22 results on '"Vincenzi, Pietro"'
Search Results
2. Core integrated simulations for the Divertor Tokamak Test facility scenarios towards consistent core–pedestal–SOL modelling
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Casiraghi, Irene, primary, Mantica, Paola, additional, Ambrosino, Roberto, additional, Aucone, Lorenzo, additional, Baiocchi, Benedetta, additional, Balbinot, L., additional, Barberis, Tommaso, additional, Castaldo, A., additional, Cavedon, Marco, additional, Frassinetti, Lorenzo, additional, Innocente, Paolo, additional, Koechl, Florian, additional, Nowak, Silvana, additional, Agostinetti, Piero, additional, Ceccuzzi, Silvio, additional, Figini, Lorenzo, additional, Granucci, Gustavo, additional, and Vincenzi, Pietro, additional
- Published
- 2023
- Full Text
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3. Kinetic and magnetic control of fusion power fluctuations in EU DEMO
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Siccinio, Mattia, David, Pierre, Grazia, Luigi E. Di, Fable, Emiliano, Mattei, Massimiliano, Maviglia, Francesco, Tsironis, Christos, Van Eester, Dirk, Vincenzi, Pietro, Chuanren, Wu, and Zohm, Hartmut
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Technology ,ddc:600 - Published
- 2022
4. First-principle integrated modelling of the main scenarios of the new Divertor Tokamak Test facility
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Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Aucone Lorenzo, Baiocchi Benedetta, Balbinot Luca, Castaldo Antonio, Citrin Jonathan, Frassinetti Lorenzo, Innocente Paolo, Mariani Alberto, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Nyström Hampus, Valisa Marco, Vincenzi Pietro, Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Mariani, A, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Nyström, H, Valisa, M, and Vincenzi, P
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Divertor Tokamak Test facility, DTT, integrated modelling, plasma, quasi-linear transport models ,Divertor Tokamak Test Facility ,DTT - Abstract
In the European Roadmap towards thermonuclear fusion power production, studying the controlled exhaust of energy and particles from a fusion reactor is a top priority research item. This is the main goal of the Divertor Tokamak Test (DTT) facility, a D-shaped superconducting tokamak (R = 2.19 m, a = 0.70 m, BT
- Published
- 2021
5. Conceptual design of a collimated neutron flux monitor and spectrometer for DTT
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Cecconello, Marco, Conroy, Sean, Ericsson, Göran, Eriksson, Jacob, Hjalmarsson, Anders, Sperduti, Andrea, Casiraghi, Irene, Mantica, Paola, Vincenzi, Pietro, Bolzonella, Tommaso, Agostinetti, Piero, Villari, Rosaria, Cecconello, Marco, Conroy, Sean, Ericsson, Göran, Eriksson, Jacob, Hjalmarsson, Anders, Sperduti, Andrea, Casiraghi, Irene, Mantica, Paola, Vincenzi, Pietro, Bolzonella, Tommaso, Agostinetti, Piero, and Villari, Rosaria
- Abstract
A conceptual design and performance studies for a collimated neutron flux monitor and neutron spectrometer for the Divertor Tokamak Test (DTT) facility are presented. This study is based on the single-null divertor configuration and for “Half Power” and “Full power” scenarios with 15 MW of negative-ion NBI, 29 MW of ECH and 3 MW of ICRF heating with a maximum neutron yield of 1.5 × 1017 s−1. Fast ion distributions (both from auxiliary heating systems and fusion born) have been simulated in TRANSP/NUBEAM and the corresponding neutron energy spectra have been calculated using DRESS. Synthetic diagnostics have been implemented to determine the neutron fluxes and spectra at the detector location. Neutron emissivity profiles, plasma position, core ion temperature and the ratio of thermal and non-thermal D ion populations can be obtained with good accuracy and time resolution.
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- 2021
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6. First-principle integrated modelling of the main scenarios of the new Divertor Tokamak Test facility
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Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Mariani, A, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Nyström, H, Valisa, M, Vincenzi, P, Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Aucone Lorenzo, Baiocchi Benedetta, Balbinot Luca, Castaldo Antonio, Citrin Jonathan, Frassinetti Lorenzo, Innocente Paolo, Mariani Alberto, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Nyström Hampus, Valisa Marco, Vincenzi Pietro, Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Mariani, A, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Nyström, H, Valisa, M, Vincenzi, P, Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Aucone Lorenzo, Baiocchi Benedetta, Balbinot Luca, Castaldo Antonio, Citrin Jonathan, Frassinetti Lorenzo, Innocente Paolo, Mariani Alberto, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Nyström Hampus, Valisa Marco, and Vincenzi Pietro
- Published
- 2021
7. Integrated modelling of the main Divertor Tokamak Test facility scenarios
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Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Dicorato, M, Frassinetti, L, Mariani, A, Vincenzi, P, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Innocente, P, Johnson, T, Nyström, H, Valisa, M, Mantica, Paola, Koechl, Florian, Ambrosino, Roberto, Aucone, Lorenzo, Baiocchi, Benedetta, Balbinot, Luca, Castaldo, Antonio, Citrin Jonathan, Dicorato, Mattia, Frassinetti, Lorenzo, Mariani, Alberto, Vincenzi, Pietro, Agostinetti, Piero, Ceccuzzi, Silvio, Figini, Lorenzo, Granucci, Gustavo, Innocente, Paolo, Johnson, Thomas, Nyström, Hampus, Valisa, Marco, Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Dicorato, M, Frassinetti, L, Mariani, A, Vincenzi, P, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Innocente, P, Johnson, T, Nyström, H, Valisa, M, Mantica, Paola, Koechl, Florian, Ambrosino, Roberto, Aucone, Lorenzo, Baiocchi, Benedetta, Balbinot, Luca, Castaldo, Antonio, Citrin Jonathan, Dicorato, Mattia, Frassinetti, Lorenzo, Mariani, Alberto, Vincenzi, Pietro, Agostinetti, Piero, Ceccuzzi, Silvio, Figini, Lorenzo, Granucci, Gustavo, Innocente, Paolo, Johnson, Thomas, Nyström, Hampus, and Valisa, Marco
- Published
- 2021
8. Overview on the first-principle integrated modelling of the main scenarios of the new Divertor Tokamak Test facility
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Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Mariani, A, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Nyström, H, Valisa, M, Vincenzi, P, Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Aucone Lorenzo, Baiocchi Benedetta, Balbinot Luca, Castaldo Antonio, Citrin Jonathan, Frassinetti Lorenzo, Innocente Paolo, Mariani Alberto, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Nyström Hampus, Valisa Marco, Vincenzi Pietro, Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Aucone, L, Baiocchi, B, Balbinot, L, Castaldo, A, Citrin, J, Frassinetti, L, Innocente, P, Mariani, A, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Nyström, H, Valisa, M, Vincenzi, P, Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Aucone Lorenzo, Baiocchi Benedetta, Balbinot Luca, Castaldo Antonio, Citrin Jonathan, Frassinetti Lorenzo, Innocente Paolo, Mariani Alberto, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Nyström Hampus, Valisa Marco, and Vincenzi Pietro
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- 2021
9. Exploring Divertor Tokamak Test (DTT) operation space and plasma scenarios through time-dependent 0.5D integrated modelling
