[1] F.Chen. An Indispensable Truth: How Fusion Power Can Save the Planet(2011).

[2] J.Wesson. Tokamaks(2004).

[3] T.Henderet?al.. Nucl. Fusion, 47, S128-S202(2007).

[4] R.Wenningeret?al.. Power handling and plasma protection aspects that affect the design of the DEMO divertor and first wall.

[5] E. J.Straitet?al.. Nucl. Fusion, 59, 112012(2019).

[6] T.Ravensbergen, T.Ravensbergen, Berkel M.van, A.Pereket?al., M.van Berkel, T.Ravensbergen, Berkel M.van, A.Pereket?al., A.Pereket?al.. Real-time feedback control of the impurity emission front in tokamak divertor plasmas. Nat. Commun., 12, 1105(2021).

[7] C.Angioliniet?al.. Tungsten transport in JET H-mode plasmas in hybrid scenario, experimental observations and modelling. Nucl. Fusion, 54, 083028(2014).

[8] G. A.Rattá, A.Rattá G., J.Vega, A.Murari, G.Vagliasindi, F.Johnson M., P. and, EFDA JET, J.Vega, A.Rattá G., J.Vega, A.Murari, G.Vagliasindi, F.Johnson M., P. and, EFDA JET, A.Murari, A.Rattá G., J.Vega, A.Murari, G.Vagliasindi, F.Johnson M., P. and, EFDA JET, G.Vagliasindi, A.Rattá G., J.Vega, A.Murari, G.Vagliasindi, F.Johnson M., P. and, EFDA JET, M. F.Johnson, A.Rattá G., J.Vega, A.Murari, G.Vagliasindi, F.Johnson M., P. and, EFDA JET, P. C.de Vries, A.Rattá G., J.Vega, A.Murari, G.Vagliasindi, F.Johnson M., P. and, EFDA JET. Nucl. Fusion, 50, 025005(2010).

[9] A.Murariet?al.. On the transfer of adaptive predictors between different devices for both mitigation and prevention of disruptions. Nucl. Fusion, 60, 056003(2020).

[10] J.Vega, J.Vega, A.Murari, S.Dormido-Cantoet?al., A.Murari, J.Vega, A.Murari, S.Dormido-Cantoet?al., S.Dormido-Cantoet?al.. Disruption prediction with artificial intelligence techniques in tokamak plasmas. Nat. Phys., 18, 741(2022).

[11] L.Pironet?al.. Progress in preparing real-time control schemes for Deuterium-Tritium operation in JET. Fusion Eng. Des., 166, 112305(2021).

[12] M.Lehnenet?al.. Nucl. Fusion, 51, 123010(2011).

[13] T.Craciunescu, T.Craciunescu, E.Peluso, A.Murari, M.Gelfusa and, E.Peluso, T.Craciunescu, E.Peluso, A.Murari, M.Gelfusa and, A.Murari, T.Craciunescu, E.Peluso, A.Murari, M.Gelfusa and, M.Gelfusa. Maximum likelihood bolometric tomography for the determination of the uncertainties in the radiation emission on JET TOKAMAK. Rev. Sci. Instrum., 89, 053504(2018).

[14] A.Murariet?al.. Investigating the thermal stability of highly radiative discharges on JET with a new tomographic method. Nucl. Fusion, 60, 046030(2020).

[15] C.Sozziet?al.. Termination of discharges in high performance scenarios in JET.

[16] R.Marianoet?al.. Acceleration of an algorithm based on the maximum likelihood bolometric tomography for the determination of uncertainties in the radiation emission on JET using heterogeneous platforms. Appl. Sci., 12, 6798(2022).

[17] A.Pauet?al.. A first analysis of JET plasma profile-based indicators for disruption prediction and avoidance. IEEE Trans. Plasma Sci., 46, 2691-2698(2018).

