2019
DOI: 10.1088/1741-4326/ab1d7a
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Impact of impurity mixture gas seeded by supersonic molecular beam injection on edge-localized modes in the HL-2A tokamak

Abstract: Impurity seeding experiments in ELMy H-mode plasmas by using supersonic molecular beam injection (SMBI) have been performed in the HL-2A tokamak. Besides pure impurity gas (neon, argon), impurities mixed with the main ion fuelling gas by different ratios were seeded into the plasma. It has been observed that the ELM behavior and plasma confinement are very sensitive to the impurity ratio. For 30% Ne impurity seeding, large ELMs are replaced by high frequency bursts (HFBs), which have higher frequency and small… Show more

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Cited by 24 publications
(18 citation statements)
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“…The IM turbulence induced impurity ion influx is demonstrated to be higher for a higher τ i = T e /T i . Interestingly, these theoretical predictions are in coincidence with the evidence observed in argon injection experiment on HL-2A tokamak [39]. The experimental observation that a lower electron density gradient is favorable for sustainment of HDPs of impurity ions is verified in turn with simulation.…”
Section: Introductionsupporting
confidence: 81%
“…The IM turbulence induced impurity ion influx is demonstrated to be higher for a higher τ i = T e /T i . Interestingly, these theoretical predictions are in coincidence with the evidence observed in argon injection experiment on HL-2A tokamak [39]. The experimental observation that a lower electron density gradient is favorable for sustainment of HDPs of impurity ions is verified in turn with simulation.…”
Section: Introductionsupporting
confidence: 81%
“…The above simulation results are evidenced for the first time in an argon injection experiment [45,46]. Figure 15 presents the radial profile of the radiation intensity I rad (a), the temporal evolutions of R/L Ti and R/L Te (b), IM turbulence intensity S integrated over 40-90 kHz (c), and the normalized density gradient of argon ions R/L nz (d) and electrons R/L ne (e), and the fluctuation intensity S and γ/ω * e of IM versus R/L nz ( f ).…”
Section: Impurity Mode Induced Turbulent Particle Transportsupporting
confidence: 52%
“…The corresponding number of the injected particles is 8.3 × 10 18 . The impurity particles are mainly deposited at the edge plasma region [37]. The fueling effect on the plasma is negligible, as figure 5(b) shows that the SMBI does not obviously increase the plasma density.…”
Section: Response Of Elms and Pedestal To Smbi-seeded Neon Gas Impuritymentioning
confidence: 93%