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Giruzzi, G, Arnas, C, Borba, A, Gopal, S, Lebedev, S, Mantsinen, M, Vincenzi, P, Bolzonella, T, Ambrosino, R, Castaldo, A, Casiraghi, I, Mantica, P, Vincenzi, Pietro, Bolzonella, Tommaso, Ambrosino, Roberto, Castaldo, Antonio, Casiraghi, Irene, Mantica, Paola, Giruzzi, G, Arnas, C, Borba, A, Gopal, S, Lebedev, S, Mantsinen, M, Vincenzi, P, Bolzonella, T, Ambrosino, R, Castaldo, A, Casiraghi, I, Mantica, P, Vincenzi, Pietro, Bolzonella, Tommaso, Ambrosino, Roberto, Castaldo, Antonio, Casiraghi, Irene, and Mantica, Paola
- Published
- 2021
10. First-principle based multi-channel integrated modelling in support to the design of the Divertor Tokamak Test facility
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Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Baiocchi, B, Castaldo, A, Citrin, J, Dicorato, M, Frassinetti, L, Mariani, A, Vincenzi, P, Agostinetti, P, Aucone, L, Balbinot, L, Ceccuzzi, S, Figini, L, Granucci, G, Innocente, P, Johnson, T, Nyström, H, Valisa, M, Casiraghi, Irene, Mantica, Paola, Koechl, Florian, Ambrosino, Roberto, Baiocchi, Benedetta, Castaldo, Antonio, Citrin, Jonathan, Dicorato, Mattia, Frassinetti, Lorenzo, Mariani, Alberto, Vincenzi, Pietro, Agostinetti, Piero, Aucone, Lorenzo, Balbinot, Luca, Ceccuzzi, Silvio, Figini, Lorenzo, Granucci, Gustavo, Innocente, Paolo, Johnson, Thomas J, Nyström, Hampus, Valisa, Marco, Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Baiocchi, B, Castaldo, A, Citrin, J, Dicorato, M, Frassinetti, L, Mariani, A, Vincenzi, P, Agostinetti, P, Aucone, L, Balbinot, L, Ceccuzzi, S, Figini, L, Granucci, G, Innocente, P, Johnson, T, Nyström, H, Valisa, M, Casiraghi, Irene, Mantica, Paola, Koechl, Florian, Ambrosino, Roberto, Baiocchi, Benedetta, Castaldo, Antonio, Citrin, Jonathan, Dicorato, Mattia, Frassinetti, Lorenzo, Mariani, Alberto, Vincenzi, Pietro, Agostinetti, Piero, Aucone, Lorenzo, Balbinot, Luca, Ceccuzzi, Silvio, Figini, Lorenzo, Granucci, Gustavo, Innocente, Paolo, Johnson, Thomas J, Nyström, Hampus, and Valisa, Marco
- Abstract
An intensive integrated modelling work of the main scenarios of the new Divertor Tokamak Test (DTT) facility with a single null divertor configuration has been performed using first principle quasi-linear transport models, in support of the design of the device and of the definition of its scientific work programme. First results of this integrated modelling work on DTT (R0 = 2.14 m, a = 0.65 m) are presented here along with outcome of the gyrokinetic simulations used to validate the reduced models in the DTT range of parameters. As a result of this work, the heating mix has been defined, the size of device has been increased to R0 = 2.19 m and a = 0.70 m, the use of pellets for fuelling has been recommended and reference profiles for diagnostic design, estimates of neutron yields and fast particle losses have been made available.
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- 2021
11. Conceptual Design of the Beamline for the DTT Neutral Beam Injector following a Double Beam Source Design Approach
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AGOSTINETTI, Piero, primary, BENEDETTI, Eugenio, additional, BOLZONELLA, Tommaso, additional, BONESSO, Massimiliano, additional, CASIRAGHI, Irene, additional, DIMA, Razvan, additional, FAVERO, Giacomo, additional, FERRO, Alberto, additional, GOBBIN, Marco, additional, GRANUCCI, Gustavo, additional, HU, Chundong, additional, MANTICA, Paola, additional, LUCCHINI, Francesco, additional, PEPATO, Adriano, additional, PILAN, Nicola, additional, RAFFAELLI, Fabrizio, additional, REBESAN, Pietro, additional, ROMANO, Afra, additional, SPIZZO, Gianluca, additional, VERONESE, Fabio, additional, VINCENZI, Pietro, additional, XIE, Yahong, additional, and XIE, Yuanlai, additional
- Published
- 2021
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12. First principle scenario modelling of the Divertor Tokamak Test facility
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Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Baiocchi Benedetta, Citrin Jonathan, Frassinetti Lorenzo, Mariani Alberto, Vincenzi Pietro, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Martin Piero, Valisa Marco, Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Baiocchi, B, Citrin, J, Frassinetti, L, Mariani, A, Vincenzi, P, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Martin, P, and Valisa, M
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Divertor Tokamak Test facility, DTT, First principle scenario modelling, integrated modelling, quasi-linear transport models ,Divertor Tokamak Test facility, DTT, scenario modelling, integrated modelling, quasi-linear transport models - Published
- 2020
13. First principle scenario modelling of the Divertor Tokamak Test facility
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Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Baiocchi, B, Citrin, J, Frassinetti, L, Mariani, A, Vincenzi, P, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Martin, P, Valisa, M, Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Baiocchi Benedetta, Citrin Jonathan, Frassinetti Lorenzo, Mariani Alberto, Vincenzi Pietro, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Martin Piero, Valisa Marco, Casiraghi, I, Mantica, P, Koechl, F, Ambrosino, R, Baiocchi, B, Citrin, J, Frassinetti, L, Mariani, A, Vincenzi, P, Agostinetti, P, Ceccuzzi, S, Figini, L, Granucci, G, Johnson, T, Martin, P, Valisa, M, Casiraghi Irene, Mantica Paola, Koechl Florian, Ambrosino Roberto, Baiocchi Benedetta, Citrin Jonathan, Frassinetti Lorenzo, Mariani Alberto, Vincenzi Pietro, Agostinetti Piero, Ceccuzzi Silvio, Figini Lorenzo, Granucci Gustavo, Johnson Thomas, Martin Piero, and Valisa Marco
- Published
- 2020
14. Design and mock-up tests of the RING photoneutralizer concept for an efficient DEMO NBI
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Vincenzi Pietro, Fassina Alessandro, Giudicotti Leonardo, and Pasqualotto Roberto
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RING photoneutralization ,optical cavity ,Physics::Plasma Physics ,photo-neutralization ,Physics::Accelerator Physics ,Physics::Optics ,NBI ,negative ions ,DEMO - Abstract
High energy (800 keV) Neutral Beam Injection (NBI) is one of the methods being considered to heat EU DEMO plasma [1]. A major issue of present NBI systems is the limited efficiency of the gas neutralizer (for ITER NBI ~55%), which impacts on the overall system efficiency. An attractive method, but still undemonstrated at full performances, is the photo-neutralization of the negative D-ion beam. In this process the energetic ions pass through an optical cavity where they impact on laser photons with a frequency chosen to maximize the neutralization cross section. The expected neutralization efficiency can be up to 70-90%. A possible scheme for photoneutralization is named RING (Recirculation Injection by Nonlinear Gating) [2] where the second harmonic of a Nd:YAG laser is extracted and trapped within a non-resonant optical cavity. A mock-up of the optical cavity has been built in Consorzio RFX to study its performances in order to demonstrate the feasibility of the RING concept and its potentiality for a full-scale NBI photoneutralizer. The mock-up has been operated with a low repetition rate (10 Hz) Nd:YAG laser (?=1064 nm). The optical alignment of the cavity appears not to be critical and first operations are aimed to achieve the 2nd harmonic generation (SHG) saturation regime. The measurements of the SHG efficiency using a Lithium Triborate (LBO) crystal confirm the non-linearity of the process with the crystal thickness. The optical properties of the recirculating light are described by measuring the beam envelope profile with a laser-triggered CCD camera and the trapped beam pulse decay time with a fast photodiode. Operations with the mock-up are fundamental to assess the optical cavity performance and estimate the loss channels affecting the beam recirculation.