[18] I.Wyss, I.Wyss, A.Murari, L.Spolladore, E.Peluso, M.Gelfusa, P.Gaudio, R.Rossi and, A.Murari, I.Wyss, A.Murari, L.Spolladore, E.Peluso, M.Gelfusa, P.Gaudio, R.Rossi and, L.Spolladore, I.Wyss, A.Murari, L.Spolladore, E.Peluso, M.Gelfusa, P.Gaudio, R.Rossi and, E.Peluso, I.Wyss, A.Murari, L.Spolladore, E.Peluso, M.Gelfusa, P.Gaudio, R.Rossi and, M.Gelfusa, I.Wyss, A.Murari, L.Spolladore, E.Peluso, M.Gelfusa, P.Gaudio, R.Rossi and, P.Gaudio, I.Wyss, A.Murari, L.Spolladore, E.Peluso, M.Gelfusa, P.Gaudio, R.Rossi and, R.Rossi. Comparison of a fast low spatial resolution inversion method and peaking factors for the detection of anomalous radiation patterns and disruption prediction. Fusion Eng. Des., 193, 113625(2023).

[19] C. L.Lawson, L.Lawson C., R. J.Hanson. Solving Least Squares Problems(1995).

[20] T.Craciunescu, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, S.Soare, I.Tiseanu, V.Zoita and, G.Bonheure, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, S.Soare, I.Tiseanu, V.Zoita and, V.Kiptily, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, S.Soare, I.Tiseanu, V.Zoita and, A.Murari, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, S.Soare, I.Tiseanu, V.Zoita and, S.Soare, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, S.Soare, I.Tiseanu, V.Zoita and, I.Tiseanu, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, S.Soare, I.Tiseanu, V.Zoita and, V.Zoita. The maximum likelihood reconstruction method for JET neutron tomography. Nucl. Instrum. Methods Phys. Res., Sect. A, 595, 623-630(2008).

[21] T.Craciunescu, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, I.Tiseanu, V.Zoita and, G.Bonheure, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, I.Tiseanu, V.Zoita and, V.Kiptily, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, I.Tiseanu, V.Zoita and, A.Murari, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, I.Tiseanu, V.Zoita and, I.Tiseanu, T.Craciunescu, G.Bonheure, V.Kiptily, A.Murari, I.Tiseanu, V.Zoita and, V.Zoita. A comparison of four reconstruction methods for JET neutron and gamma tomography. Nucl. Instrum. Methods Phys. Res., Sect. A, 605, 374-383(2009).

[22] L. A.Shepp, A.Shepp L., Y.Vardi. Maximum likelihood reconstruction for emission tomography. IEEE Trans. Med. Imaging, 1, 113-122(1982).

[23] K.Lange, and K.Lange, K.Carson. EM reconstruction algorithms for emission and transmission tomography. J. Comput. Assisted Tomogr., 8, 306-316(1984).

[24] Y.Li. Noise propagation for iterative penalized-likelihood image reconstruction based on Fisher information. Phys. Med. Biol., 56, 1083-1103(2011).

[25] E.Peluso, E.Peluso, T.Craciunescu, A.Murari, P.Carvalho, M.Gelfusa and, T.Craciunescu, E.Peluso, T.Craciunescu, A.Murari, P.Carvalho, M.Gelfusa and, A.Murari, E.Peluso, T.Craciunescu, A.Murari, P.Carvalho, M.Gelfusa and, P.Carvalho, E.Peluso, T.Craciunescu, A.Murari, P.Carvalho, M.Gelfusa and, M.Gelfusa. A comprehensive study of the uncertainties in bolometric tomography on JET using the maximum likelihood method. Rev. Sci. Instrum., 90, 123502(2019).

