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| 001 | 281498 | ||
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| 100 | 1 | _ | |a Wongrach, K. |0 P:(DE-HGF)0 |b 0 |
| 245 | _ | _ | |a Structure of the runaway electron loss during induced disruptions in TEXTOR |
| 260 | _ | _ | |a [S.l.] |c 2015 |b American Institute of Physics |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1453973250_29955 |2 PUB:(DE-HGF) |
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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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| 700 | 1 | _ | |a Willi, O. |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a Zeng, L. |0 P:(DE-Juel1)145673 |b 4 |
| 700 | 1 | _ | |a Xu, Y. |0 P:(DE-Juel1)130198 |b 5 |
| 773 | _ | _ | |a 10.1063/1.4933131 |g Vol. 22, no. 10, p. 102508 - |0 PERI:(DE-600)1472746-8 |n 10 |p 102508 - |t Physics of plasmas |v 22 |y 2015 |x 1089-7674 |
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