scholarly journals The weakened Weibel instability of collimated fast electron beam in nanotube array

2017 ◽  
Vol 35 (1) ◽  
pp. 120-125
Author(s):  
L. Liao ◽  
R. Zhao ◽  
Y. Bie ◽  
H. Zhang ◽  
C. Hu

AbstractThe Weibel instability of the collimated MeV fast electron beams in a nanotube array target is researched in this work. It is found that the filamentation of the fast electrons is significantly suppressed. When fast electrons propagate the nanotube array, a strong magnetic field is created near the surface of tubes to obstruct the transverse movement of the fast electrons and bend them into the inner vacuum spaces between the successive tubes. In consequence, the positive feedback loop between the magnetic field perturbation and the electrons density perturbation is broken and the Weibel instability is thus weakened. Furthermore, the calculated results by a hybrid particle-in-cell code have also proven this weakening effect on the Weibel instability. Because of the high-energy density delivered by the MeV electrons, these results indicate some significant applications in the high-energy physics, such as radiography, fast-electron beam focusing, and perhaps fast ignition.

Author(s):  
D. Kawahito ◽  
M. Bailly-Grandvaux ◽  
M. Dozières ◽  
C. McGuffey ◽  
P. Forestier-Colleoni ◽  
...  

Inertial confinement fusion approaches involve the creation of high-energy-density states through compression. High gain scenarios may be enabled by the beneficial heating from fast electrons produced with an intense laser and by energy containment with a high-strength magnetic field. Here, we report experimental measurements from a configuration integrating a magnetized, imploded cylindrical plasma and intense laser-driven electrons as well as multi-stage simulations that show fast electrons transport pathways at different times during the implosion and quantify their energy deposition contribution. The experiment consisted of a CH foam cylinder, inside an external coaxial magnetic field of 5 T, that was imploded using 36 OMEGA laser beams. Two-dimensional (2D) hydrodynamic modelling predicts the CH density reaches 9.0   g cm − 3 , the temperature reaches 920 eV and the external B-field is amplified at maximum compression to 580 T. At pre-determined times during the compression, the intense OMEGA EP laser irradiated one end of the cylinder to accelerate relativistic electrons into the dense imploded plasma providing additional heating. The relativistic electron beam generation was simulated using a 2D particle-in-cell (PIC) code. Finally, three-dimensional hybrid-PIC simulations calculated the electron propagation and energy deposition inside the target and revealed the roles the compressed and self-generated B-fields play in transport. During a time window before the maximum compression time, the self-generated B-field on the compression front confines the injected electrons inside the target, increasing the temperature through Joule heating. For a stronger B-field seed of 20 T, the electrons are predicted to be guided into the compressed target and provide additional collisional heating. This article is part of a discussion meeting issue ‘Prospects for high gain inertial fusion energy (part 2)’.


2015 ◽  
Vol 33 (3) ◽  
pp. 525-534 ◽  
Author(s):  
D. Del Sorbo ◽  
Y. Arikawa ◽  
D. Batani ◽  
F. Beg ◽  
J. Breil ◽  
...  

AbstractThe transport of relativistic electron beam in compressed cylindrical targets was studied from a numerical and experimental point of view. In the experiment, cylindrical targets were imploded using the Gekko XII laser facility of the Institute of Laser Engineering. Then the fast electron beam was created by shooting the LFEX laser beam. The penetration of fast electrons was studied by observing Kα emission from tracer layers in the target.


1995 ◽  
Vol 26 (3-4) ◽  
pp. 131-140 ◽  
Author(s):  
N. Glezos ◽  
I. Raptis ◽  
M. Hatzakis

1985 ◽  
Vol 45 ◽  
Author(s):  
Y. Hayafuji ◽  
A. Shibata ◽  
T. Yanada ◽  
A. Sawada ◽  
S. Usui ◽  
...  

ABSTRACTThe line-shaped electron beam annealing system which generates an electron beam of a length of 4 cm and a width af less than 100 um with a high energy density exceeding well over 100 kW/cm2 was developed for the first time with a purpose of SOI processing as its primary application. An pccelaration voltage of up to 20 kV can be used in this system. Seeded single crystalline islands with areas several mm long and 30 to 100 um in width were obtained by a single scan of the electron beam. The electron beam is generated in a pulsed way in the system due to the power restriction of the power supplies. An area of 4×5 cm2 was processed by a single scan of an electron beam at a sample speed of 530 cm/sec and a beam duration of 9.5 msec. The scanning area for one scan is determined by the beam length and the duration of the beam and sample speed.The present system could give single crystalline silicon films without any grain boundaries. The electron mobility of the electron beam recrystallized films, obtained from FETs made as a vehicle to test the electrical properties of the films, was comparable to that of the bulk silicon. A very rapid migration of silicon atoms in solid polycrystalline silicon films, which is controllable by process parameters, was also found with a migration speed of the order of 1 m/sec in a capped structure. The present electron beam system is useful in studying basic mechanisms of crystal growth in thin films. The system can have a very high throughput, a desirable feature in semiconductor industry. The present system can also be used to study the rapid thermal treatment of materials other than semiconductors including rapidly solidified materials.


2001 ◽  
Vol 89 (1) ◽  
pp. 654-661
Author(s):  
Chong-Yu Ruan ◽  
Manfred Fink

2005 ◽  
Vol 33 (5) ◽  
pp. 1648-1653 ◽  
Author(s):  
Y.D. Korolev ◽  
O.B. Frants ◽  
V.G. Geyman ◽  
N.V. Landl ◽  
R.V. Ivashov ◽  
...  

2011 ◽  
Vol 53 (12) ◽  
pp. 124012 ◽  
Author(s):  
M N Quinn ◽  
D C Carroll ◽  
X H Yuan ◽  
M Borghesi ◽  
R J Clarke ◽  
...  

2010 ◽  
Vol 12 (6) ◽  
pp. 063018 ◽  
Author(s):  
X H Yuan ◽  
A P L Robinson ◽  
M N Quinn ◽  
D C Carroll ◽  
M Borghesi ◽  
...  

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