[26] E.Peluso, E.Peluso, T.Craciunescu, M.Gelfusa, A.Murari, J.Carvalho P., P.Gaudio and, T.Craciunescu, E.Peluso, T.Craciunescu, M.Gelfusa, A.Murari, J.Carvalho P., P.Gaudio and, M.Gelfusa, E.Peluso, T.Craciunescu, M.Gelfusa, A.Murari, J.Carvalho P., P.Gaudio and, A.Murari, E.Peluso, T.Craciunescu, M.Gelfusa, A.Murari, J.Carvalho P., P.Gaudio and, P. J.Carvalho, E.Peluso, T.Craciunescu, M.Gelfusa, A.Murari, J.Carvalho P., P.Gaudio and, P.Gaudio. On the effects of missing chords and systematic errors on a new tomographic method for JET bolometry. Fusion Eng. Des., 146, 2124(2019).

[27] E.Peluso, E.Peluso, M.Gelfusa, T.Craciunescu, L.Martellucci, P.Gaudio, A.Murari and, M.Gelfusa, E.Peluso, M.Gelfusa, T.Craciunescu, L.Martellucci, P.Gaudio, A.Murari and, T.Craciunescu, E.Peluso, M.Gelfusa, T.Craciunescu, L.Martellucci, P.Gaudio, A.Murari and, L.Martellucci, E.Peluso, M.Gelfusa, T.Craciunescu, L.Martellucci, P.Gaudio, A.Murari and, P.Gaudio, E.Peluso, M.Gelfusa, T.Craciunescu, L.Martellucci, P.Gaudio, A.Murari and, A.Murari. Dealing with artefacts in JET iterative bolometric tomography using masks. Plasma Phys. Controlled Fusion, 64, 045013(2022).

[28] M.Gelfusa, M.Gelfusa, T.Craciunescu, E.Peluso, L.Giacomelli, V.Kiptily, C.Reux, G.Szepesi, A.Murari and, T.Craciunescu, M.Gelfusa, T.Craciunescu, E.Peluso, L.Giacomelli, V.Kiptily, C.Reux, G.Szepesi, A.Murari and, E.Peluso, M.Gelfusa, T.Craciunescu, E.Peluso, L.Giacomelli, V.Kiptily, C.Reux, G.Szepesi, A.Murari and, L.Giacomelli, M.Gelfusa, T.Craciunescu, E.Peluso, L.Giacomelli, V.Kiptily, C.Reux, G.Szepesi, A.Murari and, V.Kiptily, M.Gelfusa, T.Craciunescu, E.Peluso, L.Giacomelli, V.Kiptily, C.Reux, G.Szepesi, A.Murari and, C.Reux, M.Gelfusa, T.Craciunescu, E.Peluso, L.Giacomelli, V.Kiptily, C.Reux, G.Szepesi, A.Murari and, G.Szepesi, M.Gelfusa, T.Craciunescu, E.Peluso, L.Giacomelli, V.Kiptily, C.Reux, G.Szepesi, A.Murari and, A.Murari. A maximum likelihood tomographic method applied to JET gamma ray emission during the current quench. Fusion Eng. Des., 168, 112637(2021).

[29] L.Spolladore, L.Spolladore, R.Rossi, I.Wyss, P.Gaudio, A.Murari, M.Gelfusa and, R.Rossi, L.Spolladore, R.Rossi, I.Wyss, P.Gaudio, A.Murari, M.Gelfusa and, I.Wyss, L.Spolladore, R.Rossi, I.Wyss, P.Gaudio, A.Murari, M.Gelfusa and, P.Gaudio, L.Spolladore, R.Rossi, I.Wyss, P.Gaudio, A.Murari, M.Gelfusa and, A.Murari, L.Spolladore, R.Rossi, I.Wyss, P.Gaudio, A.Murari, M.Gelfusa and, M.Gelfusa. Detection of MARFEs using visible cameras for disruption prevention. Fusion Eng. Des., 190, 113507(2023).

[30] R.Rossiet?al.. Development of robust indicators for the identification of electron temperature profile anomalies and application to JET. Plasma Phys. Controlled Fusion, 64, 045002(2022).