- Published
- 2019
15. Conceptual design of a Neutral Beam Heating system for DTT
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Agostinetti Piero, Bolzonella Tommaso, Sonato Piergiorgio, Vallar Matteo, and Vincenzi Pietro
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ITER ,Divertor Tokamak Test ,Neutral Beam Heating ,DEMO ,DTT - Abstract
The main purpose of the Divertor Tokamak Test (DTT) is to study solutions to mitigate the issue of power exhaust in conditions relevant for ITER and DEMO. The key feature of such a study is to equip the machine with a significant amount of auxiliary heating power (45 MW) in order to test different divertor solutions. According to the Italian project, the experiment is foreseen to operate with the following main parameters: BT = 6 T, IP = 5.5 MA, R0 = 2.08 m, a = 0.65 m and a pulse duration of 90-100 s. It shall be able to study different divertor magnetic configurations and reach a reactor relevant power flow to the divertor. The proposed mix of heating power foreseen to achieve the target value of 45 MW delivered to the plasma will be provided by Electron Cyclotron Resonant Heating (ECRH), Ion Cyclotron Resonant Heating (ICRH) and Negative-ion-based Neutral Beam Heating (NNBH). In this framework, the conceptual design of a NNBH system for DTT is here presented, with a particular focus on the technical solutions adopted to fulfil the requirements and maximize the performances. The proposed system features two beamlines providing deuterium negative ions (D-) with an energy not smaller than 300 keV and an injected power of 5-8 MW each. The design of the main components of the injectors is described in detail, explaining the motivations behind the main design choices. A comprehensive set of simulations was carried out using several physics and engineering codes to drive the development of the design. These simulations mainly regard the efficiency of the main processes, the optics of the beam, the physics reactions along the beamline (stripping, charge-exchange and ionization), the thermo-mechanical behaviour of the acceleration grids and the coupling between the beam and the plasma in the tokamak chamber.
- Published
- 2018
16. The heating systems capability of DTT
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Granucci Gustavo, Agostinetti Piero, Bolzonella Tommaso, Bruschi Alessandro, Cardinali Alessandro, Castaldo Carmine, Ceccuzzi Silvio, Crisanti Flavio, Figini Lorenzo, Garavaglia Saul, Maggiora Riccardo, Milanesio Daniele, Moro Alessandro, Ravera Gianluca, Sonato Piergiorgio, Tuccillo Angelo Antonio, Vallar Matteo, and Vincenzi Pietro
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ICH ,NNBI ,Negative Neutral Beam Injector ,Ion Cyclotron Heating ,ECH Electron Cyclotron Heating ,Divertor Tokamak Test ,DTT - Abstract
The purpose of the italian Divertor Tokamak Test (DTT, 6 T, 5.5 MA, R0 = 2.08 m, a = 0.65 m for ~ 100 s) is to study power exhaust and divertor load in an integrated plasma scenario. To accomplish this mission DTT will be equipped with 45 MW of additional heating power to fulfill a PSEP/R >= 15 MW/m studing alternative divertor configurations in view of ITER operations and DEMO design. The heating systems considered are NNBI (Negative Neutral Beam Injector), ECH (Electron Cyclotron Heating) and ICH (Ion Cyclotron Heating). Power repartition is based on the physical and functional requirements resulting from the review of the initial design [1]. The ECH is based on the use of 170GHz/1MW gyrotron, exploiting the development done for ITER and the experience of W7-X EC system. To fulfill major requirements assigned to EC waves 20-30 MW at plasma are foreseen. The NNBI system will be based on two beamlines providing deuterium negative ions (D-) at 300 keV and an injected power of 5-8 MW each. To increase efficiency and controllability, a modular approach will be adopted for the ion source and accelerator. The main task of the ICH system is the central deposition in different heating schemes (mode conversion, minority heating and the novel three ions scheme). The frequency range is 60-90 MHz with a coupled power of 5-10 MW depending on the adopted antenna. A high reliability in delivering power to plasma will be obtained considering consolidated and available technologies together with a design architecture capable to reduce the fault risks. An overview of the three systems will be given, with a particular attention to the design integration in the DTT plant and to synergetic aspects between them.
- Published
- 2018
17. Sensitivity of fast ion losses to magnetic perturbations in the European DEMO
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Varje Jari, Kurki-Suonio Taina, Snicker Antti, Särkimäki Konsta, Vincenzi Pietro, Agostinetti Piero, Sonato Piergiorgio, and Villone Fabio
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European DEMO ,Physics::Plasma Physics ,magnetic perturbations ,fast ion losses - Abstract
The limits for the heat loads on the DEMO first wall are significantly stricter compared to those of ITER due to cooling and breeding blanket requirements. In addition to the thermal particle and radiation loads, fast particles in the form of fusion alphas and NBI ions with high energies can escape the confinement due to various magnetic perturbations and produce a significant heat load on the first wall. Previously, the losses of fusion alpha and NBI ions have been found to be manageable, with wall loads remaining below 10% of the limit of 1 MW/m2 envisaged for the DEMO first wall. This is primarily due to the plasma profiles that allow the 800 keV NBI ions to penetrate deep into the plasma before ionizing, and the generous gap of up to 20 cm between the separatrix and the first wall panels. Additionally, only losses due to toroidal field ripple were accounted for, while significant perturbations would be introduced by the possible addition of ELM control coils. In this contribution, we present ASCOT simulation results for fast ion confinement and losses under the effects of additional perturbations, including increased toroidal field ripple due to reduced ferritic inserts and reduced number of toroidal field coils, and the addition of resonant magnetic perturbations (RMP) due to ELM control coils. Additionally, the effect of NBI ionization in the scrape-off layer is discussed, which can introduce localized loads due to high-energy prompt losses.
