This title appears in the Scientific Report :
2015
Please use the identifier:
http://hdl.handle.net/2128/9788 in citations.
Please use the identifier: http://dx.doi.org/10.1063/1.4933131 in citations.
Structure of the runaway electron loss during induced disruptions in TEXTOR
Structure of the runaway electron loss during induced disruptions in TEXTOR
The loss of runaway electrons during an induced disruption is recorded by a synchrotron imaging technique using a fast infrared CCD camera. The loss is predominantly diffuse. During the “spiky-loss phase”, when the runaway beam moves close to the wall, a narrow channel between the runaway column and...
Saved in:
Personal Name(s): | Wongrach, K. |
---|---|
Finken, K. H. / Abdullaev, Sadrilla / Willi, O. / Zeng, L. / Xu, Y. | |
Contributing Institute: |
Plasmaphysik; IEK-4 |
Published in: | Physics of plasmas, 22 (2015) 10, S. 102508 - |
Imprint: |
[S.l.]
American Institute of Physics
2015
|
DOI: |
10.1063/1.4933131 |
Document Type: |
Journal Article |
Research Program: |
Tokamak Physics |
Link: |
OpenAccess OpenAccess |
Publikationsportal JuSER |
Please use the identifier: http://dx.doi.org/10.1063/1.4933131 in citations.
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520 | |a The loss of runaway electrons during an induced disruption is recorded by a synchrotron imaging technique using a fast infrared CCD camera. The loss is predominantly diffuse. During the “spiky-loss phase”, when the runaway beam moves close to the wall, a narrow channel between the runaway column and a scintillator probe is formed and lasts until the runaway beam is terminated. In some cases, the processed images show a stripe pattern at the plasma edge. A comparison between the MHD dominated disruptions and the MHD-free disruption is performed. A new mechanism of plasma disruptions with the runaway electron generation and a novel model which reproduces many characteristic features of the plasma beam evolution during a disruption is briefly described. | ||
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