scholarly journals Progress in ICF programs at CAEP

2005 ◽  
Vol 23 (2) ◽  
pp. 205-209 ◽  
Author(s):  
H.S. PENG ◽  
W.Y. ZHANG ◽  
X.M. ZHANG ◽  
Y.J. TANG ◽  
W.G. ZHENG ◽  
...  

Laser technology developments, including construction of a 286-TW Ti:Sapphire laser with a focused intensity of 1021W/cm2, installation of the TIL, prototype of the SG-III, and operation of the SG-II laser are presented. Results of the experiments on hohlraum physics, indirect-drive implosion, Thomson scattering, EOS, and X-ray laser are briefly introduced. Simulations and a code package, LARED, for target physics are outlined.

Author(s):  
Chuanxiang Tang ◽  
Wenhui Huang ◽  
Renkai Li ◽  
Yingchao Du ◽  
Lixin Yan ◽  
...  
Keyword(s):  

2001 ◽  
Author(s):  
Otto L. Landen ◽  
S. H. Glenzer ◽  
Robert C. Cauble ◽  
Richard W. Lee ◽  
M. J. Edwards ◽  
...  

1999 ◽  
Vol 17 (2) ◽  
pp. 217-224 ◽  
Author(s):  
T.R. DITTRICH ◽  
S.W. HAAN ◽  
M.M. MARINAK ◽  
D.E. HINKEL ◽  
S.M. POLLAINE ◽  
...  

Several choices exist in the design and production of capsules intended to ignite and propagate fusion burn of the deuterium–tritium (D–T) fuel when imploded by indirect drive at the National Ignition Facility (NIF). These choices include ablator material, ablator dopant concentration and distribution, capsule dimensions, and X-ray drive profile (shock timings and strengths). The choice of ablator material must also include fabrication and material characteristics, such as attainable surface finishes, permeability, strength, transparency to radio frequency and infrared radiation, thermal conductivity, and material homogeneity. Understanding the advantages and/or limitations of these choices is an ongoing effort for LLNL and LANL designers. At this time, simulations in one-, two-, and three-dimensions show that capsules with either a copper-doped beryllium or a polyimide (C22H10N2O4) ablator material have both the least sensitivity to initial surface roughnesses and favorable fabrication qualities. Simulations also indicate the existence of capsule designs based on these ablator materials which ignite and burn when imploded by less than nominal laser performance (900-kJ energy, 250-TW power, producing 250-eV peak radiation temperature). We will describe and compare these reduced-scale capsules, in addition to several designs which use the expected 300-eV peak X-ray drive obtained from operating the NIF laser at 1.3 MJ and 500 TW.


Author(s):  
B. Rus ◽  
J. Dunn ◽  
T. Mocek ◽  
A. J. Nelson ◽  
M. E. Foord ◽  
...  

1999 ◽  
Vol 24 (3) ◽  
pp. 108-118
Author(s):  
Salim Al-Shamma ◽  
Muzahim Azawe ◽  
Lubna Ismail
Keyword(s):  

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