TJ-II:Internal Transport Barriers: Difference between revisions
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The influence of magnetic topology on the formation of electron internal transport barriers (e-ITBs) has been studied experimentally in electron cyclotron heated plasmas in the stellarator [[TJ-II]]. e-ITB formation is characterized by an increase in core electron temperature and plasma potential. The positive radial electric field increases by a factor of 3 in the central plasma region when an e-ITB forms. | The influence of magnetic topology on the formation of electron internal transport barriers (e-ITBs) has been studied experimentally in electron cyclotron heated plasmas in the stellarator [[TJ-II]]. e-ITB formation is characterized by an increase in core electron temperature and plasma potential. The positive radial electric field increases by a factor of 3 in the central plasma region when an e-ITB forms. Experiments demonstrate that the formation of an e-ITB depends on the magnetic configuration. Calculations of the modification of the rotational transform due to plasma current lead to the interpretation that the formation of an e-ITB can be triggered by positioning a low order rational surface close to the plasma core region. | ||
<ref>[http://dx.doi.org/10.1088/0741-3335/46/1/017 T. Estrada et al, Plasma Phys. Control. Fusion '''46''' (2004) 277-286]</ref> | <ref>[http://dx.doi.org/10.1088/0741-3335/46/1/017 T. Estrada et al, Plasma Phys. Control. Fusion '''46''' (2004) 277-286]</ref> | ||
== References == | == References == | ||
<references /> | <references /> | ||
Revision as of 21:07, 7 August 2009
The influence of magnetic topology on the formation of electron internal transport barriers (e-ITBs) has been studied experimentally in electron cyclotron heated plasmas in the stellarator TJ-II. e-ITB formation is characterized by an increase in core electron temperature and plasma potential. The positive radial electric field increases by a factor of 3 in the central plasma region when an e-ITB forms. Experiments demonstrate that the formation of an e-ITB depends on the magnetic configuration. Calculations of the modification of the rotational transform due to plasma current lead to the interpretation that the formation of an e-ITB can be triggered by positioning a low order rational surface close to the plasma core region. [1]