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ITER envisages the use of two heating neutral beam injectors plus an optional one as part of the auxiliary heating and current drive system. The 16.5 MW expected neutral beam power per injector is several notches higher than worldwide…

Plasma Physics · Physics 2023-04-05 D. Marcuzzi , V. Toigo , M. Boldrin , G. Chitarin , S. Dal Bello , L. Grando , A. Luchetta , R. Pasqualotto , M. Pavei , G. Serianni , L. Zanotto , R. Agnello , P. Agostinetti , M. Agostini , D. Aprile , M. Barbisan , M. Battistella , G. Berton , M. Bigi , M. Brombin , V. Candela , V. Candeloro , A. Canton , R. Casagrande , C. Cavallini , R. Cavazzana , L. Cordaro , N. Cruz , M. Dalla Palma , M. Dan , A. De Lorenzi , R. Delogu , M. De Muri , M. De Nardi , S. Denizeau , M. Fadone , F. Fellin , A. Ferro , E. Gaio , C. Gasparrini , F. Gnesotto , P. Jain , A. La Rosa , D. Lopez-Bruna , R. Lorenzini , A. Maistrello , G. Manduchi , S. Manfrin , N. Marconato , I. Mario , G. Martini , R. Milazzo , T. Patton , S. Peruzzo , N. Pilan , A. Pimazzoni , C. Poggi , N. Pomaro , B. Pouradier-Duteil , M. Recchia , A. Rigoni-Garola , D. Rizzetto , A. Rizzolo , F. Santoro , E. Sartori , B. Segalini , A. Shepherd , M. Siragusa , P. Sonato , A. Sottocornola , E. Spada , S. Spagnolo , M. Spolaore , C. Taliercio , P. Tinti , P. Tomsič , L. Trevisan , M. Ugoletti , M. Valente , M. Valisa , F. Veronese , M. Vignando , P. Zaccaria , R. Zagorski , B. Zaniol , M. Zaupa , M. Zuin , M. Cavenago , D. Boilson , C. Rotti , H. Decamps , F. Geli , A. Sharma , P. Veltri , J. Zacks , M. Simon , F. Paolucci , A. Garbuglia , D. Gutierrez , A. Masiello , G. Mico , C. Labate , P. Readman , E. Bragulat , L. Bailly-Maitre , G. Gomez , G. Kouzmenko , F. Albajar , M. Kashiwagi , H. Tobari , A. Kojima , M. Murayama , S. Hatakeyama , E. Oshita , T. Maejima , N. Shibata , Y. Yamashita , K. Watanabe , N. P. Singh , M. J. Singh , H. Dhola , U. Fantz , B. Heinemann , C. Wimmer , D. Wünderlich , K. Tsumori , G. Croci , G. Gorini , A. Muraro , M. Rebai , M. Tardocchi , L. Giacomelli , D. Rigamonti , F. Taccogna , D. Bruno , M. Rutigliano , S. Longo , S. Deambrosis , E. Miorin , F. Montagner , A. Tonti , F. Panin

The SPIDER experiment, part of the Neutral Beam Test Facility (NBTF) at Consorzio RFX (Padua, Italy), is the prototype of the negative ion source for the ITER neutral beam injectors; the source is coupled to a 100 kV three-grid acceleration…

Plasma Physics · Physics 2023-04-07 M. Barbisan , B. Zaniol , R. Pasqualotto , G. Serianni , M. Ugoletti

Consorzio RFX and INFN-LNL are building a flexible small ion source (NIO1) capable of producing about 130 mA of H- ions accelerated at 60 KeV. Aim of the experiment is to test and develop the instrumentation for SPIDER and MITICA, the…

Plasma Physics · Physics 2022-11-08 M. Barbisan , B. Zaniol , M. Cavenago , R. Pasqualotto

The Neutral beam Injectors of the ITER experiment will be based on negative ion sources for the generation of beams composed by 1 MeV H/D particles. The prototype of these sources is currently under testing in the SPIDER experiment, part of…

Plasma Physics · Physics 2023-08-30 M. Barbisan , R. Agnello , G. Casati , R. Pasqualotto , E. Sartori , G. Serianni

The Neutral Beam Injectors of the ITER experiment will rely on negative ion sources to produce 16.7 MW beams of H/D particles accelerated at 1 MeV. The prototype of these sources was built and is currently operated in the SPIDER experiment…

MITICA (Megavolt ITER Injector & Concept Advancement), the full scale prototype of ITER Heating Neutral Beam, is under realization at the Neutral Beam Test Facility (Padova, Italy). It is designed to deliver 16.5 MW to ITER plasma, obtained…

