Regime of very high confinement in the boronized DIII-D tokamak

  • G. L. Jackson
  • , J. Winter
  • , T. S. Taylor
  • , K. H. Burrell
  • , J. C. Deboo
  • , C. M. Greenfield
  • , R. J. Groebner
  • , T. Hodapp
  • , K. Holtrop
  • , E. A. Lazarus
  • , L. L. Lao
  • , S. I. Lippmann
  • , T. H. Osborne
  • , T. W. Petrie
  • , J. Phillips
  • , R. James
  • , D. P. Schissel
  • , E. J. Strait
  • , A. D. Turnbull
  • , W. P. West

Research output: Contribution to journalArticlepeer-review

198 Scopus citations

Abstract

Following boronization, tokamak discharges in DIII-D have been obtained with confinement times up to a factor of 3.5 above the ITER89-P L-mode scaling and 1.8 times greater than the DIII-D/JET H-mode scaling relation. Very high confinement phases are characterized by relatively high central density with ne(0)1×1020 m-3, and central ion temperatures up to 13.6 keV at moderate plasma currents (1.6 MA) and heating powers (12.515.3 MW). These discharges exhibit a low fraction of radiated power, P25%, Zeff(0) close to unity, and lower impurity influxes than comparable DIII-D discharges before boronization.

Original languageEnglish
Pages (from-to)3098-3101
Number of pages4
JournalPhysical Review Letters
Volume67
Issue number22
DOIs
StatePublished - 1991
Externally publishedYes

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