2016
DOI: 10.1063/1.4947235
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Level crossings, excess times, and transient plasma–wall interactions in fusion plasmas

Abstract: Based on a stochastic model for intermittent fluctuations in the boundary region of magnetically confined plasmas, an expression for the level crossing rate is derived from the joint distribution of the process and its derivative. From this the average time spent by the process above a certain threshold level is obtained. This provides novel predictions of plasma-wall interactions due to transient transport events associated with radial motion of blob-like structures in the scrape-off layer.

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Cited by 25 publications
(67 citation statements)
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References 18 publications
(41 reference statements)
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“…VII. Based on the foregoing discussion of pulse propagation, it is of interest to consider a stochastic process given by the super-position of a random sequence of K pulses [34][35][36][37][38][39] …”
Section: A Super-position Of Pulsesmentioning
confidence: 99%
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“…VII. Based on the foregoing discussion of pulse propagation, it is of interest to consider a stochastic process given by the super-position of a random sequence of K pulses [34][35][36][37][38][39] …”
Section: A Super-position Of Pulsesmentioning
confidence: 99%
“…[11][12][13][14][15][23][24][25][26][27][28][29][30][31][32] The present study incorporates these features in a stochastic model for intermittent plasma fluctuations in the SOL, described as a super-position of uncorrelated pulses. [34][35][36][37][38][39] This model explains many of the salient experimental findings and empirical scaling relations, including broad plasma profiles and large fluctuation levels, skewed and flattened probability density functions, and a parabolic relation between the skewness and flatness moments. The latter has been observed in the boundary region of numerous experiments on magnetized plasmas.…”
Section: Introductionmentioning
confidence: 99%
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“…The case of a one-sided exponential pulse function is readily generalized to a pulse shape that is continuous by introducing a finite pulse rise time, 79,82,88 …”
Section: B Two-sided Exponential Pulsementioning
confidence: 99%
“…A n and the mean value for the process is Φ = γ A and the variance is Φ 2 rms = γ A 2 /2. For both one-and two-sided exponential pulses, the characteristic function is C Φ (u) = (1 + iu A ) γ and the probability density function for the random variable is a Gamma distribution 85,86,88 …”
Section: Appendix A: Probability Densitiesmentioning
confidence: 99%