The ITER Heating Neutral Beam (HNB) injector is required to deliver 16.7 MW power into the plasma from a neutralised beam of H-/D- negative ions, produced by an RF source and accelerated up to 1 MeV. To enhance the H-/D- production, the…

Plasma Physics · Physics 2022-11-04 M. Barbisan , R. Pasqualotto , A. Rizzolo

The NIO1 experiment hosts a flexible RF H- ion source, developed by INFN-LNL and Consorzio RFX to improve the present concepts for the production and acceleration of negative ions. The source is also used to benchmark the instrumentation…

Plasma Physics · Physics 2022-11-09 M. Barbisan , B. Zaniol , M. Cavenago , G. Serianni , R. Pasqualotto

The ITER Heating Neutral Beams (HNBs) require large, high-energy H/D atom beams (285/330 A/m^2 extracted current density, and 1/0.87 MeV acceleration energy, respectively for H and D). To address the associated challenges, the SPIDER…

Plasma Physics · Physics 2025-11-05 R. Agnello , M. Barbisan , R. Pasqualotto , B. Pouradier-Duteil , E. Sartori , A. Tiso , B. Zaniol

The Heating Neutral Beam Injectors (HNBs) for ITER will have to deliver 16.7 MW beams of H/D particles at 1 MeV energy. The beams will be produced from H-/D- ions, generated by a radiofrequency plasma source coupled to an ion acceleration…

The SPIDER H-/D- ion source is currently in operation in the Neutral Beam Test facility (NBTF) at Consorzio RFX (Padova, Italy) to prove the possibility of generating up to 40 A of negative ions, with a maximum extracted current density of…

Plasma Physics · Physics 2022-11-11 M. Barbisan , S. Cristofaro , L. Zampieri , R. Pasqualotto , A. Rizzolo

The SPIDER experiment, operated at the Neutral Beam Test Facility of Consorzio RFX, Padua, hosts the prototype of the H-/D- ion source for the ITER neutral beam injectors. The maximization of the ion current extracted from the source and…

Plasma Physics · Physics 2023-08-30 M. Barbisan , R. Agnello , G. Casati , R. Pasqualotto , C. Poggi , E. Sartori , M. Spolaore , G. Serianni

SPIDER is the prototype ion source of MITICA, the full-size neutral beam heating system conceived for the ITER tokamak. It includes eight drivers to heat and sustain the inductively coupled plasma (ICP). Owing to their near cylindrical…

Plasma Physics · Physics 2023-05-17 D. López-Bruna , P. Jain , M. Recchia , B. Zaniol , E. Sartori , C. Poggi , V. Candeloro , G. Serianni , P. Veltri

A conceptual experimental method for providing a new measurement of the underlying beta decay spectra from fission products is presented. The goal is to provide additional information related to the prediction of the antineutrino emission…

Nuclear Experiment · Physics 2013-04-16 D. Asner , K. A. Burns , B. Greenfield , M. S. Kos , J. L. Orrell , M. Schram , B. A. VanDevender , D. Wootan

In this paper we develop an analytical framework for the study of electrochemical impedance of mixed ionic and electronic conductors (MIEC). The framework is based on first-principles and it features the coupling of electrochemical…

Chemical Physics · Physics 2017-08-23 Francesco Ciucci , Yong Hao , David G. Goodwin

The ITER Vertical Neutron Camera (VNC) is a multichannel collimator system designed to measure the neutron emissivity profile and spectra. The energy spectrum measurements of neutrons made by the VNC will contribute to the reconstruction of…

Plasma Physics · Physics 2020-01-29 Timofey Kormilitsyn , Grigory Nemtsev , Roman Rodionov , Yury Kashchuk , Dmitry Portnov

For the ITER-like wall, the JET mirror link divertor spectroscopy system was redesigned to fully cover the tungsten horizontal strike plate with faster time resolution and improved near-UV performance. Since the ITER-like wall project…

We propose applications of Radioactive Ion Beam facilities to investigate physics beyond the Standard Model. In particular, we focus on the possible measurement of coherent neutrino-nucleus scattering and on a search for sterile neutrinos,…

High Energy Physics - Phenomenology · Physics 2015-06-04 Catalina Espinoza , Rimantas Lazauskas , Cristina Volpe

In the development of magnetically confined fusion as an economically sustainable power source, ITER is currently under construction. Beyond ITER is the DEMO programme in which the physics and engineering aspects of a future fusion power…

Plasma Physics · Physics 2014-02-28 R. McAdams
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