Corrigendum: Study of the effect of sawteeth on fast ions and neutron emission in MAST using a neutron camera (2018 Plasma Phys. Control. Fusion 60 055008)

2019 ◽  
Vol 61 (12) ◽  
pp. 129501
Author(s):  
M Cecconello ◽  
A Sperduti ◽  
2009 ◽  
Vol 76 (1) ◽  
pp. 101-106 ◽  
Author(s):  
X. YANG ◽  
J. LIU ◽  
T. GAO ◽  
M. LI ◽  
Y. J. SHI ◽  
...  

AbstractRunaway transport is used to probe the magnetic fluctuation level for TEXTOR disruption plasmas. A zero-dimensional model of the current quench including the generation of runaway electrons has been applied to simulate the experimental current evolution during major disruptions [Plasma Phys. Control. Fusion50 (2008), 105007]. According to the loss rate of runaway electrons used in the fitting parameter of the zero-dimensional model, the magnetic fluctuation level in TEXTOR is derived. It is found that the magnetic fluctuation level is in the order of 10−5, and it increases with the atom number mixed into the plasma.


2018 ◽  
Vol 60 (9) ◽  
pp. 099501
Author(s):  
James K Koga ◽  
Sergei V Bulanov ◽  
Timur Zh Esirkepov ◽  
Masaki Kando ◽  
Stepan S Bulanov ◽  
...  

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)].


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