[31] A.Bhattacharyya. On a measure of divergence between two multinomial populations. Indian J. Stat., 7, 401-406(1946).

[32] F. C.Schuelleret?al.. Disruptions in tokamaks. Plasma Phys. Controlled Fusion, 37, A135(1995).

[33] M.Greenwald, M.Greenwald, L.Terry J., M.Wolfe S., S.Ejima, G.Bell M., M.Kaye S., G. and, J. L.Terry, M.Greenwald, L.Terry J., M.Wolfe S., S.Ejima, G.Bell M., M.Kaye S., G. and, S. M.Wolfe, M.Greenwald, L.Terry J., M.Wolfe S., S.Ejima, G.Bell M., M.Kaye S., G. and, S.Ejima, M.Greenwald, L.Terry J., M.Wolfe S., S.Ejima, G.Bell M., M.Kaye S., G. and, M. G.Bell, M.Greenwald, L.Terry J., M.Wolfe S., S.Ejima, G.Bell M., M.Kaye S., G. and, S. M.Kaye, M.Greenwald, L.Terry J., M.Wolfe S., S.Ejima, G.Bell M., M.Kaye S., G. and, G. H.Neilson. A new look at density limits in tokamaks. Nucl. Fusion, 28, 2199-2207(1988).

[34] G. A.Rattáet?al.. An advanced disruption predictor for JET tested in a simulated real-time environment. Nucl. Fusion, 50, 025005(2010).

[35] C. D.Challiset?al.. Nucl. Fusion, 60, 086008(2020).

[36] G.Pucellaet?al.. Onset of tearing modes in plasma termination on JET: The role of temperature hollowing and edge cooling. Nucl. Fusion, 61, 046020(2021).

[37] B.Lipschultzet?al.. Marfe: An edge plasma phenomenon. Nucl. Fusion, 24, 977(1984).

[38] J. F.Drake. Marfes: Radiative condensation in tokamak edge plasma. Phys. Fluids, 30, 2429(1987).

[39] G. A.Rattá, A.Rattá G., J.Vega, A.Murari, D.Gadariya, JET and, J.Vega, A.Rattá G., J.Vega, A.Murari, D.Gadariya, JET and, A.Murari, A.Rattá G., J.Vega, A.Murari, D.Gadariya, JET and, D.Gadariya, A.Rattá G., J.Vega, A.Murari, D.Gadariya, JET and. PHAD: A phase-oriented disruption prediction strategy for avoidance, prevention, and mitigation in JET. Nucl. Fusion, 61, 116055(2021).

[40] A. R.Fieldet?al.. The impact of felling and W radiation on the performance of high-power, ITER-baseline scenario plasma in JET-ILW. Plasma Phys. Controlled Fusion, 63, 095013(2021).

[41] J.Garciaet?al.. Integrated scenario development at JET for DT operation and ITER risk mitigation.

[42] L.Piron, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, D.Van Eester, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, D.Frigione, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, L.Garzotti, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, P. J.Lomas, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, M.Lennholm, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, F.Rimini, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, F.Auriemma, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, M.Baruzzo, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, P. J.Carvalho, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, D. R.Ferreira, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, A. R.Field, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, K.Kirov, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, Z.Stancar, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, C. I.Stuart, L.Piron, Eester D.Van, D.Frigione, L.Garzotti, J.Lomas P., M.Lennholm, F.Rimini, F.Auriemma, M.Baruzzo, J.Carvalho P., R.Ferreira D., R.Field A., K.Kirov, Z.Stancar, I.Stuart C., D.Valcarcel and, D.Valcarcel. Radiation control in deuterium, tritium and deuterium-tritium JET baseline plasmas - part. Fusion Eng. Des, 193, 113634(2023).

[43] E.Lercheet?al.. ICRH for core impurity mitigation in JET-ILW. AIP Conf. Proc., 1689, 030002(2015).

