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安装在韩国超导托卡马克先进研究装置(KSTAR)上的新型单晶色散干涉仪及其首次测量。

The new single crystal dispersion interferometer installed on KSTAR and its first measurement.

作者信息

Lee Dong-Geun, Lee K C, Juhn J-W, Lee Jae-Seok, Ghim Y-C

机构信息

Department of Nuclear and Quantum Engineering, Korea Advanced Institute of Science and Technology, Daejeon 34141, Republic of Korea.

Korea Institute of Fusion Energy, Daejeon 34133, Republic of Korea.

出版信息

Rev Sci Instrum. 2021 Mar 1;92(3):033536. doi: 10.1063/5.0043629.

Abstract

Dispersion interferometers have been used to measure line integrated electron densities from many fusion devices. To optically suppress noise due to mechanical vibrations, a conventional dispersion interferometer typically uses two nonlinear crystals located before and after the plasma along the laser beam path. Due to the long beam path, it can be difficult to overlap the fundamental and second harmonic laser beams for a heterodyne dispersion interferometer and to focus the beams on the second nonlinear crystal located after the plasma, especially when the aperture of the nonlinear crystal is small, i.e., of the order of mm. To overcome such difficulties, a new concept of a heterodyne dispersion interferometer, a single crystal dispersion interferometer (SCDI), is developed and installed on KSTAR with the laser wavelength of 1064 nm. The concept and the optical setup of the KSTAR SCDI are discussed, as well as its first measurement during a shattered pellet injection that produces abrupt and large changes in the electron density. To demonstrate feasibility, the KSTAR SCDI measurements are also compared with those from the existing two-color interferometer.

摘要

色散干涉仪已被用于测量许多聚变装置中的线积分电子密度。为了光学抑制由机械振动引起的噪声,传统的色散干涉仪通常沿着激光束路径在等离子体之前和之后使用两块非线性晶体。由于光束路径较长,对于外差色散干涉仪来说,很难使基频激光束和二次谐波激光束重叠,并且难以将光束聚焦在等离子体之后的第二块非线性晶体上,尤其是当非线性晶体的孔径很小时,即毫米量级。为了克服这些困难,一种外差色散干涉仪的新概念——单晶色散干涉仪(SCDI)被开发出来,并安装在激光波长为1064 nm的韩国超导托卡马克先进研究装置(KSTAR)上。讨论了KSTAR SCDI的概念和光学设置,以及在破碎弹丸注入期间的首次测量,破碎弹丸注入会使电子密度产生突然且大幅的变化。为了证明可行性,还将KSTAR SCDI的测量结果与现有的双色干涉仪的测量结果进行了比较。

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