Nd:YAG laser Thomson scattering diagnostics for a laboratory magnetosphere

N Kenmochi; M Nishiura; Z Yoshida; I Yamada; H Funaba; T Sugata; K Nakamura; S Katsura

doi:10.1063/1.5037473

Nd:YAG laser Thomson scattering diagnostics for a laboratory magnetosphere

Rev Sci Instrum. 2018 Oct;89(10):10C101. doi: 10.1063/1.5037473.

Authors

N Kenmochi¹, M Nishiura¹, Z Yoshida¹, I Yamada², H Funaba², T Sugata¹, K Nakamura¹, S Katsura¹

Affiliations

¹ Graduate School of Frontier Sciences, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan.
² National Institute for Fusion Science, 322-6 Oroshi-cho, Toki, Gifu 509-5292, Japan.

PMID: 30399734
DOI: 10.1063/1.5037473

Abstract

A new Nd:YAG laser Thomson scattering (TS) system has been developed to explore the mechanism of high-beta plasma formation in the RT-1 device. The TS system is designed to measure electron temperatures (T_e) from 10 eV to 50 keV and electron densities (n_e) of more than 1.0 × 10¹⁷ m^-3. To measure at the low-density limit, the receiving optics views the long scattering length (60 mm) using a bright optical system with both a large collection window (260-mm diameter) and large collection lenses (300-mm diameter, a solid angle of ∼68 × 10^-3 str). The scattered light of the 1.2-J Nd:YAG laser (repetition frequency: 10 Hz) is detected with a scattering angle of 90° and is transferred via a set of lenses and an optical fiber bundle to a polychromator. After Raman scattering measurement for the optical alignment and an absolute calibration, we successfully measured T_e = 72.2 eV and n_e = 0.43 × 10¹⁶ m^-3 for the coil-supported case and T_e = 79.2 eV and n_e = 1.28 × 10¹⁶ m^-3 for the coil-levitated case near the inner edge in the magnetospheric plasmas.