- Published
- 2018
18. Layout and first measurements of the RING optical cavity for laser NBI photoneutralization
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Vincenzi Pietro, Fassina Alessandro, Giudicotti Leonardo, and Pasqualotto Roberto
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neutral beam insection ,laser NBI photoneutralization ,RING optical cavity ,Physics::Optics ,Physics::Accelerator Physics ,NBI - Abstract
One of the most used systems to heat the plasma to thermonuclear temperatures in fusion experiments is the injection of energetic neutral beams (Neutral Beam Injection - NBI). In the path toward the European demonstrative fusion reactor DEMO, the efficient neutralization of a high energy (~1MeV) negative ion beam in a NBI system is one of the major issues. Current gas neutralizers limit the neutralization efficiency to
- Published
- 2017
19. Innovative H&CD designs and the impact of their configurations on the performance of the EU DEMO fusion power plant reactor
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Franke Thomas, Simonin Alain, Bachmann Christian, Strauss Dirk, Aiello Gaetano, Federici Gianfranco, Giovanni Grossetti, Granucci Gustavo, Noterdaeme Jean-Marie, Jelonnek John, Kostas Avramidis, Tran Minh Quang, Sonato Piergiorgio, Agostinetti Piero, Vincenzi Pietro, Wenninger Ronald, Zheng Shanliang, and Scherer Theo
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Improvements of Heating & Current Drive ,plasma heating and control ,H&CD ,DEMO - Abstract
Improvements of Heating & Current Drive (H&CD) systems are being investigated for a demonstration fusion power plant DEMO to deliver net electricity for the grid around 2050 [1]. Compared to ITER, which has to show the generation of 500 MW thermal power, the target of DEMO is the successful production of 300 to 500 MW electrical power to the grid and to aim for a self-sufficient Tritium fuel cycle [2]. Three H&CD systems are under development for DEMO in Europe, the Electron Cyclotron (EC) System, the Neutral Beam Injection (NBI) System and the Ion Cyclotron (IC) System. Based on present studies [3] for plasma ramp-up, ramp-down and flat top phases, to be further validated in more detailed simulations, the assumed total launched power needed from the H&CD system in DEMO is in the range of 50-100 MW, to be provided for plasma heating and control. Among other topics, the paper describes the new designs and R&D status of H&CD systems considered for their deployment in DEMO in Europe and the impact of the H&CD configurations on their performances based on those areas described in the European fusion electricity roadmap [4] for the integrated design and system development. These configurations encompass the operation of NBI with reduced Caesium consumption, with modular ion sources and improved injector wall-plug efficiencies, EC system with increased gyrotron frequencies above ITER ones, as well as multi-purpose and frequency step-tunable radio frequency sources, and related strategies for the fabrication of large Brewster angle diamond windows, together with EC launcher designs compatible with a fusion power plant environment, avoiding front-steering by using different launcher concepts. The project also elaborates on new solutions to further increase the wall-plug efficiencies of H&CD systems based on more advanced concepts, with the target to reduce the recirculating power fraction in future fusion power plants. Different studies under investigation will be discussed such as, for NBI, the photo-neutralization and, for EC, new concepts for gyrotron multi-stage depressed collector. This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014-2018 under grant agreement No 633053. The views and opinions expressed herein do not necessarily reflect those of the European Commission. With special thanks to whole WPHCD team for the durable, constructive and fruitful collaboration. [1] Federici, G., et al., ´Overview of EU DEMO design and R&D activities´, Fus. Eng. Design, vol. 89, pp. 882-889, 2014 Wenninger, R., et al., 'The physics and technology basis entering European system code studies for DEMO', Nucl. Fusion 57, 016011, 2017 Vincenzi, P., et al, ´EU DEMO transient phases: main constraints and heating mix studies for rampup and ramp-down', SOFT 2016, accepted for publication in Fus. Eng. Design Romanelli, F., et al., ´Fusion electricity: a roadmap to the realisation of fusion energy´, EFDA, Nov. 2012
- Published
- 2017
20. Interaction between neutral beam fast particles and plasma in fusion experiments
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Vincenzi, Pietro
- Subjects
FIS/03 Fisica della materia ,ASCOT ,JINTRAC ,NBI ,heating ,slowing down ,energetic particles ,Settore FIS/03 - Fisica della Materia ,modelling ,stellarator ,FIT3D ,neutral beam injection ,JET ,Physics::Plasma Physics ,METIS ,current drive ,ionization ,TASK3D-a ,fast ions ,LHD ,nuclear fusion, tokamak, stellarator, neutral beam injection, modelling, NBI, JET, LHD, tokamak, ASCOT, PENCIL, METIS, FIT3D, TASK3D-a, JINTRAC, heating, plasma, current drive, fast ions, energetic particles, slowing down, ionization ,tokamak ,PENCIL ,nuclear fusion ,plasma - Abstract
Neutral beam injection (NBI) is one of the most used and reliable methods to heat plasmas in magnetically confined fusion devices. NBI is used in most of the present experiments, it will be used as dominant auxiliary power system in ITER experiment and studies are ongoing for DEMO reactor preconceptual designs with neutral beam (NB) systems. NBI is an essential actuator for plasma scenarios in terms of heating and driven current. This thesis presents the work performed during the 3 years of my Ph.D.. It focuses on numerical studies of the interaction between energetic particles coming from NBI and magnetically confined hot plasmas. The main aspects discussed in this thesis are the neutral beam ionization, fast ion confinement, fast ion losses, power deposition and driven current. A brief discussion of NBI as fuelling source is also presented. NBI modelling tools have been applied to study different devices with dominant NB power: the largest tokamak in operation (JET), the largest helical device in operation (LHD) and DEMO tokamak reactor concept. Detailed modelling of NBI by means of a Monte Carlo orbit following code has been provided for JET discharge analyses. A predictive simulation aimed at reconstructing the ion temperature profile with strong ion heating from NBI has been performed, resulting in a reliable prediction when the experimental measurement was not available due to a diagnostic fault. JET NBI-plasma interaction has been studied by predictive simulations for H discharges starting from reference D discharges in support of JET isotope studies. The isotopic change and the consequent effect on NBI-plasma interaction has been discussed also for LHD helical device, where studies in preparation of future D experiments (instead of H) are ongoing. NBI is one of the options as additional power system for a demonstrative fusion power plant (DEMO), and a pre-conceptual design of the reactor is ongoing within EUROfusion activities. DEMO scenario simulations have been carried out both for pulsed and steady-state concepts. The role of NBI as dominant heating and current drive system has been investigated by sensitivity studies, comparisons with other heating systems and transport investigations of transient phases (plasma ramp-up and ramp-down).
- Published
- 2016
21. Requirements and modelling of fast particle injection in RFX-mod tokamak plasmas
- Author
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Vallar Matteo, Artaud Jean-Francois, Bolzonella Tommaso, Valisa Marco, and Vincenzi Pietro
- Subjects
Physics::Plasma Physics ,Physics::Accelerator Physics - Abstract
The planned upgrade of the RFX-mod device is a good opportunity to widen the operational space of the machine, in both RFP and tokamak configurations. Installation of a power neutral beam injector (NBI) is also envisaged and a NBI system compatible with RFX-mod is already available on site. It was previously installed in TPE-RX (Tsukuba, Japan), it has a nominal power of 1.25 MW, a nominal current of 50A and it can operate at a voltage of 25kV for 30ms (or 15 kV for 100ms). A porthole in the modified vacuum toroidal support structure is planned to be adapted to host this injector, which would operate in the equatorial plane and in a perpendicular direction with respect to the plasma column. This geometry is the only one possible due to mechanical constraints, mainly linked to toroidal field coils configuration.In this work, the METIS simulator is used to study the feasibility of TPE-RX injector integration in RFX-mod tokamak plasmas. METIS code allows the simulation of a full tokamak discharge in a time of the order of a few minutes by using relations coming from scaling laws coupled with simplified source models. The neutral beam injection in METIS is described by a decay equation applied in a simplified geometry and an analytical solution of the Fokker-Planck equation. In order to estimate a set of requirements for an NBI system to be applied to RFX-mod tokamak plasmas the beam shine-through has been carefully considered for a wide range of scenarios. Finally some indications of the physical effects to be expected from NBI-plasma coupling will be highlighted, with special attention to the beam energy absorption (both in terms of time dependent quantities and of spatial profiles) and to the possibility of inducing a transition from L to H confinement modes.
