◽  
S.B. Swanekamp ◽  
D. Weidenheimer ◽  
D. Giorgi ◽  
...  

1993 ◽  
Vol 11 (1) ◽  
pp. 177-184 ◽  
Author(s):  
M. Aydin ◽  
H. Hora

Smoothing of laser-plasma interaction by ISI, RPP, SSD, etc. was mainly directed to overcome lateral nonuniformity of irradiation. While these problems are in no way less important, we derived numerically the model of the Laue rippling and hydrorelaxation model for explanation of the measured temporal pulsation in the 10- to 40-ps range and how the smoothing schemes suppress these pulsations. The partial standing wave fields of the normally coherent laser-irradiated plasma corona is then suppressed by smoothing and conclusion for tests for this model, e.g., by the “question mark experiment” is given. The result provides a physics solution of the laser interaction problem for direct-drive inertial fusion energy


2013 ◽  
Vol 64 (2) ◽  
pp. 179-186 ◽  
Author(s):  
Matthew F. Wolford ◽  
John D. Sethian ◽  
Matthew C. Myers ◽  
Frank Hegeler ◽  
John L. Giuliani ◽  
...  

2010 ◽  
Vol 38 (4) ◽  
pp. 690-703 ◽  
Author(s):  
J D Sethian ◽  
D G Colombant ◽  
J L Giuliani ◽  
R H Lehmberg ◽  
M C Myers ◽  
...  
Keyword(s):  

2003 ◽  
Vol 43 (3) ◽  
pp. 353-358 ◽  
Author(s):  
William Samuel Rickman ◽  
Daniel T. Goodin

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