Effect of Yacora evaluated molecular rates on SOLPS-ITERsimulations
ORAL
Abstract
The production of D2+ results in plasma-molecular interactions such as MAR and MAD
[1, 2, 3]. MAR results in recombination of D+ which lowers the ion target flux and MAD is a
means of molecular dissociation; These reactions form excited D which result in radiative
losses, ultimately lowering the plasma temperature [1, 3]. After detachment onset, the plasma
temperature near the target drops to low levels where electron impact ionisation of D2 begins
to reduce. In these conditions molecular charge exchange becomes the main source of D2+ [2].
SOLPS-ITER does not replicate the levels of MAR, and MAD seen experimentally on MAST
Upgrade and TCV [1, 3]. This originates from the AMJUEL molecular effective charge
exchange rate coefficient. Which contains inaccuracies below 2 eV [4, 5, 6, 7].
A molecular rate coefficient dataset has been calculated as input for EIRENE based on the
vibrationally-resolved Yacora ground state model (Yacora-H2(X1, v)) which uses the Yacora
ODE solver [8, 9]. This dataset was applied to an isolated divertor leg geometry in
SOLPS-ITER with MAST Upgrade L-mode Super-X conditions and compared to an AMJUEL
reference [10]. Below Te = 1 eV , the novel molecular charge exchange effective rate coefficient
increases the levels of D2+. In the highest density case, MAR and MAD increases by a factor of
∼ 4 and ∼ 2 respectively. This results in stronger ion target flux roll-over, and larger power
dissipation during detachment that are qualitatively in better agreement with trends on
MAST Upgrade and TCV [1, 3].
[1, 2, 3]. MAR results in recombination of D+ which lowers the ion target flux and MAD is a
means of molecular dissociation; These reactions form excited D which result in radiative
losses, ultimately lowering the plasma temperature [1, 3]. After detachment onset, the plasma
temperature near the target drops to low levels where electron impact ionisation of D2 begins
to reduce. In these conditions molecular charge exchange becomes the main source of D2+ [2].
SOLPS-ITER does not replicate the levels of MAR, and MAD seen experimentally on MAST
Upgrade and TCV [1, 3]. This originates from the AMJUEL molecular effective charge
exchange rate coefficient. Which contains inaccuracies below 2 eV [4, 5, 6, 7].
A molecular rate coefficient dataset has been calculated as input for EIRENE based on the
vibrationally-resolved Yacora ground state model (Yacora-H2(X1, v)) which uses the Yacora
ODE solver [8, 9]. This dataset was applied to an isolated divertor leg geometry in
SOLPS-ITER with MAST Upgrade L-mode Super-X conditions and compared to an AMJUEL
reference [10]. Below Te = 1 eV , the novel molecular charge exchange effective rate coefficient
increases the levels of D2+. In the highest density case, MAR and MAD increases by a factor of
∼ 4 and ∼ 2 respectively. This results in stronger ion target flux roll-over, and larger power
dissipation during detachment that are qualitatively in better agreement with trends on
MAST Upgrade and TCV [1, 3].
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Publication: Planned submission of this work as a paper prior to the conference under the title
"Impact of Yacora evaluated molecular rates on detached
SOLPS-ITER simulations".
Presenters
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Joseph E Bryant
University of Liverpool
Authors
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Joseph E Bryant
University of Liverpool
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Kirsty McKay
University of Liverpool
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James R Harrison
UK Atomic Energy Authority (UKAEA)
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David Moulton
UK Atomic Energy Authority (UKAEA)
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Kevin Verhaegh
United Kingdom Atomic Energy Agency, UK Atomic Energy Authority (UKAEA)
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Cyd Cowley
University of York
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Richard C Bergmayr
Max Planck Institute for Plasma Physics
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Ursel E Fantz
Max Planck Institute for Plasma Physics
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Dirk Wünderlich
Max Planck Institute for Plasma Physics