Neoclassical tearing mode seeding by Alfvén eigenmode coupling in MAST-U

Nuclear Fusion 66:12 (2026)

Authors:

K Thomas, L Bardoczi, K Gibson, J Ruiz Ruiz, M Dreval, D Ryan, K McClements, C Michael

Abstract:

We present evidence of tearing mode seeding by nonlinear three-wave coupling of Alfvén eigenmodes in a tokamak plasma. Here, a m,n = 2,1 magnetic island appears to be seeded in a MAST-U discharge by coupling of (Formula presented) (Formula presented) and (Formula presented) (Formula presented) Alfvén eigenmodes, which is demonstrated by increased squared normalised bicoherence calculated from magnetic probes preceding tearing mode onset. This observation offers a new explanation for tearing modes that would be otherwise addressed as spontaneous, and indicates three-wave coupling can seed 2,1 magnetic islands in plasmas without pre-existing (Formula presented) (Formula presented) tearing modes. Further, this mechanism has the potential to be more prevalent in burning plasmas expected in future fusion devices.

Depletion of Dark Matter Spikes by Massive Black Hole Mergers

ArXiv 2611.1317 (2026)

Authors:

Charlie Sharpe, Thomas FM Spieksma, Yonadav Barry Ginat, Ricarda S Beckmann, Alexander Heger, Bence Kocsis

Violent relaxation redux

ArXiv 2611.09531 (2026)

Authors:

Michael L Nastac, Yonadav Barry Ginat, Robert J Ewart, Michael Barnes, Alexander A Schekochihin

Ion dynamics in the ion diffusion region of symmetric magnetic reconnection

Physics of Plasmas AIP Publishing 33:11 (2026) 112101

Authors:

C Norgren, M Hesse, M André, L Richard, Yu V Khotyaintsev, DB Graham, T Phan

Abstract:

We investigate ion dynamics in the ion diffusion region of an antiparallel symmetric reconnection event observed by the Magnetospheric MultiScale mission in Earth's magnetotail. Through detailed investigation of the ion velocity distribution functions, we show that the ion dynamics are initially (upon first entering the current sheet) dominated by the acceleration from the Hall electric and magnetic fields. The Hall electric field ballistically accelerates the ions toward the neutral sheet. The subsequent magnetic forces associated with the reconnecting and Hall magnetic fields have two distinct effects. First, the magnetic force due to the reconnecting magnetic field upstream of the X line delays the Speiser acceleration by gyroturning the ions in the direction opposite to the reconnection electric field. Second, the magnetic force due to the Hall magnetic field gyroturns the ions toward the outflow, kick-starting the outflow jet over short distances. These dynamics are consistent with fast reconnection rates.

Overview of the MAST Upgrade physics programme: testing novel concepts at low aspect ratio to inform future devices

Nuclear Fusion IOP Publishing 66:11 (2026)

Authors:

