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L-H transition physics in hydrogen and deuterium: key role of the edge radial electric field and ion heat flux

MPS-Authors
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Ryter,  F.
Tokamak Scenario Development (E1), Max Planck Institute for Plasma Physics, Max Planck Society;

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Cavedon,  M.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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Happel,  T.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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McDermott,  R. M.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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Viezzer,  E.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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Conway,  G. D.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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Fischer,  R.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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Kurzan,  B.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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Pütterich,  T.
Plasma Edge and Wall (E2M), Max Planck Institute for Plasma Physics, Max Planck Society;

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Tardini,  G.
Tokamak Scenario Development (E1), Max Planck Institute for Plasma Physics, Max Planck Society;

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Willensdorfer,  M.
Tokamak Scenario Development (E1), Max Planck Institute for Plasma Physics, Max Planck Society;

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Citation

Ryter, F., Cavedon, M., Happel, T., McDermott, R. M., Viezzer, E., Conway, G. D., et al. (2016). L-H transition physics in hydrogen and deuterium: key role of the edge radial electric field and ion heat flux. Plasma Physics and Controlled Fusion, 58: 014007. doi:10.1088/0741-3335/58/1/014007.


Cite as: https://hdl.handle.net/11858/00-001M-0000-0028-FE02-2
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