A yttrium-aluminum-garnet Thomson scattering (TS) system was constructed and applied to the tandem mirror GAMMA 10 plasma to measure the electron temperature. A large solid-angle TS light-collection system was set using a spherical mirror system and a large numerical aperture of bundled optical fiber. A five-channel polychromator with avalanche silicon photo diodes was employed after being calibrated with standard light. Calibration was performed by Rayleigh and Raman scattering. An electron temperature increase from 40 eV to 80 eV was observed with application of electron cyclotron heating to plug/barrier cells. GAMMA 10 is the world largest tandem mirror machine with which plasma confinement is achieved not only by a magnetic mirror configuration but also high potentials at both end regions [1][2][3]. The main plasma is produced and heated by ion-cyclotron range of frequency waves. The confinement potentials are produced by plug and barrier electron cyclotron heating (P/B-ECH) at the plug/barrier regions. During the formation of confinement potential, the typical electron density, electron temperature, and ion temperature are about 2 × 10 18 m −3 , 0.1 keV, and 5 keV, respectively. Thomson scattering (TS) is the most reliable diagnostic for measuring electron temperature and electron density. In GAMMA 10, a ruby-laser TS system was installed to measure the electron temperature. However, the system experienced problems. Previously, electron temperature has been measured by soft X-ray measurement. Thus far, direct electron heating by ECH experiments have been conducted in the central cell. In addition, density and potential fluctuation suppressions during the formation of confinement potential have been studied using a gold neutral beam probe system [1][2][3]. After the aforementioned problems with the ruby-laser TS system, we planned to install a neodymiumdoped, yttrium-aluminum-garnet laser (Nd:YAG) TS system to measure electron temperature directly in the central cell of GAMMA 10. In comparison with the ruby-laser author's e-mail: yosikawa@prc.tsukuba.ac.jp system, operation of the YAG laser system is easier and the repetition rate of such a system is much larger. The YAG TS system is normally used in higher electron density plasmas, over 10 19 m −3 . Moreover, an efficient TS system is necessary to measure low-density plasmas in the region of less than 10 19 m −3 , such as the GAMMA 10 plasma and the peripheral plasma of high-density fusion plasmas. To obtain a TS signal with a good signal-to-noise ratio, we developed an optical-collection system with a large solid angle. In this paper, we describe the newly installed YAG TS system and the first results of electron temperature and density measurements in the tandem mirror GAMMA 10. The YAG TS system is constructed with laser, incident optics, light-collection optics, signal-detection electronics, and a data-recording system. A 10-Hz Nd:YAG laser (Continuum, Powerlite 9010) with an energy per pulse of 2 J, a pulse width of about 10 ns, and operating at a fund...