Laser-Driven Ablation Front in ICF

Author(s):  
Paul Clavin ◽  
Geoff Searby
Keyword(s):  
2006 ◽  
Vol 96 (11) ◽  
Author(s):  
O. V. Gotchev ◽  
V. N. Goncharov ◽  
J. P. Knauer ◽  
T. R. Boehly ◽  
T. J. B. Collins ◽  
...  

1991 ◽  
Vol 9 (2) ◽  
pp. 273-281 ◽  
Author(s):  
J. Sanz ◽  
A. Estevez

The Rayleigh—Taylor instability is studied by means of a slab model and when slab thickness D is comparable to the ablation-to-critical surface distance. Under these conditions the perturbations originating at the ablation front reach the critical surface, and in order to determine the instability growth rate, we must impose boundary conditions at the corona. Stabilization occurs for perturbation wave numbers such that kD ˜ 10.


1977 ◽  
Vol 55 (12) ◽  
pp. 1047-1054 ◽  
Author(s):  
Boye Ahlborn

The particle end losses from a linear magnetic fusion reactor can be suppressed by establishing an ablation front in a cold gas blanket. The power density W(W/cm2) to drive the thermal front may be drawn from inside (energy end losses) or outside (auxiliary heating). With W below 109 W/cm2 and a D–T blanket the particle outflow is retarded. With higher W values the flow is completely stopped and the fusion plasma is recompressed by a shock wave traveling inwards from the ends.


Author(s):  
D.T. Michel ◽  
A.K. Davis ◽  
W. Armstrong ◽  
R. Bahr ◽  
R. Epstein ◽  
...  

Self-emission x-ray shadowgraphy provides a method to measure the ablation-front trajectory and low-mode nonuniformity of a target imploded by directly illuminating a fusion capsule with laser beams. The technique uses time-resolved images of soft x-rays ( ${>}1$  keV) emitted from the coronal plasma of the target imaged onto an x-ray framing camera to determine the position of the ablation front. Methods used to accurately measure the ablation-front radius ( ${\it\delta}R=\pm 1.15~{\rm\mu}\text{m}$ ), image-to-image timing ( ${\it\delta}({\rm\Delta}t)=\pm 2.5$  ps) and absolute timing ( ${\it\delta}t=\pm 10$  ps) are presented. Angular averaging of the images provides an average radius measurement of ${\it\delta}(R_{\text{av}})=\pm 0.15~{\rm\mu}\text{m}$ and an error in velocity of ${\it\delta}V/V=\pm 3\%$ . This technique was applied on the Omega Laser Facility [Boehly et al., Opt. Commun. 133, 495 (1997)] and the National Ignition Facility [Campbell and Hogan, Plasma Phys. Control. Fusion 41, B39 (1999)].


2021 ◽  
Vol 158 ◽  
pp. 108297
Author(s):  
Akinobu Morita ◽  
Akitoshi Hotta ◽  
Noboru Yamazaki

2014 ◽  
Vol 21 (12) ◽  
pp. 122702 ◽  
Author(s):  
A. Casner ◽  
L. Masse ◽  
B. Delorme ◽  
D. Martinez ◽  
G. Huser ◽  
...  

Author(s):  
B.A. Remington ◽  
M.M. Marinak ◽  
S.V. Weber ◽  
K.S. Budil ◽  
O.L. Landen ◽  
...  

2001 ◽  
Author(s):  
Andre L. Richard ◽  
B. Meyer ◽  
P. Salvatore ◽  
Philippe Troussel ◽  
Pascal Munsch ◽  
...  

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