The JET 2019-2020 scientific and technological programme exploited the results of years of concerted scientific and engineering work, including the ITER-like wall (ILW: Be wall and W divertor) installed in 2010, improved diagnostic capabilities now fully available, a major Neutral Beam Injection (NBI) upgrade providing record power in 2019-2020, and tested the technical & procedural preparation for safe operation with tritium. Research along three complementary axes yielded a wealth of new results. Firstly, the JET plasma programme delivered scenarios suitable for high fusion power and alpha particle physics in the coming D-T campaign (DTE2), with record sustained neutron rates, as well as plasmas for clarifying the impact of isotope mass on plasma core, edge and plasma-wall interactions, and for ITER pre-fusion power operation. The efficacy of the newly installed Shattered Pellet Injector for mitigating disruption forces and runaway electrons was demonstrated. Secondly, research on the consequences of long-term exposure to JET-ILW plasma was completed, with emphasis on wall damage and fuel retention, and with analyses of wall materials and dust particles that will help validate assumptions and codes for design & operation of ITER and DEMO. Thirdly, the nuclear technology programme aiming to deliver maximum technological return from operations in D, T and D-T benefited from the highest D-D neutron yield in years, securing results for validating radiation transport and activation codes, and nuclear data for ITER.

This paper builds on earlier work to give a consistent treatment of the positive column of discharges in electronegative gases covering the transition from collisionless to collisional. In particular it seeks to elucidate the conditions under which there is an ion-ion plasma core surrounded by an electron-ion plasma, and when there is not. The parameters which describe the processes of ionization, attachment, detachment and recombination are related to the central negative ion density relative to the electron density and, where appropriate, the size of the core. The use, by earlier workers, of the Boltzmann approximation to describe the negative ion distribution and to obtain ambipolar diffusion coefficients at higher pressures is shown not to be justified. This leads to the clarification of an inconsistency in the literature. Where possible, the work is related to other recent treatments of the same problem in order to begin to build a comprehensive picture of such discharges. The need to have results which combine both detachment and recombination as the negative ion loss processes is identified as outstanding. This, when rectified, should lead to a fully comprehensive treatment.

Alpha particles with energies on the order of megaelectronvolts will be the main source of plasma heating in future magnetic confinement fusion reactors. Instead of heating fuel ions, most of the energy of alpha particles is transferred to electrons in the plasma. Furthermore, alpha particles can also excite Alfvénic instabilities, which were previously considered to be detrimental to the performance of the fusion device. Here we report improved thermal ion confinement in the presence of megaelectronvolts ions and strong fast ion-driven Alfvénic instabilities in recent experiments on the Joint European Torus. Detailed transport analysis of these experiments reveals turbulence suppression through a complex multi-scale mechanism that generates large-scale zonal flows. This holds promise for more economical operation of fusion reactors with dominant alpha particle heating and ultimately cheaper fusion electricity.

Models the positive column in strongly electronegative gases, where recombination is the dominant mechanism of charge loss in the volume. The pressure range is taken to be such that mobility governs particle motion. It is related to earlier work in gases like oxygen, where detachment is the dominant loss mechanism and there are many similarities with the case where the attachment/ionization rate ratio P was <1, treated by Daniels, Franklin and Snell (1990). It is shown that P is necessarily less than unity and that it is not physically possible to have a discharge where electron-ion recombination is the only loss mechanism. The structure found is that of a central positive ion-negative ion core surrounded by a conventional electron-positive ion plasma with a sharp transition region of fractional thickness given by the parameter l1/2 where l is a normalized ratio of ion recombination rate beta i and ionization rate nu i given by beta ine0/ nu i where ne0 is the central electron density. Expressions are found for the ion plasma dimensions and the eigenvalue lambda , which relates the ionization rate, discharge radius, ion mobility and electron temperature, and comparison is made with the work of Volynets et al. (1993). The physical characteristics of such discharges are explained by the treatment given for the first time since the problem was formulated in 1949.