High power industrial laser and present status of development of laser technology in automated branches of industry abroad (survey)

1991 ◽  
Vol 12 (3) ◽  
pp. 237-249
Author(s):  
P. G. Grigor'ev ◽  
A. A. Stepanov ◽  
V. A. Shcheglov
1998 ◽  
Vol 59 (4) ◽  
pp. 587-610 ◽  
Author(s):  
P. E. VANDENPLAS ◽  
A. M. MESSIAEN ◽  
J. P. H. E. ONGENA ◽  
U. SAMM ◽  
B. UNTERBERG

From 1990, the boronized TEXTOR tokamak was characterized by an improved confinement (coined the ‘I mode’) at high power that was substantially better than the L mode, but densities had to be limited to n[bar]e0/nGR[lsim ]0.5–0.6, where nGR is the Greenwald density limit. With the injection of Ne, Si or Ar in order to increase the edge radiation and provided that γ=Prad/Ptot[greater, similar]0.5, PNBI-co/Ptot[greater, similar]0.25 and n[bar]e0/nGR[greater, similar]0.75, a further improved confinement called the radiative improved mode (RI mode) was discovered in 1993 on TEXTOR, a tokamak of intermediate size, and confirmed on TEXTOR-94. The radiated power fraction γ can reach 0.9, and the radiation is nearly isotropically distributed over the torus wall. The RI mode is characterized by its ability to obtain simultaneously and stationarily high densities and high confinement. It is linked to a substantial lowering of edge ne, Te and Ti, a reduction in particle transport and a peaking of the density profile. The RI-mode confinement scales on TEXTOR as τE= (n[bar]e0/nGR)τITERH93-P and values up to n[bar]e0/nGR≈1.2 are obtained. There is no detrimental concentration of the seeded impurity at the centre of the plasma. Results of three different interpretative and modelling approaches are in agreement with the improved confinement features; the preliminary indications are that ITG turbulence is strongly reduced. The Z mode observed on ISX-B has a clear resemblance to the RI mode. The very favourable features of the RI mode justify efforts in trying to establish it on larger machines to verify if the present scaling then holds.


2020 ◽  
Vol 49 (12) ◽  
pp. 20201076-20201076
Author(s):  
白振旭 Zhenxu Bai ◽  
杨学宗 Xuezong Yang ◽  
陈晖 Hui Chen ◽  
金舵 Duo Jin ◽  
丁洁 Jie Ding ◽  
...  

2021 ◽  
Author(s):  
Jianqiang Zhu ◽  
Xiaoqi Zhang ◽  
Zhixiang Zhang ◽  
Jiangfeng Wang ◽  
Hui Wei ◽  
...  

2002 ◽  
Author(s):  
Petr G. Eliseev ◽  
Andrei A. Ionin ◽  
Yurii M. Klimachev ◽  
Dmitrii V. Sinitsyn ◽  
Jinhyun Lee ◽  
...  

1989 ◽  
Vol 7 (3) ◽  
pp. 383-392 ◽  
Author(s):  
Y. Owadano ◽  
I. Okuda ◽  
Y. Matsumoto ◽  
M. Tanimoto ◽  
T. Tomie ◽  
...  

The present status of the development of a high-power KrF laser system, Ashura, is described. The main amplifier has generated 710 J (95 ns) at the pumping density of 1·lMW/cm3 with the wall plug efficiency of 2·0%. Maximum power of 9·0 GW (200 J/22 ns) per beam has been obtained from the beam lines of six-time pulse multiplexing. Power density of 1 × 1014 W/cm2 has been achieved on target with a 10−6 pre-pulse.


2017 ◽  
Author(s):  
Sameeh I. Batarseh ◽  
Ramona Graves ◽  
Omar Al Obaid ◽  
Abdullah Al Hartih ◽  
Haitham Othman

1994 ◽  
Author(s):  
Alexei A. Betev ◽  
Leonid I. Danilov ◽  
Vyatcheslav T. Karpukhin ◽  
Yuri B. Konev ◽  
Yurii V. Lipukhin

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