Author:
Lachhvani Lavkesh,Pahari Sambaran,Goswami Rajiv,Yeole Yogesh G.,Shah Minsha,Mohurle Nikhil,Chattopadhyay Prabal K.
Abstract
AbstractConfinement time of electron plasmas trapped using a purely toroidal magnetic field has been found to exceed $${100}\, \hbox {s}$$
100
s
in a small aspect ratio ($$R_{o}/a \sim {1.59}$$
R
o
/
a
∼
1.59
, $$R_o$$
R
o
and a are device major and minor radius, respectively), partial torus. It improves upon the previously reported confinement time by nearly two orders of magnitude. Lifetime is estimated from the frequency scaling of the linear diocotron mode launched from sections of the wall, that are also used for mode diagnostics. Confinement improves as neutral pressures are reduced to $$< 5 \times 10^{-10} \hbox{mbar}$$
<
5
×
10
-
10
mbar
in the presence of a steady state magnetic field of 200 Gauss ($$\sim {60}\, \hbox {s}$$
∼
60
s
with droop $$< 0.1\%$$
<
0.1
%
) at $${100}\, \hbox {V}$$
100
V
electron injection energies. With reduced pressures the role of (ion driven) instability diminishes and loss mechanisms resulting from elastic electron–neutral (e–n) and the ubiquitous electron–electron (e–e) scattering seem to play an important role which suggests low electron temperatures. The contribution to electron population resulting from the ionization of background neutral gas at these temperatures and pressures are expected to be insignificant and is corroborated in our experiments.
Publisher
Springer Science and Business Media LLC
Cited by
1 articles.
订阅此论文施引文献
订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献