Ongena, J.Suttrop, W.Becoulet, M.Cordey, G.Dumortier, P.Eich, T.Ingesson, L. C.Jachmich, S.Lang, P.Loarte, A.Lomas, P.Maddison, G. P.Messiaen, A.Nave, M. F. F.Rapp, J.Saibene, G.Sartori, R.Sauter, O.Strachan, J. D.Unterberg, B.Valovic, M.Alper, B.Andrew, P.Baranov, Y.Brzozowski, J.Bucalossi, J.Brix, M.Budny, R.Charlet, M.Coffey, I.De Baar, M.De Vries, P.Gowers, C.Hawkes, N.von Hellermann, M.Hillis, D. L.Hogan, J.Jackson, G. L.Joffrin, E.Jupen, C.Kallenbach, A.Koslowski, H. R.Lawson, K. D.Mantsinen, M.Matthews, G.Monier-Garbet, P.McDonald, D.Milani, F.Murakami, M.Murari, A.Neu, R.Parail, V.Podda, S.Puiatti, M. E.Righi, E.Sartori, F.Sarazin, Y.Staebler, A.Stamp, M.Telesca, G.Valisa, M.Weyssow, B.Zastrow, K. D.2008-04-162008-04-162008-04-16200110.1088/0741-3335/43/12A/302https://infoscience.epfl.ch/handle/20.500.14299/21722WOS:000173342000004758Recent progress towards obtaining high density and high confinement in JET as required for the ITER reference scenario at Q = 10 is summarized. Plasmas with simultaneous confinement H-98(y.2) = 1 and densities up to n/n(Gw) similar to 1 are now routinely obtained. This has been possible (i) by using plasmas at high (delta similar to 0.5) and medium (delta similar to 0.3-0.4) triangularity with sufficient heating power to maintain Type I ELMs, (ii) with impurity seeded plasmas at high (delta similar to 0.5) and low (delta less than or equal to 0.2) triangularity, (iii) with an optimized pellet injection sequence, maintaining the energy confinement and raising the density, and (iv) by carefully tuning the gas puff rate leading to plasmas with peaked density profiles and good confinement at long time scales. These high performance discharges exhibit Type I ELMs, with a new and more favourable behaviour observed at high densities, requiring further studies. Techniques for a possible mitigation of these ELMs are discussed, and first promising results are obtained with impurity seeding in discharges at high triangularity. Scaling studies using the new data of this year show a strong dependence of confinement on upper triangularity, density and proximity to the Greenwald limit. Observed MHD instabilities and methods to avoid these in high density and high confinement plasmas are discussed.JETITERtext::journal::journal article::research article