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The snowflake (SF) magnetic configuration is investigated as a potential power exhaust solution for a fusion reactor, but also to improve our understanding of divertor physics in general. Unlike a conventional single null (SN), it features an additional nearby x-point, which deeply modifies the magnetic field in the scrape-off layer (SOL) and can thereby affect parallel and cross-field transport of heat and particles. This paper investigates the power exhaust properties of the snowflake minus (SF-) configuration on the TCV tokamak, for Ohmically heated, L-mode, low-density, attached plasmas for a range of x-point separations, magnetic field directions and locations of the secondary x-point (low-field-side (LFS) or high-field-side (HFS)). Due to the relatively large x-point separation in physical space, this study probes x-point transport features in general, rather than reactor relevant aspects of the SF configuration. The target heat fluxes at all strike points are simultaneously monitored with an infrared (IR) thermography system and the kinetic profiles of the SOL at the outer mid-plane with a reciprocating probe (RCP). The placement of the additional x-point is seen to affect the inner-outer divertor power balance. An effective heat flux width lambda(eff)(q,u) for the SOL in the low poloidal field region is inferred from the measured power repartition between the two SOL manifolds created by the secondary x-point. For the HFS SF- configuration (secondary null in the LFS SOL), the lambda(eff)(q,u) is two times larger than that measured by the RCP at the outer mid-plane and by IR at the outer target of a comparable SN, while the outer mid-plane SOL profiles are similar to the SN. This is interpreted as the effect of increased effective cross-field diffusivity chi(null)(perpendicular to) in the intra-null region relative to the rest of the SOL. For the HFS SF-configuration (secondary null in the HFS SOL), no such increased transport is observed. The pressure-driven plasma convection expected near the primary null cannot explain the increased chi(null)(perpendicular to), which is instead consistent with interchange ballooning-like turbulence enhanced by the low poloidal field.
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limited'' configuration, where the main plasma touches the reactor wall, and the contact point defines the Last Closed Flux Surface (LCFS). In this thesis, we advance the understanding of SOL physics in limited plasmas, combining experiments and numerical simulations. In particular, two topics are addressed. First, the separation between the
near'' and ``far'' SOL is investigated. The near SOL extends typically a few mm from the LCFS, features steep radial profiles of parallel heat flux and is responsible for the peak of heat deposition on the tokamak first wall. The far SOL, typically a few cm wide, features flatter heat flux profiles, and accounts for the majority of the heat deposited on the first wall. Secondly, blob dynamics is investigated. Blobs are high density plasma filaments generated by turbulence, and are an ubiquitous feature of plasmas in open magnetic field lines. The blobs travel outwards to the reactor walls, increasing the cross field transport. Dedicated experiments have been performed on the TCV tokamak. Inboard-limited Deuterium (D) and Helium (He) plasma discharges are performed, varying the main plasma parameters (current, density and shaping). The parallel heat flux radial profiles are determined with infrared thermography. For the first time, the presence of a near SOL in TCV limited plasmas is reported, both for D and He discharges. The near SOL is found to disappear for high plasma resistivity. Non-ambipolar currents are measured to flow to the wall in the near SOL using Langmuir probes, and their presence is found to correlate with the strength of the near SOL heat fluxes. A simple interpretation is given. The heat fluxes and electric potentials are also measured on the low field side using a reciprocating Langmuir probe, and compared with the ones measured on the tokamak wall. A method for the mitigation and suppression of the near SOL heat fluxes through impurity seeding is proposed, and first experimental evidences are presented. The experiments are compared with numerical simulations of the TCV SOL, performed with the GBS code. The simulated parallel heat flux profiles qualitatively agree with the experimental ones, showing the presence of a near and far SOL. Also, non-ambipolar currents are observed to flow to the wall. The effect of resistivity is investigated through a second simulation with a 40 times higher resistivity. The blob dynamics in TCV is investigated using a conditional average sampling technique on the reciprocating Langmuir probe data. The results for two discharges, for low and high resistivity respectively, are discussed. A blob detection and tracking algorithm is applied to the numerical simulation outputs, and the results are discussed.Basil Duval, Benoît Labit, Roberto Maurizio, Holger Reimerdes, Umar Sheikh, Christian Gabriel Theiler, Cedric Kar-Wai Tsui