- Published
- 2016
22. Evidence of9Be + pnuclear reactions during 2ωCHand hydrogen minority ICRH in JET-ILW hydrogen and deuterium plasmas
- Author
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Krasilnikov, A. V., Kiptily, V., Lerche, E., Van Eester, D., Afanasyev, V. I., Giroud, C., Goloborodko, V., Hellesen, C., Popovichev, S. V., Mironov, M. I., Litaudon, X., Abduallev, S., Abhangi, M., Abreu, P., Afzal, M., Aggarwal, K. M., Ahlgren, T., Ahn, J. H., Aho Mantila, L., Aiba, N., Airila, M., Albanese, R., Aldred, V., Alegre, D., Alessi, E., Aleynikov, P., Alfier, Alberto, Alkseev, A., Allinson, M., Alper, B., Alves, E., Ambrosino, G., Ambrosino, R., Amicucci, L., Amosov, V., Andersson Sundén, E., Angelone, M., Anghel, M., Angioni, C., Appel, L., Appelbee, C., Arena, P., Ariola, M., Arnichand, H., Arshad, S., Ash, A., Ashikawa, N., Aslanyan, V., Asunta, O., Auriemma, Fulvio, Austin, Y., Avotina, L., Axton, M. D., Ayres, C., Bacharis, M., Baciero, A., Baiã¡o, D., Bailey, S., Baker, A., Balboa, I., Balden, M., Balshaw, N., Bament, R., Banks, J. W., Baranov, Y. F., Barnard, M. A., Barnes, D., Barnes, M., Barnsley, R., Baron Wiechec, A., Barrera Orte, L., Baruzzo, Matteo, Basiuk, V., Bassan, M., Bastow, R., Batista, A., Batistoni, P., Baughan, R., Bauvir, B., Baylor, L., Bazylev, B., Beal, J., Beaumont, P. S., Beckers, M., Beckett, B., Becoulet, A., Bekris, N., Beldishevski, M., Bell, K., Belli, F., Bellinger, M., Belonohy, Ã. ‰., Ben Ayed, N., Benterman, N. A., Bergsã¥ker, H., Bernardo, J., Bernert, M., Berry, M., Bertalot, L., Besliu, C., Beurskens, M., Bieg, B., Bielecki, J., Biewer, T., Bigi, M., Bãlkovã¡, P., Binda, F., Bisoffi, A., Bizarro, J. P. S., Bjã¶rkas, C., Blackburn, J., Blackman, K., Blackman, T. R., Blanchard, P., Blatchford, P., Bobkov, V., Boboc, A., Bodnã¡r, G., Bogar, O., Bolshakova, I., Bolzonella, Tommaso, Bonanomi, N., Bonelli, F., Boom, J., Booth, J., Borba, D., Borodin, D., Borodkina, I., Botrugno, A., Bottereau, C., Boulting, P., Bourdelle, C., Bowden, M., Bower, C., Bowman, C., Boyce, T., Boyd, C., Boyer, H. J., Bradshaw, J. M. A., Braic, V., Bravanec, R., Breizman, B., Bremond, S., Brennan, P. D., Breton, S., Brett, A., Brezinsek, S., Bright, M. D. J., Brix, M., Broeckx, W., Brombin, Matteo, Broså‚awski, A., Brown, D. P. D., Brown, M., Bruno, E., Bucalossi, J., Buch, J., Buchanan, J., Buckley, M. A., Budny, R., Bufferand, H., Bulman, M., Bulmer, N., Bunting, P., Buratti, P., Burckhart, A., Buscarino, A., Busse, A., Butler, N. K., Bykov, I., Byrne, J., Cahyna, P., Calabrã², G., Calvo, I., Camenen, Y., Camp, P., Campling, D. C., Cane, J., Cannas, B., Capel, A. J., Card, P. J., Cardinali, A., Carman, P., Carr, M., Carralero, D., Carraro, L., Carvalho, B. B., Carvalho, I., Carvalho, P., Casson, F. J., Castaldo, C., Catarino, N., Caumont, J., Causa, F., Cavazzana, R., Cave Ayland, K., Cavinato, M., Cecconello, M., Ceccuzzi, S., Cecil, E., Cenedese, Angelo, Cesario, R., Challis, C. D., Chandler, M., Chandra, D., Chang, C. S., Chankin, A., Chapman, I. T., Chapman, S. C., Chernyshova, M., Chitarin, Giuseppe, Ciraolo, G., Ciric, D., Citrin, J., Clairet, F., Clark, E., Clark, M., Clarkson, R., Clatworthy, D., Clements, C., Cleverly, M., Coad, J. P., Coates, P. A., Cobalt, A., Coccorese, V., Cocilovo, V., Coda, S., Coelho, R., Coenen, J. W., Coffey, I., Colas, L., Collins, S., Conka, D., Conroy, S., Conway, N., Coombs, D., Cooper, D., Cooper, S. R., Corradino, C., Corre, Y., Corrigan, G., Cortes, S., Coster, D., Couchman, A. S., Cox, M. P., Craciunescu, T., Cramp, S., Craven, R., Crisanti, F., Croci, G., Croft, D., Crombã©, K., Crowe, R., Cruz, N., Cseh, G., Cufar, A., Cullen, A., Curuia, M., Czarnecka, A., Dabirikhah, H., Dalgliesh, P., Dalley, S., Dankowski, J., Darrow, D., Davies, O., Davis, W., Day, C., Day, I. E., De Bock, M., De Castro, A., De La Cal, E., De La Luna, E., De Masi, G., De Pablos, J. L., De Temmerman, G., De Tommasi, G., De Vries, P., Deakin, K., Deane, J., Degli Agostini, F., Dejarnac, R., Delabie, E., Den Harder, N., Dendy, R. O., Denis, J., Denner, P., Devaux, S., Devynck, P., Di Maio, F., Di Siena, A., Di Troia, C., Dinca, P., D'Inca, R., Ding, B., Dittmar, T., Doerk, H., Doerner, R. P., Donnã©, T., Dorling, S. E., Dormido Canto, S., Doswon, S., Douai, D., Doyle, P. T., Drenik, A., Drewelow, P., Drews, P., Duckworth, P. h., Dumont, R., Dumortier, P., Dunai, D., Dunne, M., Äžuran, I., Durodiã©, F., Dutta, P., Duval, B. P., Dux, R., Dylst, K., Dzysiuk, N., Edappala, P. V., Edmond, J., Edwards, A. M., Edwards, J., Eich, T. h., Ekedahl, A., El Jorf, R., Elsmore, C. G., Enachescu, M., Ericsson, G., Eriksson, F., Eriksson, J., Eriksson, L. G., Esposito, B., Esquembri, S., Esser, H. G., Esteve, D., Evans, B., Evans, G. E., Evison, G., Ewart, G. D., Fagan, D., Faitsch, M., Falie, D., Fanni, A., Fasoli, A., Faustin, J. M., Fawlk, N., Fazendeiro, L., Fedorczak, N., Felton, R. C., Fenton, K., Fernades, A., Fernandes, H., Ferreira, J., Fessey, J. A., Fã©vrier, O., Ficker, O., Field, A., Fietz, S., Figueiredo, A., Figueiredo, J., Fil, A., Finburg, P., Firdaouss, M., Fischer, U., Fittill, L., Fitzgerald, M., Flammini, D., Flanagan, J., Fleming, C., Flinders, K., Fonnesu, N., Fontdecaba, J. M., Formisano, A., Forsythe, L., Fortuna, L., Fortuna Zalesna, E., Fortune, M., Foster, S., Franke, T., Franklin, T., Frasca, M., Frassinetti, L., Freisinger, M., Fresa, R., Frigione, D., Fuchs, V., Fuller, D., Futatani, S., Fyvie, J., Gã¡l, K., Galassi, D., Gaå‚azka, K., Galdon Quiroga, J., Gallagher, J., Gallart, D., Galvã¡o, R., Gao, X., Gao, Y., Garcia, J., Garcia