JR Harrison, A Aboutaleb, M Aljunid, SY Allan, R Allan, A Alli, H Anand, Y Andrew, LC Appel, A Ash, J Ashton, F Auriemma, O Bachmann, S Bakes, P Balazs, O Bardsley, M Barnes, B Barrett, D Baver, C Beckley, J Bennett, J Bentley, J Berkery, M Bernert, N Bertelli, P Bilkova, S Blackmore, A Bock, W Boeglin, P Bohm, J Booth, A Bosnjak, C Bowman, J Bradley, L Bramucci, D Brida, M Brix, PK Browning, D Brunetti, P Bryant, J Bryant, J Buchanan, M Bull, M Bulman, N Bulmer, D Burke, P Cahill, P Cano-Megías, M Carpita, A Carruthers, L Casali, A Cassidy, F Causa, M Cecconello, A Celora, M Cha, B Chamberlain, B Chapman, B Chapman-Oplopoiou, R Chazal, X Chen, J Clark, M Clark, T Clayton, K Collie, D Collishaw-Schepman, JW Connor, M Coy, S Cramp, N Crocker, D Cruse, G Cunningham, M Czarski, I Cziegler, Y Damizia, P Davies, K Davies, I Day, E Delabie, GL Derks, S Dixon, J Dobrashian, M Dreval, X Du, H Dudding, D Dunai, M Dunne, F Ebrahimi, J Edmond, J Edwards, H El-Haroun, S Elmore, Y Enters, M Faitsch, F Federici, N Fedorczak, F Felici, N Ferraro, AR Field, P Figueiredo, I FitzGerald, M Fitzgerald, R Fitzpatrick, C Fitzpatrick, S Frankel, L Frassinetti, D Frattolillo, S Freethy, W Fuller, R Futtersack, S Gabriellini, K Gage, J Galdon, J Galdon-Quiroga, M Gambrioli, C Garner, L Garzotti, TE Gheorghiu, KJ Gibson, C Gibson, E Giovannozzi, C Giroud, J Goatley, A Goodyear, M Gorelenkova, S Gosden, G Grassler, JP Graves, D Greenhouse, R Griffiths, VH Hall-Chen, CJ Ham, E Harrington, R Harrison, A Haupt, J Hawes, S Hegedus, SS Henderson, C Heo, C Hickling, M Hill, B Hnat, C Hogben, B Honey, L Howlett, Z Huang, A Hudoba, J Hughes, R Hussain, K Imada, P Ivanov, A Jackson, P Jacquet, F Jaulmes, P Jepson, T Jones, P Jones, M Juvonen, V Kachkanov, B Kandan, I Katramados, S Kaye, YO Kazakov, D Keeling, D Kennedy, A Kenny, H-T Kim, D King, R King, A King, V Kiptily, A Kirjasuo, A Kirk, A Kit, A Kleiner, M Knolker, S Kobussen, M Kochan, L Kogan, B Kool, D Kos, M Kotschenreuther, M Lampert, A Lawson, K Lawson, K-W Lee, G Lee, J Lee, M Lees, S Leigh, AW Leonard, G Liddiard, B Lipschultz, E Litherland-Smith, YQ Liu, BA Lomanowski, J Lombardo, N Lonigro, J Lore, J Lovell, R Lucock, T Luong, A Lvovskiy, J Macdonald, T Macwan, S Mahajan, F Maiden, R Maingi, C Man-Friel, F Mansfield, M Markl, S Marsden, R Martin, R Mathew, R Maurizio, U Mazzarese, S Mazzi, R McAdams, G McArdle, J McBride, K McClements, J McClenaghan, D McConville, K McKay, C McKnight, P McKnight, A McLean, BF McMillan, A McShee, J Measures, N Mehay, S Menmuir, HF Meyer, CA Michael, F Militello, IG Miron, R Mishra, J Mitchell, D Moiraf, P Monaghan, R Mooney, N Mooring, R Morales Gomes, D Morbey, S Mordijck, C Morgan, J Morris, D Moulton, S Munaretto, A Munasinghe, A Muraro, O Myatra, Y-S Na, TF Neiser, AO Nelson, SL Newton, M Nicassio, MG O’Mullane, C Olde, HJ Oliver, P Ollus, J Omotani, M Ono, FP Orsitto, R Osawa, N Osborne, T Osborne, R Otin, E Ozturk, F Palermo, A Pankin, I Paradela Pérez, J Parisi, E Parr, B Parry, BS Patel, E Pawelec, D Payne, C Paz-Soldan, A Phelps, L Piron, C Piron, G Pokol, R Preece, M Price, B Pritchard, R Proudfoot, G Pucella, T Pumfrett, D-Y Pyo, H Reimerdes, T Rhodes, E Ribeiro, D Rigamonti, J Riquezes, JF Rivero-Rodriguez, J Roberts, M Robson, K Ronald, E Rose, D Ryan, P Ryan, S Saarelma, S Sabbagh, A Salmi, R Sarwar, P Saunders, O Sauter, R Scannell, R Sealey, R Seath, S Sharapov, R Sharma, H Sheikh, S Shiraiwa, B Sieglin, SA Silburn, M Simmonds, J Simpson, A Sladkomedova, J Smith, P Smith, M Sos, VA Soukhanovskii, D Speirs, C Srinivasan, G Staebler, R Stephen, P Stevenson, J Stobbs, C Stroud, H Sun, H Sun, G Szepesi, DM Takács, T Tala, C Tame, C Theiler, B Thomas, S Thomas, S Thomas, N Thomas-Davies, AJ Thornton, A Tilley, I Tirkova, M Tobin, E Tomasina, A Tonel, P Tonner, A Tookey, G Tvalashvili, M Vallar, M Valovic, RGL Vann, L Velarde, L Velarde, K Verhaegh, E Viezzer, C Vincent, M Walsh, T Walsh, M Warr, S Wiesen, TA Wijkamp, D Wilkins, J Willis, T Wilson, HR Wilson, N Winston, G Withenshaw, H Wong, M Wood, R Worrall, Q Xia, G Xia, L Xiang, G Xiang, T Xu, JH Yu, V Zamkovska, M Zerbini, VK Zotta, M Zurita, LE di Grazia

Abstract:

The research programme performed on the Mega Amp Spherical Tokamak (MAST) Upgrade experiment has made significant advances in developing the physics understanding of low aspect ratio tokamaks in support of the operation of ITER and design of fusion powerplants. High performance plasma scenarios have been developed to facilitate a broad programme of experiments, in which confinement is constrained by the presence of m/n = 2/1 modes that cause substantial losses of fast ions. The onset of these modes coincides with the q = 2 surface residing in a local minimum in the toroidal current density profile. The maximum electron temperature at the pedestal top, Te,ped is limited with gas fuelling to ∼350 eV to maintain regular ELMs; higher Te,ped results in a transition to a non-stationary ELM-free regime. The operational space of spherical tokamaks has been expanded into small and ELM-free regimes. Strong shaping of the last closed flux surface can induce a transition from large to small ELMs, and ELM suppression with resonant magnetic perturbations has been observed for the first time in a low aspect ratio tokamak. Negative triangularity shaping has induced a transition from ELMy H-mode to a high-performance L-mode regime for the first time in a low aspect ratio tokamak. In studies of fast ion confinement, losses of fast particles due to Global Alfvén Eigenmodes have been identified. Interactions between fast ions generated by off-axis neutral beam injection and thermal neutrals can result in significant losses of fast ions. Experiments with on- and off-axis neutral beam injection exhibit a flux pumping mechanism, where the central safety factor is held to ∼1 in the absence of sawteeth. In studies of pedestal physics, it has been found that elevated main chamber neutral pressures result in an increase in the electron density and reduction in the temperature at the pedestal top. Advances in understanding plasma exhaust include the integration of a high-performance plasma core with detached outer divertors in the X-point target configuration. A newly commissioned lower divertor cryopump reduces the lower divertor neutral pressure by up to 50%, with minimal effect on the main chamber or upper divertor. New measurements and SOLPS-ITER simulations emphasise the importance of plasma–neutral interactions on divertor detachment in the conditions accessible in experiments. Real-time control of the ionisation front location in both divertor chambers independently has been demonstrated in double null experiments, enabled by the tightly baffled divertor chambers.