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Impact of nitrogen seeding on detachment and Scrape-off Layer properties in type-I ELMy H-mode TCV plasmas

ORAL

Abstract

Seeded impurities are essential to achieve divertor detachment, thereby mitigating the Scrape-off Layer (SOL) heat and particle exhaust in tokamak devices. Nonetheless, knowledge of their effect on SOL transport mechanisms is currently limited, complicating extrapolation to next step fusion reactors. To this end, a dataset of N2-seeded type-I ELMy H-mode TCV plasmas in either low density, high input power (low collisionality, -ν*) or medium-high density, lower power (high-ν*) regimes has been assembled and is presented in this work. The D2 gas fuelling and N2 injection rates have been varied independently to disentangle their effects on SOL profiles. Both scenarios have been successfully detached with N2 seeding, albeit only in between ELMs. A sustained higher core radiation and an increase in effective ion charge Zeff in the confined region suggest core impurity accumulation during and after N2 injection. At high-ν*, seeding N2 at zero D2 rate does not yield any clear change in either the near SOL density gradient lengths and far SOL shoulder amplitude, or on the edge electron temperature profile. At low-ν*, increasing the D2 gas rate without seeding results in a progressive flattening of the SOL density profile. On the other hand, it is observed that seeding N2 at low-ν* has a more pronounced effect compared to high-ν*, leading to cooling of the edge pedestal and overall steepening of the density profile, in terms of a decrease in the near SOL decay length and a distinct reduction in the far SOL shoulder.

Publication: I am planning to write a paper that includes the materials within this conference contributions. The timeline of this paper is still under decision.

Presenters

  • Adriano Stagni

    Consorzio RFX, Corso Stati Uniti 4, Padova, Italy, Consorzio RFX

Authors

  • Adriano Stagni

    Consorzio RFX, Corso Stati Uniti 4, Padova, Italy, Consorzio RFX

  • Nicola Vianello

    Consorzio RFX, Corso Stati Uniti 4, Padova, Italy

  • Holger Reimerdes

    EPFL - Swiss Plasma Center (SPC), EPFL Swiss Plasma Center, École Polytechnique Fédérale de Lausanne

  • Martim Zurita

    EPFL Swiss Plasma Center, EPFL - Swiss Plasma Center (SPC), Ecole Polytechnique Federale de Lausanne

  • Benoit Labit

    École Polytechnique Fédérale de Lausanne, Swiss Plasma Center, CH-1015 Lausanne, Switzerland, EPFL Swiss Plasma Center, École Polytechnique Fédérale de Lausanne

  • Matteo Agostini

    Consorzio RFX / CNR - ISTP Padova

  • Garance Durr-Legoupil-Nicoud

    EPFL - Swiss Plasma Center (SPC), EPFL Swiss Plasma Center, École Polytechnique Fédérale de Lausanne

  • Ondrej Grover

    Max-Planck-Institute for Plasmaphysics

  • Miriam La Matina

    Consorzio RFX / CRF - Centro Ricerche Fusione, Padova, Italy

  • Riccardo I Morgan

    EPFL Swiss Plasma Center, EPFL - Swiss Plasma Center (SPC), EPFL-SPC

  • Artur Perek

    EPFL Swiss Plasma Center, EPFL - Swiss Plasma Center (SPC), École Polytechnique Fédérale de Lausanne

  • Davide Silvagni

    Max-Planck-Institut für Plasmaphysik

  • Margherita Ugoletti

    Consorzio RFX, Corso Stati Uniti 4, Padova, Italy

  • Yinghan Wang

    EPFL Swiss Plasma Center, École Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC), EPFL - Swiss Plasma Center (SPC)

  • Matthias Bernert

    Max Planck Institute for Plasma Physics

  • Nicolas Fedorczak

    CEA, IRFM

  • Olivier Fevrier

    Swiss Plasma Center, EPFL, Lausanne, EPFL Swiss Plasma Center, EPFL - Swiss Plasma Center (SPC), École Polytechnique Fédérale de Lausanne

  • Stuart S Henderson

    United Kingdom Atomic Energy Authority, UKAEA

  • Christian Theiler

    EPFL Swiss Plasma Center, École Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC), EPFL - Swiss Plasma Center (SPC), EPFL Swiss Plasma Center (SPC)