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The mechanism behind this phenomenological limit is not understood, but probably associated with edge gradient limits. | The mechanism behind this phenomenological limit is not understood, but probably associated with edge gradient limits. | ||
Recently, an explanation based on the formation of magnetic island was proposed. <ref>[[doi:10.1103/PhysRevLett.108.165004|D.A. Gates and L. Delgado-Aparicio, ''Origin of Tokamak Density Limit Scalings'', Phys. Rev. Lett. '''108''' (2012) 165004]]</ref> | Recently, an explanation based on the formation of magnetic island was proposed. <ref>[[doi:10.1103/PhysRevLett.108.165004|D.A. Gates and L. Delgado-Aparicio, ''Origin of Tokamak Density Limit Scalings'', Phys. Rev. Lett. '''108''' (2012) 165004]]</ref> | ||
== See also == | |||
* High density limit in [[Reversed Field Pinch]]es. <ref>[[doi:10.1063/1.3063060|M.E. Puiatti, P. Scarin, G. Spizzo, et al., ''High density limit in reversed field pinches'', Phys. Plasmas '''16''' (2009) 012505]]</ref> | |||
== References == | == References == | ||
<references /> | <references /> |