Carrasco, A., GarcÃa Muñoz, M., Gardarein, J. L., Garzotti, L., Gaudio, P., Gauthier, E., Gear, D. F., Gee, S. J., Geiger, B., Gelfusa, M., Gerasimov, S., Gervasini, G., Gethins, M., Ghani, Z., Ghate, M., Gherendi, M., Giacalone, J. C., Giacomelli, L., Gibson, C. S., Giegerich, T., Gil, C., Gil, L., Gilligan, S., Gin, D., Giovannozzi, E., Girardo, J. B., Giruzzi, Gerardo, Glã¶ggler, S., Godwin, J., Goff, J., Gohil, P., Goloborod'Ko, V., Gomes, R., Goncalves, B., Goniche, M., Goodliffe, M., Goodyear, A., Gorini, G., Gosk, M., Goulding, R., Goussarov, A., Gowland, R., Graham, B., Graham, M. E., Graves, J. P., Grazier, N., Grazier, P., Green, N. R., Greuner, H., Grierson, B., Griph, F. S., Grisolia, C., Grist, D., Groth, M., Grove, R., Grundy, C. N., Grzonka, J., Guard, D., Guã©rard, C., Guillemaut, C., Guirlet, R., Gurl, C., Utoh, H. H., Hackett, L. J., Hacquin, S., Hagar, A., Hager, R., Hakola, A., Halitovs, M., Hall, S. J., Hallworth Cook, S. P., Hamlyn Harris, C., Hammond, K., Harrington, C., Harrison, J., Harting, D., Hasenbeck, F., Hatano, Y., Hatch, D. R., Haupt, T. D. V., Hawes, J., Hawkes, N. C., Hawkins, J., Hawkins, P., Haydon, P. W., Hayter, N., Hazel, S., Heesterman, P. J. L., Heinola, K., Hellsten, T., Helou, W., Hemming, O. N., Hender, T. C., Henderson, M., Henderson, S. S., Henriques, R., Hepple, D., Hermon, G., Hertout, P., Hidalgo, C., Highcock, E. G., Hill, M., Hillairet, J., Hillesheim, J., Hillis, D., Hizanidis, K., Hjalmarsson, A., Hobirk, J., Hodille, E., Hogben, C. H. A., Hogeweij, G. M. D., Hollingsworth, A., Hollis, S., Homfray, D. A., Horã¡ä ek, J., Hornung, G., Horton, A. R., Horton, L. D., Horvath, L., Hotchin, S. P., Hough, M. R., Howarth, P. J., Hubbard, A., Huber, A., Huber, V., Huddleston, T. M., Hughes, M., Huijsmans, G. T. A., Hunter, C. L., Huynh, P., Hynes, A. M., Iglesias, D., Imazawa, N., Imbeaux, F., Imrãå¡ek, M., Incelli, M., Innocente, P., Irishkin, M., Ivanova Stanik, I., Jachmich, S., Jacobsen, A. S., Jacquet, P., Jansons, J., Jardin, A., Jã¤rvinen, A., Jaulmes, F., Jednorã³g, S., Jenkins, I., Jeong, C., Jepu, I., Joffrin, E., Johnson, R., Johnson, T., Johnston, Jane, Joita, L., Jones, G., Jones, T. T. C., Hoshino, K. K., Kallenbach, A., Kamiya, K., Kaniewski, J., Kantor, A., Kappatou, A., Karhunen, J., Karkinsky, D., Karnowska, I., Kaufman, M., Kaveney, G., Kazakov, Y., Kazantzidis, V., Keeling, D. L., Keenan, T., Keep, J., Kempenaars, M., Kennedy, C., Kenny, D., Kent, J., Kent, O. N., Khilkevich, E., Kim, H. T., Kim, H. S., Kinch, A., King, C., King, D., King, R. F., Kinna, D. J., Kirk, A., Kirov, K., Kirschner, A., Kizane, G., Klepper, C., Klix, A., Knight, P., Knipe, S. J., Knott, S., Kobuchi, T., Kã¶chl, F., Kocsis, G., Kodeli, I., Kogan, L., Kogut, D., Koivuranta, S., Kominis, Y., Kã¶ppen, M., Kos, B., Koskela, T., Koslowski, H. R., Koubiti, M., Kovari, M., Kowalska StrzÈ©ciwilk, E., Krasilnikov, A., Krasilnikov, V., Krawczyk, N., Kresina, M., Krieger, K., Krivska, A., Kruezi, U., Ksiaå¼ek, I., Kukushkin, A., Kundu, A., Kurki Suonio, T., Kwak, S., Kwiatkowski, R., Kwon, O. J., Laguardia, L., Lahtinen, A., Laing, A., Lam, N., Lambertz, H. T., Lane, C., Lang, P. T., Lanthaler, S., Lapins, J., Lasa, A., Last, J. R., Å aszyå„ska, E., Lawless, R., Lawson, A., Lawson, K. D., Lazaros, A., Lazzaro, E., Leddy, J., Lee, S., Lefebvre, X., Leggate, H. J., Lehmann, J., Lehnen, M., Leichtle, D., Leichuer, P., Leipold, F., Lengar, I., Lennholm, M., Lescinskis, A., Lesnoj, S., Letellier, E., Leyland, M., Leysen, W., Li, L., Liang, Y., Likonen, J., Linke, J., Linsmeier, C. h., Lipschultz, B., Liu, G., Liu, Y., Lo Schiavo, V. P., Loarer, T., Loarte, A., Lobel, R. C., Lomanowski, B., Lomas, P. J., Lã¶nnroth, J., Lã³pez, J. M., López Razola, J., Lorenzini, R., Losada, U., Lovell, J. J., Loving, A. B., Lowry, C., Luce, T., Lucock, R. M. A., Lukin, A., Luna, C., Lungaroni, M., Lungu, C. P., Lungu, M., Lunniss, A., Lupelli, I., Lyssoivan, A., Macdonald, N., Macheta, P., Maczewa, K., Magesh, B., Maget, P., Maggi, C., Maier, H., Mailloux, J., Makkonen, T., Makwana, R., Malaquias, A., Malizia, A., Manas, P., Manning, A., Manso, M. E., Mantica, P., Mantsinen, M., Manzanares, A., Maquet, P. h., Marandet, Y., Marcenko, N., Marchetto, C., Marchuk, O., Marinelli, M., Marinucci, M., Markoviä, T., Marocco, D., Marot, L., Marren, C. A., Marshal, R., Martin, A., Martin, Y., MartÃn De Aguilera, A., Martãnez, F. J., MartÃn SolÃs, J. R., Martynova, Y., Maruyama, S., Masiello, A., Maslov, M., Matejcik, S., Mattei, M., Matthews, G. F., Maviglia, F., Mayer, M., Mayoral, M. L., May Smith, T., Mazon, D., Mazzotta, C., Mcadams, R., Mccarthy, P. J., Mcclements, K. G., Mccormack, O., Mccullen, P. A., Mcdonald, D., Mcintosh, S., Mckean, R., Mckehon, J., Meadows, R. C., Meakins, A., Medina, F., Medland, M., Medley, S., Meigh, S., Meigs, A. G., Meisl, G., Meitner, S., Meneses, L., Menmuir, S., Mergia, K., Merrigan, I. R., Mertens, P. h., Meshchaninov, S., Messiaen, A., Meyer, H., Mianowski, S., Michling, R., Middleton Gear, D., Miettunen, J., Militello, F., Militello