TY - JOUR
T1 - Identification of waves by RF magnetic probes during lower hybrid wave injection experiments on the TST-2 spherical tokamak
AU - Shinya, Takahiro
AU - Ejiri, Akira
AU - Takase, Yuichi
AU - Wakatsuki, Takuma
AU - Oosako, Takuya
AU - Tsujii, Naoto
AU - Kakuda, Hidetoshi
AU - Furui, Hirokazu
AU - Hiratsuka, Junichi
AU - Inada, Takuma
AU - Imamura, Kazuhiro
AU - Nakamura, Keishun
AU - Nakanishi, Ayaka
AU - Sonehara, Masateru
AU - Togashi, Hiro
AU - Tsuda, Shintaro
AU - Yamaguchi, Takashi
AU - Kasahara, Hiroshi
AU - Saito, Kenji
AU - Seki, Tetsuo
AU - Shimpo, Fujio
AU - Nagashima, Yoshihiko
AU - Watanabe, Osamu
AU - Yamada, Takuma
N1 - Publisher Copyright:
© 2014 The Japan Society of Plasma Science and Nuclear Fusion Research.
PY - 2014
Y1 - 2014
N2 - RF magnetic probes can be used to measure not only the wavevector, but also the polarization of waves in plasmas. A 5-channel RF magnetic probe (5ch-RFMP) was installed in the TST-2 spherical tokamak and the waves were studied in detail during lower hybrid wave injection experiments. From the polarization measurements, the poloidal RF magnetic field is found to be dominant. In addition to polarization, components of k perpendicular to the major radial direction were obtained from phase differences among the five channels. The radial wavenumber was obtained by scanning the radial position of the 5ch-RFMP on a shot by shot basis. The measured wavevector and polarization in the plasma edge region were consistent with those calculated from the wave equation for the slow wave branch. While the waves with small and large k∥ were excited by the antenna, only the small k∥ component was measured by the 5ch-RFMP; this suggests that the waves with larger k∥ were absorbed by the plasma.
AB - RF magnetic probes can be used to measure not only the wavevector, but also the polarization of waves in plasmas. A 5-channel RF magnetic probe (5ch-RFMP) was installed in the TST-2 spherical tokamak and the waves were studied in detail during lower hybrid wave injection experiments. From the polarization measurements, the poloidal RF magnetic field is found to be dominant. In addition to polarization, components of k perpendicular to the major radial direction were obtained from phase differences among the five channels. The radial wavenumber was obtained by scanning the radial position of the 5ch-RFMP on a shot by shot basis. The measured wavevector and polarization in the plasma edge region were consistent with those calculated from the wave equation for the slow wave branch. While the waves with small and large k∥ were excited by the antenna, only the small k∥ component was measured by the 5ch-RFMP; this suggests that the waves with larger k∥ were absorbed by the plasma.
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U2 - 10.1585/pfr.9.3402040
DO - 10.1585/pfr.9.3402040
M3 - Article
AN - SCOPUS:84945280004
SN - 1880-6821
VL - 9
JO - Plasma and Fusion Research
JF - Plasma and Fusion Research
IS - SpecialIssue2
M1 - 3402040
ER -