Inter-ELM pedestal turbulence dynamics dependence on q95 and temperature gradient

• Published in: Nuclear fusion Vol. 64; no. 9; pp. 096001 - 96009
• Main Authors: Yan, Z., McKee, G.R., Xia, J., Jian, X., Groebner, R., Rhodes, T., Barada, K., Haskey, S., Chen, J., Banerjee, S., Laggner, F.
• Format: Journal Article
• Language: English
• Published: United States IOP Publishing 01.09.2024; IOP Science
• Subjects: DIII-D; H-mode; Inter-ELM turbulence; pedestal
• ISSN: 0029-5515; 1741-4326
• DOI: 10.1088/1741-4326/ad536a

Abstract A series of dedicated experiments from DIII-D tokamak provide spatially and temporally resolved measurements of electron density and temperature, and multiscale and multichannel fluctuations over a wide range of conditions. Measurements of long wavelength density fluctuations in the type-I ELMing H-mode pedestal routinely revealed a coexistence of multiple instabilities that exhibit dramatic different dynamic behaviors as q 95 and temperature gradient are varied, apparently responsible for limiting pedestal temperature profiles. Two distinct frequency bands of density fluctuations are modulated with ELM cycle with frequency above 200kHz propagating in the electron diamagnetic direction in the lab frame (electron mode) and below 200kHz propagating in the ion diamagnetic direction (ion mode). The electron mode amplitude peaks near the electron temperature gradient region and increases with q 95 which seems to be correlated with the increased χ e at higher q 95 , similar to the characteristics expected for Micro-tearing Mode (MTM). At higher q 95 , during the inter-ELM period, the ion mode decays at later phase of the ELM cycle. Consistently, the poloidal correlation length of the ion mode is also found to reduce which suggests the possible E×B flow shear suppression of ion mode at later phase of the ELM cycle as the E r well recovers. In contrast, the electron mode grows during the ELM cycle and reaches saturation at around 50-60% of ELM period. Linear gyrokinetic simulations find the MTMs as the most unstable mode in the pedestal electron temperature gradient region. The higher q 95 and lower magnetic shear destabilize MTMs. These observations provide key insights of the underlying physics of multifield properties and rich dataset of experimental ‘fingerprints’ that enable new tests of the theoretical pedestal models and lead to developing a predictive model for pedestal formation on ITER and future burning plasma experiments.