TJ-II:Excitation of zonal flow oscillations by energetic particles: Difference between revisions

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(Created page with "== Experimental campaign == 2017 Spring == Proposal title == '''Excitation of zonal flow oscillations by energetic particles''' == Name and affiliation of proponent == Edilb...")
 
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'''Motivation'''
'''Motivation'''


In stellarators the zonal flows (ZF) undergo several oscillations depending on the magnetic geometry and the plasma conditions. First, a Geodesic Acoustic Mode (GAM) oscillation, similar to that in tokamaks, appears, whose collisionless damping strongly depends on the rotational transform. A new oscillation, at a lower frequency, recently discovered theoretically [Mishchenko PoP 2008], appears in stelallarators that is not present in quasisymmetric devices. In TJ-II, both oscillations have been found in simulations [Sánchez PPCF 2013] and the low frequency one has been identified for the first time during pellet injection experiments [Alonso PRL 2017]. Other experimental evidences appear to be related to zonal flow oscillations, both low frequency  [Pedrosa PoP 2008] and GAM [Castejón PPCF 2016].  
In stellarators the zonal flows (ZF) undergo several oscillations depending on the magnetic geometry and the plasma conditions. First, a Geodesic Acoustic Mode (GAM) oscillation, similar to that in tokamaks, appears, whose collisionless damping strongly depends on the rotational transform. A new oscillation, at a lower frequency, recently discovered theoretically <ref>Mishchenko PoP 2008</ref>, appears in stelallarators that is not present in quasisymmetric devices. In TJ-II, both oscillations have been found in simulations <ref>Sánchez PPCF 2013</ref> and the low frequency one has been identified for the first time during pellet injection experiments <ref>Alonso PRL 2017</ref>. Other experimental evidences appear to be related to zonal flow oscillations, both low frequency  <ref>Pedrosa PoP 2008</ref> and GAM <ref>Castejón PPCF 2016</ref>.  


According to gyrokinetic simulations, the GAM and LFO oscillations are damped in the TJ-II geometry (even collisionlessly) and the necessary driving mechanism has not been identified so far. The turbulence can drive (non-linearly) these oscillations, but it is not the only option as driving mechanism.  
According to gyrokinetic simulations, the GAM and LFO oscillations are damped in the TJ-II geometry (even collisionlessly) and the necessary driving mechanism has not been identified so far. The turbulence can drive (non-linearly) these oscillations, but it is not the only option as driving mechanism.  
In tokamaks it has been found that energetic particles can drive the GAM oscillation (EGAMs) [Zarzoso PRL 2013 and reference therein], but in stellarators there are less evidences [Sun EFL 2016] and the oscillation fauna is wider than in tokamaks.
In tokamaks it has been found that energetic particles can drive the GAM oscillation (EGAMs) <ref>Zarzoso PRL 2013 and reference therein</ref>, but in stellarators there are less evidences <ref>Sun EFL 2016</ref> and the oscillation fauna is wider than in tokamaks.
   
   


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Preferred dates: (format dd-mm-yyyy)
Preferred dates: (format dd-mm-yyyy)


== References ==
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