000834319 001__ 834319 000834319 005__ 20240711114045.0 000834319 0247_ $$2doi$$a10.1088/1741-4326/aa69dd 000834319 0247_ $$2ISSN$$a0029-5515 000834319 0247_ $$2ISSN$$a1741-4326 000834319 0247_ $$2Handle$$a2128/14737 000834319 0247_ $$2WOS$$aWOS:000425870200002 000834319 0247_ $$2altmetric$$aaltmetric:19614984 000834319 037__ $$aFZJ-2017-04298 000834319 082__ $$a530 000834319 1001_ $$0P:(DE-Juel1)5247$$aWiesen, S.$$b0$$eCorresponding author$$ufzj 000834319 245__ $$aImpact of the JET ITER-like wall on H-mode plasma fueling 000834319 260__ $$aVienna$$bIAEA$$c2017 000834319 3367_ $$2DRIVER$$aarticle 000834319 3367_ $$2DataCite$$aOutput Types/Journal article 000834319 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1498464940_10865 000834319 3367_ $$2BibTeX$$aARTICLE 000834319 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000834319 3367_ $$00$$2EndNote$$aJournal Article 000834319 520__ $$aJET ITER-like wall (ILW) experiments show that the edge density evolution is strongly linked with the poloidal distribution of the ionization source. The fueling profile in the JET-ILW is more delocalized as compared to JET-C (JET with carbon-based plasma-facing components PFCs). Compared to JET-C the H-mode pedestal fueling cycle is dynamically influenced by a combination of plasma–wall interaction features, in particular: (1) edge-localized modes (ELMs) induced energetic particles are kinetically reflected on W divertor PFCs leading to distributed refueling away from the divertor depending on the divertor plasma configuration, (2) delayed molecular re-emission and outgassing of particles being trapped in W PFCs (bulk-W at the high field side and W-coated CFCs at the low field side) with different fuel content and (3) outgassing from Be co-deposits located on top of the high-field side baffle region shortly after the ELM. In view of the results of a set of well diagnosed series of JET-ILW type-I ELMy H-mode discharges with good statistics, the aforementioned effects are discussed in view of H-mode pedestal fueling capacity. The ongoing modelling activities with the focus on coupled core-edge plasma simulations and plasma–wall interaction are described and discussed also in view of possible code improvements required. 000834319 536__ $$0G:(DE-HGF)POF3-174$$a174 - Plasma-Wall-Interaction (POF3-174)$$cPOF3-174$$fPOF III$$x0 000834319 588__ $$aDataset connected to CrossRef 000834319 7001_ $$0P:(DE-Juel1)129976$$aBrezinsek, S.$$b1$$ufzj 000834319 7001_ $$0P:(DE-HGF)0$$aWischmeier, M.$$b2 000834319 7001_ $$0P:(DE-HGF)0$$aDe la Luna, E.$$b3 000834319 7001_ $$0P:(DE-Juel1)171218$$aGroth, M.$$b4$$ufzj 000834319 7001_ $$0P:(DE-HGF)0$$aJaervinen, A. E.$$b5 000834319 7001_ $$0P:(DE-HGF)0$$ade la Cal, E.$$b6 000834319 7001_ $$0P:(DE-HGF)0$$aLosada, U.$$b7 000834319 7001_ $$0P:(DE-HGF)0$$ade Aguilera, A. 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