Asp, E., Miloshevsky, G., Mink, F., Minucci, S., Miyoshi, Y., Mlynã¡å™, J., Molina, D., Monakhov, I., Moneti, M., Mooney, R., Moradi, S., Mordijck, S., Moreira, L., Moreno, R., Moro, F., Morris, A. W., Morris, J., Moser, L., Mosher, S., Moulton, D., Murari, A., Muraro, A., Murphy, S., Asakura, N. N., Y. S., Na, Nabais, F., Naish, R., Nakano, T., Nardon, E., Naulin, V., Nave, M. F. F., Nedzelski, I., Nemtsev, G., Nespoli, F., Neto, A., Neu, R., Neverov, V. S., Newman, M., Nicholls, K. J., Nicolas, T., Nielsen, A. H., Nielsen, P., Nilsson, E., Nishijima, D., Noble, C., Nocente, M., Nodwell, D., Nordlund, K., Nordman, H., Nouailletas, R., Nunes, I., Oberkofler, M., Odupitan, T., Ogawa, M. T., O'Gorman, T., Okabayashi, M., Olney, R., Omolayo, O., O'Mullane, M., Ongena, J., Orsitto, F., Orszagh, J., Oswuigwe, B. I., Otin, R., Owen, A., Paccagnella, R., Pace, N., Pacella, D., Packer, L. W., Page, A., Pajuste, E., Palazzo, S., Pamela, S., Panja, S., Papp, P., Paprok, R., Parail, V., Park, M., Parra Diaz, F., Parsons, M., Pasqualotto, R., Patel, A., Pathak, S., Paton, D., Patten, H., Pau, A., Pawelec, E., Paz Soldan, C., Peackoc, A., Pearson, I. J., Pehkonen, S. P., Peluso, E., Penot, C., Pereira, A., Pereira, R., Pereira Puglia, P. P., Perez Von Thun, C., Peruzzo, S., Peschanyi, S., Peterka, M., Petersson, P., Petravich, G., Petre, A., Petrella, N., Petrå¾ilka, V., Peysson, Y., Pfefferlã©, D., Philipps, V., Pillon, M., Pintsuk, G., Piovesan, P., Pires Dos Reis, A., Piron, Lidia, Pironti, A., Pisano, F., Pitts, R., Pizzo, F., Plyusnin, V., Pomaro, N., Pompilian, O. G., Pool, P. J., Popovichev, S., Porfiri, M. T., Porosnicu, C., Porton, M., Possnert, G., Potzel, S., Powell, T., Pozzi, J., Prajapati, V., Prakash, R., Prestopino, G., Price, D., Price, M., Price, R., Prior, P., Proudfoot, R., Pucella, G., Puglia, P., Puiatti, M. E., Pulley, D., Purahoo, K., Pã¼tterich, T. h., Rachlew, E., Rack, M., Ragona, R., Rainford, M. S. J., Rakha, A., Ramogida, G., Ranjan, S., Rapson, C. J., Rasmussen, J. J., Rathod, K., Rattã¡, G., Ratynskaia, S., Ravera, G., Rayner, C., Rebai, M., Reece, D., Reed, A., Rã©fy, D., Regan, B., Regaã±a, J., Reich, M., Reid, N., Reimold, F., Reinhart, M., Reinke, M., Reiser, D., Rendell, D., Reux, C., Reyes Cortes, S. D. A., Reynolds, S., Riccardo, V., Richardson, N., Riddle, K., Rigamonti, D., Rimini, F. G., Risner, J., Riva, M., Roach, C., Robins, R. J., Robinson, S. A., Robinson, T., Robson, D. W., Roccella, R., Rodionov, R., Rodrigues, P., Rodriguez, J., Rohde, V., Romanelli, F., Romanelli, M., Romanelli, S., Romazanov, J., Rowe, S., Rubel, M., Rubinacci, G., Rubino, G., Ruchko, L., Ruiz, M., Ruset, C., Rzadkiewicz, J., Saarelma, S., Sabot, R., Safi, E., Sagar, P., Saibene, G., Saint Laurent, F., Salewski, M., Salmi, A., Salmon, R., Salzedas, F., Samaddar, D., Samm, U., Sandiford, D., Santa, P., Santala, M. I. K., Santos, B., Santucci, A., Sartori, F., Sartori, R., Sauter, O., Scannell, R., Schlummer, T., Schmid, K., Schmidt, V., Schmuck, S., Schneider, M., Schã¶pf, K., Schwã¶rer, D., Scott, S. D., Sergienko, G., Sertoli, M., Shabbir, A., Sharapov, S. E., Shaw, A., Shaw, R., Sheikh, H., Shepherd, A., Shevelev, A., Shumack, A., Sias, G., Sibbald, M., Sieglin, B., Silburn, S., Silva, A., Silva, C., Simmons, P. A., Simpson, J., Simpson Hutchinson, J., Sinha, A., Sipilã¤, S. K., Sips, A. C. C., Sirã©n, P., Sirinelli, A., Sjã¶strand, H., Skiba, M., Skilton, R., Slabkowska, K., Slade, B., Smith, N., Smith, P. G., Smith, R., Smith, T. J., Smithies, M., Snoj, L., Soare, S., Solano, E. R., Somers, A., Sommariva, C., Sonato, Piergiorgio, Sopplesa, A., Sousa, J., Sozzi, C., Spagnolo, Silvia, Spelzini, T., Spineanu, F., Stables, G., Stamatelatos, I., Stamp, M. F., Staniec, P., Stankå«nas, G., Stan Sion, C., Stead, M. J., Stefanikova, E., Stepanov, I., Stephen, A. V., Stephen, M., Stevens, A., Stevens, B. D., Strachan, J., Strand, P., Strauss, H. R., Strã¶m, P., Stubbs, G., Studholme, W., Subba, F., Summers, H. P., Svensson, J., Åšwiderski, Å., Szabolics, T., Szawlowski, M., Szepesi, G., Suzuki, T. T., Tã¡l, B., Tala, T., Talbot, A. R., Talebzadeh, S., Taliercio, Cesare, Tamain, P., Tame, C., Tang, W., Tardocchi, M., Taroni, L., Taylor, D., Taylor, K. A., Tegnered, D., Telesca, G., Teplova, N., Terranova, David, Testa, D., Tholerus, E., Thomas, J., Thomas, J. D., Thomas, P., Thompson, A., Thompson, C. A., Thompson, V. K., Thorne, L., Thornton, A., Thrysã¸e, A. S., Tigwell, P. A., Tipton, N., Tiseanu, I., Tojo, H., Tokitani, M., Tolias, P., Tomeå¡, M., Tonner, P., Towndrow, M., Trimble, P., Tripsky, M., Tsalas, M., Tsavalas, P., Tskhakaya Jun, D., Turner, I., Turner, M. M., Turnyanskiy, M., Tvalashvili, G., Tyrrell, S. G. J., Uccello, A., Ul Abidin, Z., Uljanovs, J., Ulyatt, D., Urano, H., Uytdenhouwen, I., Vadgama, A. P., Valcarcel, D., Valentinuzzi, M., Valisa, M., Vallejos Olivares, P., Valovic, M., Van De Mortel, M., Van Renterghem, W., Van Rooij, G. J., Varje, J., Varoutis, S., Vartanian, S., Vasava, K., Vasilopoulou, T., Vega, J., Verdoolaege, G., Verhoeven, R., Verona, C., Verona Rinati, G., Veshchev, E., Vianello, N., Vicente, J., Viezzer, E., Villari, S., Villone, F., Vincenzi, Pietro, Vinyar, I., Viola, B., Vitins, A., Vizvary, Z., Vlad, M., Voitsekhovitch, I., Vondrã¡ä ek, P., Vora, N., Vu, T., Pires De Sa, W. 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V., Kiptily, V., Lerche, E., Van Eester, D., Afanasyev, V. I., Giroud, C., Goloborodko, V., Hellesen, C., Popovichev, S. V., Mironov, M. I., Litaudon, X., Abduallev, S., Abhangi, M., Abreu, P., Afzal, M., Aggarwal, K. M., Ahlgren, T., Ahn, J. H., Aho-Mantila, L., Aiba, N., Airila, M., Albanese, R., Aldred, V., Alegre, D., Alessi, E., Aleynikov, P., Alfer, A., Alkseev, A., Allinson, M., Alper, B., Alves, E., Ambrosino, G., Ambrosino, R., Amicucci, L., Amosov, V., Sunden, E. A., Angelone, M., Anghel, M., Angioni, C., Appel, L., Appelbee, C., Arena, P., Ariola, M., Arnichand, H., Arshad, S., Ash, A., Ashikawa, N., Aslanyan, V., Asunta, O., Auriemma, F., Austin, Y., Avotina, L., Axton, M. D., Ayres, C., Bacharis, M., Baciero, A., Baiao, D., Bailey, S., Baker, A., Balboa, I., Balden, M., Balshaw, N., Bament, R., Banks, J. W., Baranov, Y. F., Barnard, M. A., Barnes, D., Barnes, M., Barnsley, R., Wiechec, A. B., Orte, L. 