1973
DOI: 10.1103/physrevlett.31.690
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Runaway Electrons in a Plasma

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Cited by 134 publications
(95 citation statements)
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“…The collisional effects for runaway electrons are modeled by the Monte-Carlo method, where each collision induces changes in momentum space according to [2,4,11] ∆p = − n e e 4 ln Λm…”
Section: Theoretical Model and Numerical Algorithmmentioning
confidence: 99%
See 1 more Smart Citation
“…The collisional effects for runaway electrons are modeled by the Monte-Carlo method, where each collision induces changes in momentum space according to [2,4,11] ∆p = − n e e 4 ln Λm…”
Section: Theoretical Model and Numerical Algorithmmentioning
confidence: 99%
“…In tokamaks, relativistic runaway electrons are often observed during and after a plasma disruption or during a fast plasma shutdown [1][2][3][4]. The growth-rate of avalanche runaway electron induced by knock-on process, synchrotron radiation and magnetic fluctuations has been studied extensively [5][6][7].…”
Section: Introductionmentioning
confidence: 99%
“…where A = z/v, and the collisional flux is taken in the approximation of Maxwellian field ions and electrons with T = T. In the 2-D code 4 we use the most general expressions for the coefficients A(v) and B(v) 5 , but otherwise we work with their simpler high-energy limits Az~1+Z, B=~1…”
Section: The Distribution Function From 2-d Numerical Integrationmentioning
confidence: 99%
“…Recent researches indicate that tokamak, a magnetic confinement fusion energy device, may be the largest artificial positron factory in the world [4,5]. In large tokamaks like JET and JT-60U, above 10 14 positrons are generated in a post-disruption plasma by runaway electrons [6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22]. The dynamics of these positrons after birth in tokamaks is a noteworthy question that may yield valuable information about the runaway dynamics and disruption process in tokamaks.…”
mentioning
confidence: 99%