17–22 May 2026
marinaforum REGENSBURG
Europe/Berlin timezone

I10 Overview of Divertor and SOL Physics Results Following the Installation of the Tungsten Divertor in KSTAR

19 May 2026, 13:50
30m
Invited G. Power Exhaust, Plasma Detachment and Heat Load Control Invited Talk

Speaker

Hyungho Lee (KFE)

Description

Since the installation of the actively cooled lower tungsten (W) divertor in 2023, KSTAR has conducted four experimental campaigns (>7,200 discharges; avg. 6.5–7 MW, ~10 s) addressing critical plasma-surface interactions and optimizing divertor performance. Previously, KSTAR operated with carbon wall for 15 years (~32,800 discharges). This overview synthesizes key physics and engineering results from the campaigns with the W divertor
Initial experiments confirmed that W impurities transported into the core plasma significantly degrade performance, with 2D radiation profiles measured by Infra-Red Video Bolometer (IRVB) revealing a distinct outboard-localized radiation power loss. To rigorously investigate these phenomena, diagnostic capabilities were significantly enhanced, including the development of W-flux monitors and real-time IRVB systems. Additionally, impurity transport codes were utilized to derive W concentration profiles by analyzing 2D radiation, Vacuum Ultraviolet Spectroscopy, and Compact Advanced EUV Spectrometer (CAES) measurements.
A novel “β-kicking” NBI heating scenario was developed. By optimizing NBI power injection immediately after the H-mode transition, this scenario mitigated impurity accumulation and restored plasma performance to levels comparable to the carbon-divertor phase.
Divertor detachment control was extensively explored using neon (Ne) and nitrogen (N) injection. While N injection effectively controlled the ion saturation current measured by Langmuir Probes (LPs) at the striking point on the outer divertor target, high injection rates led to increased W concentration in the core plasma. This trade-off highlights the necessity of optimizing N gas injection rates. Advanced real-time control systems were also deployed, including a feedback algorithm utilizing real-time 2D IRVB data and a UEDGE-based surrogate model. Furthermore, a novel Machine Learning-based virtual diagnostic system, trained on Absolute Extreme Ultraviolet, LPs, and historical IRVB data, demonstrated the capability to predict 2D radiation profiles and control the radiation front without direct real-time IRVB input.
Wall conditioning strategies have evolved to support high-performance operations. Impurity Powder Dropper (IPD) boronization provided a quantitative assessment of W-source reduction at the divertor target. Notably, the IPD system is now integrated into the Plasma Control System, enabling feedback-controlled injection to optimize boronization specifically for long-pulse discharges. In preparation for the full-W wall transition after the 2026 campaign, these advanced conditioning techniques, along with improved ECWC scenarios, are being established as essential tools for ensuring successful plasma start-up and effective wall conditioning.
Finally, material challenges were identified. Localized melting of W monoblocks and structural issues, such as dislodgement of the W plate, occurred. These incidents and implications for future operations are discussed.

Author

Hyungho Lee (KFE)

Co-authors

Y.-C Ghim (KAIST) Junghoo Hwang (Korea Advanced Institute of Science and Technology) SangKyeun Kim (Princeton Plasma Physics Laboratory) David Eldon (General Atomics) Hanna Schamis (Princeton Plasma Physics Laboratory) Eric Gilson (Princeton Plasma Physics Laboratory) Dr Anchal Gupta (Blue Laser Fusion) Dr Cheolsik Byun (PPPL) Seungtae Oh (KFE) Eunnam Bang (Korea Insutitute of Fusion Energy) Juhyeok Jang (Korea Institute of Fusion Energy) Changmin Shin (KAIST) SOOHYUN SON (KFE) Dongcheol Seo (GNOI) Mr Yoonseong Han (KAIST) Junhyeok Yoon (KAIST) Koung Moon Kim (KFE) Jae-in Song (KFE) Suk-Ho Hong (General Atomics) Richard A. Pitts (ITER Organization, Route de Vinon-sur-Verdon, CS 90 046, 13067 St. Paul Lez Durance Cedex, France) Dr Soohyun Park (KFE) Dr Sungjin Kwon (KFE) Mr Sangwoo Kwag (KFE) Mr Hongtack Kim (KFE) Mr Yongbok Chang (KFE) Mr Nakhyung Song (KFE) Andrey Pshenov (ITER Organization, Route de Vinon-sur-Verdon, CS 90 046, 13067 St. Paul Lez Durance, Cedex, France) Kwangpyo Kim (KFE) Changrae Seon (KFE) Dr Hyungseok Kim (KFE) June-Woo Juhn (Korea Institute of Fusion Energy) Dr Wonik Jeong (KFE) Hoiyun Jeong (Korea Advanced Institute of Science & Technology) Mr Myungkyu Kim (KFE) Yegeon Lim (Caltech) Jun-gyo Bak (Korea Insutitute of Fusion Energy) Hung Su Kim (Korea Insutitute of Fusion Energy) Seungmin Bong (KAIST) KyuBeen Kwon (Oak Ridge Associated Universities) Sang-Hee Hahn (Korea Institute of Fusion Energy) Dr Giwook Shin (KFE) Valentina Alarcon (North Carolina State University) Florian Laggner (North Carolina State University) Mr Sangwon Yun (KFE) Soo-hwan Park (KFE) Hyunmyung Lee (KFE) Alessandro Bortolon (Princeton Plasma Physics National Laboratory) Alex Nagy (Princeton Plasma Physics Laboratory) Rajesh Maingi (Princeton Plasma Physics Laboratory) Dr Youngmu Jeon (KFE) Dr Hyunsun Han (KFE) Mr Youngok Kim (KFE) In-sik Woo (KFE) Chanyeong Lee (Korea Advanced Institute of Science and Technology) Wonho Choe (Korea Advanced Institute of Science and Technology) Prof. Yongseok Hwang (SNU)

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