Conceptual design of the beam source for the DEMO Neutral Beam Injectors

DEMO (DEMOnstration Fusion Power Plant) is a proposed nuclear fusion power plant that is intended to follow the ITER experimental reactor. The main goal of DEMO will be to demonstrate the possibility to produce electric energy from the fusion reaction. The injection of high energy neutral beams is one of the main tools to heat the plasma up to fusion conditions. A conceptual design of the Neutral Beam Injector (NBI) for the DEMO fusion reactor, is currently being developed by Consorzio RFX in collaboration with other European research institutes. High efficiency and low recirculating power, which are fundamental requirements for the success of DEMO, have been taken into special consideration for the DEMO NBI. Moreover, particular attention has been paid to the issues related to reliability, availability, maintainability and inspectability. A conceptual design of the beam source for the DEMO NBI is here presented featuring 20 sub-sources (two adjacent columns of 10 sub-sources each), following a modular design concept, with each sub-source featuring its radio frequency driver, capable of increasing the reliability and availability of the DEMO NBI. Copper grids with increasing size of the apertures have been adopted in the accelerator, with three main layouts of the apertures (circular apertures, slotted apertures and frame-like apertures for each sub-source). This design, permitting to significantly decrease the stripping losses in the accelerator without spoiling the beam optics, has been investigated with a self-consistent model able to study at the same time the magnetic field, the electrostatic field and the trajectory of the negative ions. Moreover, the status on the R&D carried out in Europe on the ion sources is presented.

[1]  R. S. Hemsworth,et al.  Gas flow and related beam losses in the ITER neutral beam injector , 2006 .

[2]  P. Garibaldi,et al.  R&D around a photoneutralizer-based NBI system (Siphore) in view of a DEMO Tokamak steady state fusion reactor , 2015, 1911.12210.

[3]  P. Zaccaria,et al.  Physics and engineering design of the accelerator and electron dump for SPIDER , 2011 .

[4]  B. Heinemann,et al.  First experiments with Cs doped Mo as surface converter for negative hydrogen ion sources , 2015 .

[5]  C. Martens,et al.  Physical performance analysis and progress of the development of the negative ion RF source for the ITER NBI system , 2009 .

[6]  Masaki Osakabe,et al.  High-power and long-pulse injection with negative-ion-based neutral beam injectors in the Large Helical Device , 2006 .

[7]  B. P. Duval,et al.  A novel helicon plasma source for negative ion beams for fusion , 2016 .

[8]  U. Fantz,et al.  Investigation of Helicon discharges as RF coupling concept of negative hydrogen ion sources , 2013 .

[9]  Julien Hillairet,et al.  Technological and physics assessments on heating and current drive systems for DEMO , 2015 .

[10]  U. Fantz,et al.  Comparison of the B field dependency of plasma parameters of a weakly magnetized inductive and Helicon hydrogen discharge , 2016 .

[11]  Emanuele Sartori,et al.  AVOCADO: A numerical code to calculate gas pressure distribution , 2013 .

[12]  David Ward,et al.  Modelling of pulsed and steady-state DEMO scenarios , 2015 .

[13]  R. S. Hemsworth,et al.  Detailed design optimization of the MITICA negative ion accelerator in view of the ITER NBI , 2015 .

[14]  Nicola Pilan,et al.  Magnetic Field Effect on Voltage Holding in the MITICA Electrostatic Accelerator , 2014, IEEE Transactions on Plasma Science.

[15]  Masaki Osakabe,et al.  Compensation of beam deflection due to the magnetic field using beam steering by aperture displacement technique in the multibeamlet negative ion source , 2001 .

[16]  H. D. Esch,et al.  SINGAP: The European concept for negative ion acceleration in the ITER neutral injectors , 2002 .

[17]  T. Giegerich,et al.  Conceptuation of a continuously working vacuum pump train for fusion power plants , 2013 .

[18]  R Pasqualotto,et al.  A feasibility study of a NBI photoneutralizer based on nonlinear gating laser recirculation. , 2016, The Review of scientific instruments.

[19]  P. Guittienne,et al.  Towards an optimal antenna for helicon waves excitation , 2005 .

[20]  R. S. Hemsworth,et al.  Compensations of beamlet deflections for 1 MeV accelerator of ITER NBI , 2013 .

[21]  J. D. Evans,et al.  Low-field helicon discharges , 1997 .

[22]  R. S. Hemsworth,et al.  Updated physics design ITER-SINGAP accelerator , 2005 .

[23]  Roderick Boswell Very efficient plasma generation by whistler waves near the lower hybrid frequency , 1984 .

[24]  D. Aprile,et al.  Cancellation of the ion deflection due to electron-suppression magnetic field in a negative-ion accelerator. , 2014, The Review of scientific instruments.

[25]  B. Heinemann,et al.  Large-area radio frequency plasma sources for fusion applications , 1998 .

[26]  B Heinemann,et al.  Long pulse large area beam extraction with a rf driven H(-)/D(-) source. , 2008, The Review of scientific instruments.

[27]  G. Granucci,et al.  On the present status of the EU demo H&CD systems, technology, functions and mix , 2015, 2015 IEEE 26th Symposium on Fusion Engineering (SOFE).

[28]  V. Toigo,et al.  Progress in the realization of the PRIMA neutral beam test facility , 2015 .