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CALSCALE:GREGORIAN
PRODID:UW-Madison-Physics-Events
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SEQUENCE:1
UID:UW-Physics-Event-8646
DTSTART:20240304T180000Z
DTEND:20240304T191500Z
DTSTAMP:20260413T223402Z
LAST-MODIFIED:20240228T082537Z
LOCATION:1227 Engineering Hall
SUMMARY:Schnack Memorial Seminar: "Plasma instabilities associated wit
 h runaway electron beam and their potential influences”\, Plasma Phy
 sics (Physics/ECE/NE 922) Seminar\, Dr. Chang Liu\, PPPL (Princeton Pl
 asma Physics Laboratory)
DESCRIPTION:High-energy runaway electron beams can be generated in fus
 ion experiments during various discharge phases. Control and mitigatio
 n of runaway electron beams and reducing their energy impact on the pl
 asma-facing walls is critical to the operation of ITER and other tokam
 aks. Interestingly\, the high energy of these electrons can also provo
 ke plasma instabilities\, creating pathways for the electrons to dissi
 pate energy and diffuse in space. In this presentation\, I will discus
 s some of the common instabilities driven by runaway electrons observe
 d in experiments and the efforts to model them. High-frequency plasma 
 waves\, such as whistler and extraordinary electron (EXEL) waves\, can
  be stimulated by the anisotropic distribution of runaway electrons an
 d resonating with their cyclotron motion. This resonance can lead to r
 apid pitch-angle scattering\, manifested as an abrupt increase in elec
 tron cyclotron emission (ECE) signals. In addition\, these instabiliti
 es can affect the runaway electrons' avalanche growth and raise the cr
 itical electric field for the transition from growth to decay of runaw
 ay electron population. Lower frequency plasma waves can also be excit
 ed if they resonate with the precession motion of the trapped runaway 
 electrons. The excitation of plasma instabilities in the Alfvén frequ
 ency range has been observed in DIII-D\, AUG and JET disruption experi
 ments\, and has been shown to contribute to the loss of runaway electr
 ons during current quench. The interaction between these Alfvén oscil
 lations in the background plasma and runaway electrons can be explored
  through kinetic-MHD simulations\, including calculations of linear gr
 owth\, nonlinear saturation\, and the consequent transport of runaway 
 electrons.
URL:https://www.physics.wisc.edu/events/?id=8646
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