[44] M.Konget?al.. Physics-based control of neoclassical tearing modes on TCV. Plasma Phys. Controlled Fusion, 64, 044008(2022).

[45] D. R.Ferreira, R.Ferreira D., J.Carvalho P., H.Fernandes and, P. J.Carvalho, R.Ferreira D., J.Carvalho P., H.Fernandes and, H.Fernandes. Deep learning for plasma tomography and disruption prediction from bolometer data. IEEE Trans. Plasma Sci., 48, 36-45(2019).

[46] D. R.Ferreiraet?al.. Fusion Eng. Des., 164, 112179(2021).

[47] D. R.Ferreiraet?al.. Deep learning for the analysis of disruption precursors based on plasma tomography. Fusion Sci. Technol., 76, 901-911(2020).

[48] A.Murariet?al.. Prototype of an adaptive disruption predictor for JET based on fuzzy logic and regression trees. Nucl. Fusion, 48, 035010(2008).

[49] C.Reaet?al.. Disruption prediction investigations using machine learning tools on DIII-D and Alcator C-Mod. Plasma Phys. Controlled Fusion, 60, 084004(2018).

[50] A.Murariet?al.. Adaptive predictors based on probabilistic SVM for real-time disruption mitigation on JET. Nucl. Fusion, 58, 056002(2018).

[51] C.Rea, C.Rea, J.Montes K., G.Erickson K., S.Granetz R., R. and, K. J.Montes, C.Rea, J.Montes K., G.Erickson K., S.Granetz R., R. and, K. G.Erickson, C.Rea, J.Montes K., G.Erickson K., S.Granetz R., R. and, R. S.Granetz, C.Rea, J.Montes K., G.Erickson K., S.Granetz R., R. and, R. A.Tinguely. A real-time machine learning-based disruption predictor in DIII-D. Nucl. Fusion, 59, 096016(2019).

[52] A.Murari, A.Murari, M.Lungaroni, M.Gelfusa, E.Peluso, J.Vega, JET and, M.Lungaroni, A.Murari, M.Lungaroni, M.Gelfusa, E.Peluso, J.Vega, JET and, M.Gelfusa, A.Murari, M.Lungaroni, M.Gelfusa, E.Peluso, J.Vega, JET and, E.Peluso, A.Murari, M.Lungaroni, M.Gelfusa, E.Peluso, J.Vega, JET and, J.Vega, A.Murari, M.Lungaroni, M.Gelfusa, E.Peluso, J.Vega, JET and. Adaptive learning for disruption prediction in non-stationary conditions. Nucl. Fusion, 59, 086037(2019).

[53] A.Murari, A.Murari, R.Rossi, M.Lungaroni, M.Baruzzo, M.Gelfusa and, R.Rossi, A.Murari, R.Rossi, M.Lungaroni, M.Baruzzo, M.Gelfusa and, M.Lungaroni, A.Murari, R.Rossi, M.Lungaroni, M.Baruzzo, M.Gelfusa and, M.Baruzzo, A.Murari, R.Rossi, M.Lungaroni, M.Baruzzo, M.Gelfusa and, M.Gelfusa. Stacking of predictors for the automatic classification of disruption types to optimize the control logic. Nucl. Fusion, 61, 036027(2021).

[54] A.Murariet?al.. Investigating the physics of tokamak global stability with interpretable machine learning tools. Appl. Sci., 10, 6683(2020).

[55] E.Pelusoet?al.. Alternative detection of n = 1 modes slowing down on ASDEX Upgrade. Appl. Sci., 10, 7891(2020).

[56] M. E.Puiattiet?al.. Radiation pattern and impurity transport in argon seeded ELMy H-mode discharges in JET. Plasma Phys. Controlled Fusion, 44, 1863-1878(2002).

[57] L.Pironet?al.. Radiation control in tritium and deuterium-tritium JET baseline plasmas—Part II. Fusion Eng. Des., 192, 113695(2023).