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D., Breton, S., Brett, A., Brezinsek, S., Bright, M. D. J., Brix, M., Broeckx, W., Brombin, M., Brosfawski, A., Brown, D. P. D., Brown, M., Bruno, E., Bucalossi, J., Buch, J., Buchanan, J., Buckley, M. A., Budny, R., Bufferand, H., Bulman, M., Bulmer, N., Bunting, P., Buratti, P., Burckhart, A., Buscarino, A., Busse, A., Butler, N. K., Bykov, I., Byrne, J., Cahyna, P., Calabro, G., Calvo, I., Camenen, Y., Camp, P., Campling, D. C., Cane, J., Cannas, B., Capel, A. J., Card, P. J., Cardinali, A., Carman, P., Carr, M., Carralero, D., Carraro, L., Carvalho, B. B., Carvalho, I., Carvalho, P., Casson, F. J., Castaldo, C., Catarino, N., Caumont, J., Causa, F., Cavazzana, R., Cave-Ayland, K., Cavinato, M., Cecconello, M., Ceccuzzi, S., Cecil, E., Cenedese, A., Cesario, R., Challis, C. D., Chandler, M., Chandra, D., Chang, C. S., Chankin, A., Chapman, I. T., Chapman, S. 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A., Fevrier, O., Ficker, O., Field, A., Fietz, S., Figueiredo, A., Figueiredo, J., Fil, A., Finburg, P., Firdaouss, M., Fischer, U., Fittill, L., Fitzgerald, M., Flammini, D., Flanagan, J., Fleming, C., Flinders, K., Fonnesu, N., Fontdecaba, J. M., Formisano, A., Forsythe, L., Fortuna, L., Fortuna-Zalesna, E., Fortune, M., Foster, S., Franke, T., Franklin, T., Frasca, M., Frassinetti, L., Freisinger, M., Fresa, R., Frigione, D., Fuchs, V., Fuller, D., Futatani, S., Fyvie, J., Gal, K., Galassi, D., Gafqzka, K., Galdon-Quiroga, J., Gallagher, J., Gallart, D., Galvao, R., Gao, X., Gao, Y., Garcia, J., Garcia-Carrasco, A., Garcia-Munoz, M., Gardarein, J. -L., Garzotti, L., Gaudio, P., Gauthier, E., Gear, D. F., Gee, S. J., Geiger, B., Gelfusa, M., Gerasimov, S., Gervasini, G., Gethins, M., Ghani, Z., Ghate, M., Gherendi, M., Giacalone, J. C., Giacomelli, L., Gibson, C. S., Giegerich, T., Gil, C., Gil, L., Gilligan, S., Gin, D., Giovannozzi, E., Girardo, J. 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E., Mantica, P., Mantsinen, M., Manzanares, A., Maquet, Ph., Marandet, Y., Marcenko, N., Marchetto, C., Marchuk, O., Marinelli, M., Marinucci, M., Markovic, T., Marocco, D., Marot, L., Marren, C. A., Marshal, R., Martin, A., Martin, Y., De Aguilera, A. M., Martinez, F. J., Martin-Solis, J. R., Martynova, Y., Maruyama, S., Masiello, A., Maslov, M., Matejcik, S., Mattei, M., Matthews, G. F., Maviglia, F., Mayer, M., Mayoral, M. L., May-Smith, T., Mazon, D., Mazzotta, C., Mcadams, R., Mccarthy, P. J., Mcclements, K. G., Mccormack, O., Mccullen, P. A., Mcdonald, D., Mcintosh, S., Mckean, R., Mckehon, J., Meadows, R. C., Meakins, A., Medina, F., Medland, M., Medley, S., Meigh, S., Meigs, A. G., Meisl, G., Meitner, S., Meneses, L., Menmuir, S., Mergia, K., Merrigan, I. 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W., Roccella, R., Rodionov, R., Rodrigues, P., Rodriguez, J., Rohde, V., Romanelli, F., Romanelli, M., Romanelli, S., Romazanov, J., Rowe, S., Rubel, M., Rubinacci, G., Rubino, G., Ruchko, L., Ruiz, M., Ruset, C., Rzadkiewicz, J., Saarelma, S., Sabot, R., Saf, E., Sagar, P., Saibene, G., Saint-Laurent, F., Salewski, M., Salmi, A., Salmon, R., Salzedas, F., Samaddar, D., Samm, U., Sandiford, D., Santa, P., Santala, M. I. K., Santos, B., Santucci, A., Sartori, F., Sartori, R., Sauter, O., Scannell, R., Schlummer, T., Schmid, K., Schmidt, V., Schmuck, S., Schneider, M., Schopf, K., Schworer, D., Scott, S. D., Sergienko, G., Sertoli, M., Shabbir, A., Sharapov, S. E., Shaw, A., Shaw, R., Sheikh, H., Shepherd, A., Shevelev, A., Shumack, A., Sias, G., Sibbald, M., Sieglin, B., Silburn, S., Silva, A., Silva, C., Simmons, P. A., Simpson, J., Simpson-Hutchinson, J., Sinha, A., Sipila, S. K., Sips, A. C. 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- Subjects
Nuclear reaction ,Nuclear and High Energy Physics ,Materials science ,Hydrogen ,beryllium ,proton ,nuclear reactions ,ICRH ,alpha-particles ,Population ,chemistry.chemical_element ,nuclear reaction ,01 natural sciences ,7. Clean energy ,010305 fluids & plasmas ,Ion ,0103 physical sciences ,Nuclear fusion ,education ,Neutral particle ,010302 applied physics ,education.field_of_study ,alpha-particle ,Alpha particle ,Condensed Matter Physics ,Settore ING-IND/20 - Misure e Strumentazione Nucleari ,Deuterium ,chemistry ,Atomic physics - Abstract
The intensity of 9Be + p nuclear fusion reactions was experimentally studied during second harmonic (2ω CH) ion-cyclotron resonance heating (ICRH) and further analyzed during fundamental hydrogen minority ICRH of JET-ILW hydrogen and deuterium plasmas. In relatively low-density plasmas with a high ICRH power, a population of fast H+ ions was created and measured by neutral particle analyzers. Primary and secondary nuclear reaction products, due to 9Be + p interaction, were observed with fast ion loss detectors, γ-ray spectrometers and neutron flux monitors and spectrometers. The possibility of using 9Be(p, d)2α and 9Be(p, α)6Li nuclear reactions to create a population of fast alpha particles and study their behaviour in non-active stage of ITER operation is discussed in the paper.
- Published
- 2018
- Full Text
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