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dc.contributor.authorOsborne, T.
dc.contributor.authorRyter, F.
dc.contributor.authorAustin, M.
dc.contributor.authorBarrera Orte, L.
dc.contributor.authorChurchill, R. M.
dc.contributor.authorCziegler, I.
dc.contributor.authorFenstermacher, M.
dc.contributor.authorFischer, R.
dc.contributor.authorGerhardt, S.
dc.contributor.authorGroebner, R.
dc.contributor.authorGohil, P.
dc.contributor.authorHappel, T.
dc.contributor.authorLoarte, A.
dc.contributor.authorMaingi, R.
dc.contributor.authorManz, P.
dc.contributor.authorMcDermott, R. M.
dc.contributor.authorMcKee, G.
dc.contributor.authorRhodes, T. L.
dc.contributor.authorSchmitz, L.
dc.contributor.authorTheiler, C.
dc.contributor.authorViezzer, E.
dc.contributor.authorWalk, J. R.
dc.contributor.authorWolfrum, E.
dc.contributor.authorYan, Z.
dc.contributor.authorHubbard, Amanda E
dc.contributor.authorHughes Jr, Jerry
dc.contributor.authorMarinoni, Alessandro
dc.contributor.authorMarmar, Earl S
dc.contributor.authorRice, John E
dc.contributor.authorWalk Jr, John R
dc.contributor.authorWhyte, Dennis G
dc.contributor.authorWolfe, Stephen M
dc.date.accessioned2017-05-09T13:43:23Z
dc.date.available2017-05-09T13:43:23Z
dc.date.issued2016-07
dc.date.submitted2016-05
dc.identifier.issn0029-5515
dc.identifier.issn1741-4326
dc.identifier.urihttp://hdl.handle.net/1721.1/108763
dc.description.abstractThis paper describes joint ITPA studies of the I-mode regime, which features an edge thermal barrier together with L-mode-like particle and impurity transport and no edge localized modes (ELMs). The regime has been demonstrated on the Alcator C-Mod, ASDEX Upgrade and DIII-D tokamaks, over a wide range of device parameters and pedestal conditions. Dimensionless parameters at the pedestal show overlap across devices and extend to low collisionality. When they are matched, pedestal temperature profiles are also similar. Pedestals are stable to peeling–ballooning modes, consistent with lack of ELMs. Access to I-mode is independent of heating method (neutral beam injection, ion cyclotron and/or electron cyclotron resonance heating). Normalized energy confinement H 98,y2  ≥  1 has been achieved for a range of 3  ≤  q 95  ≤  4.9 and scales favourably with power. Changes in turbulence in the pedestal region accompany the transition from L-mode to I-mode. The L–I threshold increases with plasma density and current, and with device size, but has a weak dependence on toroidal magnetic field B T. The upper limit of power for I-modes, which is set by I–H transitions, increases with B T and the power range is largest on Alcator C-Mod at B  >  5 T. Issues for extrapolation to ITER and other future fusion devices are discussed.en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-FC02-99ER54512-CMOD)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-SC0012469)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-FC02-04ER54698)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-FG02-94ER54235)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-AC52-07NA27344)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-AC02-09CH11466)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-FG02-89ER53296)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-FG02-08ER54999)en_US
dc.description.sponsorshipUnited States. Department of Energy (DE-FG02-08ER54984)en_US
dc.language.isoen_US
dc.publisherIOP Publishingen_US
dc.relation.isversionofhttp://dx.doi.org/10.1088/0029-5515/56/8/086003en_US
dc.rightsCreative Commons Attribution-Noncommercial-Share Alikeen_US
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/4.0/en_US
dc.sourceProf. Whyte via Chris Sherratten_US
dc.titleMulti-device studies of pedestal physics and confinement in the I-mode regimeen_US
dc.typeArticleen_US
dc.identifier.citationHubbard, A.E.; Osborne, T.; Ryter, F.; Austin, M.; Barrera Orte, L.; Churchill, R.M. and Cziegler, I. et al. “Multi-Device Studies of Pedestal Physics and Confinement in the I-Mode Regime.” Nuclear Fusion 56, no. 8 (July 2016): 086003.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Centeren_US
dc.contributor.approverWhyte, Dennisen_US
dc.contributor.mitauthorHubbard, Amanda E
dc.contributor.mitauthorHughes Jr, Jerry
dc.contributor.mitauthorMarinoni, Alessandro
dc.contributor.mitauthorMarmar, Earl S
dc.contributor.mitauthorRice, John E
dc.contributor.mitauthorWalk Jr, John R
dc.contributor.mitauthorWhyte, Dennis G
dc.contributor.mitauthorWolfe, Stephen M
dc.relation.journalNuclear Fusionen_US
dc.eprint.versionAuthor's final manuscripten_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dspace.orderedauthorsHubbard, A.E.; Osborne, T.; Ryter, F.; Austin, M.; Barrera Orte, L.; Churchill, R.M.; Cziegler, I.; Fenstermacher, M.; Fischer, R.; Gerhardt, S.; Groebner, R.; Gohil, P.; Happel, T.; Hughes, J.W.; Loarte, A.; Maingi, R.; Manz, P.; Marinoni, A.; Marmar, E.S.; McDermott, R.M.; McKee, G.; Rhodes, T.L.; Rice, J.E.; Schmitz, L.; Theiler, C.; Viezzer, E.; Walk, J.R.; White, A.; Whyte, D.; Wolfe, S.; Wolfrum, E.; Yan, Z.en_US
dspace.embargo.termsNen_US
dc.identifier.orcidhttps://orcid.org/0000-0003-1004-5782
dc.identifier.orcidhttps://orcid.org/0000-0002-5283-0546
dc.identifier.orcidhttps://orcid.org/0000-0001-8319-5971
dc.identifier.orcidhttps://orcid.org/0000-0001-8324-4227
dc.identifier.orcidhttps://orcid.org/0000-0002-9001-5606
mit.licenseOPEN_ACCESS_POLICYen_US
mit.metadata.statusComplete


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