2006
DOI: 10.1103/physrevlett.97.045006
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Properties of Geodesic Acoustic Modes and the Relation to Density Fluctuations

Abstract: The geodesic acoustic mode (GAM) is a high frequency branch of zonal flows, which is observed in toroidal plasmas. Because of toroidal curvature effects, density fluctuations are excited, which are investigated with the O-mode correlation reflectometer at TEXTOR. This Letter reports on the poloidal distribution of GAM induced density fluctuation and compares them with theoretical predictions. The influence of the GAM flows on the ambient turbulence is studied, too.

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Cited by 90 publications
(125 citation statements)
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“…These findings were confirmed by measurements with the hydrogen diagnostic beam RUDI [35]. Also the application of the upgraded reflectometer system allowed to observe geodesic acoustic modes in the plasma edge and resolve their role for density fluctuations and the impact of RMP on this important high frequency zonal flow domain [36]. The heat transport characteristics in the transition region between the stochastic layer and the core plasma, i.e.…”
Section: Resultssupporting
confidence: 59%
“…These findings were confirmed by measurements with the hydrogen diagnostic beam RUDI [35]. Also the application of the upgraded reflectometer system allowed to observe geodesic acoustic modes in the plasma edge and resolve their role for density fluctuations and the impact of RMP on this important high frequency zonal flow domain [36]. The heat transport characteristics in the transition region between the stochastic layer and the core plasma, i.e.…”
Section: Resultssupporting
confidence: 59%
“…Linearizing the above set of equations (19)(20)(21)(22)(23)(24)(25), taking Fourier transforms and neglecting n , T i,e , one obtains the following dispersion relation…”
Section: A Linear Gam Dispersionmentioning
confidence: 99%
“…Otherwise they are excited by nonlinear processes like turbulent reynolds stresses [12][13][14][15][16][17][18], poloidally asymmetric particle fluxes [19] and heat fluxes [20]. Due to their finite frequency (usually a few kHz), distinct from that of broadband turbulence, GAMs are easier to detect, and thus have been observed on several tokamaks such as ASDEX Upgrade (AUG) [21] using Doppler backscattering (DBS), TEXTOR [22]using O-mode correlation reflectometer, and DIIID [23] using beam emission spectroscopy (BES). As of today, GAMS are observed in the majority of the tokamaks in the world including recent observations of GAMs in Tore Supra [24] using a DBS system.…”
Section: Introductionmentioning
confidence: 99%
“…Thus, it is a powerful tool for the study of Zonal flow, which has a E r perturbation radially localized in toroidal plasmas [4,5,6]. Because of the flexibility of the diagnostic arrangements, the spatiotemporal characteristics of Zonal flows were obtained in both L-mode and H-mode plasmas [7,8,9,10], even the spatial distribution of GAM in density fluctuation was evidenced by poloidal correlation reflectometry [11].…”
Section: Introductionmentioning
confidence: 99%