Physics and engineering design of the accelerator and electron dump for SPIDER

The ITER Neutral Beam Test Facility (PRIMA) is planned to be built at Consorzio RFX (Padova, Italy). PRIMA includes two experimental devices: a full size ion source with low voltage extraction called SPIDER and a full size neutral beam injector at full beam power called MITICA. SPIDER is the first experimental device to be built and operated, aiming at testing the extraction of a negative ion beam (made of H− and in a later stage D− ions) from an ITER size ion source. The main requirements of this experiment are a H−/D− extracted current density larger than 355/285 A m−2, an energy of 100 keV and a pulse duration of up to 3600 s.Several analytical and numerical codes have been used for the design optimization process, some of which are commercial codes, while some others were developed ad hoc. The codes are used to simulate the electrical fields (SLACCAD, BYPO, OPERA), the magnetic fields (OPERA, ANSYS, COMSOL, PERMAG), the beam aiming (OPERA, IRES), the pressure inside the accelerator (CONDUCT, STRIP), the stripping reactions and transmitted/dumped power (EAMCC), the operating temperature, stress and deformations (ALIGN, ANSYS) and the heat loads on the electron dump (ED) (EDAC, BACKSCAT).An integrated approach, taking into consideration at the same time physics and engineering aspects, has been adopted all along the design process. Particular care has been taken in investigating the many interactions between physics and engineering aspects of the experiment. According to the 'robust design' philosophy, a comprehensive set of sensitivity analyses was performed, in order to investigate the influence of the design choices on the most relevant operating parameters.The design of the SPIDER accelerator, here described, has been developed in order to satisfy with reasonable margin all the requirements given by ITER, from the physics and engineering points of view. In particular, a new approach to the compensation of unwanted beam deflections inside the accelerator and a new concept for the ED have been introduced.

[1]  H. D. Esch,et al.  Electron dumps for ITER HNB and DNB beamlines , 2010 .

[2]  G. Serianni,et al.  Design and analyses of a one-dimensional CFC calorimeter for SPIDER beam characterisation , 2010 .

[3]  William B. Herrmannsfeldt,et al.  ELECTRON TRAJECTORY PROGRAM , 1979 .

[4]  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 .

[5]  R. S. Hemsworth,et al.  Modeling of secondary emission processes in the negative ion based electrostatic accelerator of the International Thermonuclear Experimental Reactor , 2008 .

[6]  T. Kulevoy,et al.  Development of Small Multiaperture Negative Ion Beam Sources and Related Simulation Tools , 2009 .

[7]  P. Spädtke Numerical simulation of ion beam related problems (invited) , 1992 .

[8]  Andrea Rizzolo,et al.  Detail design of the beam source for the SPIDER experiment , 2010 .

[9]  C. Martens,et al.  Overview of the RF source development programme at IPP Garching , 2006 .

[10]  M J Singh,et al.  Physics design of a 100 keV acceleration grid system for the diagnostic neutral beam for international tokamak experimental reactor. , 2010, The Review of scientific instruments.

[11]  A. Bejan,et al.  Heat transfer handbook , 2003 .

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

[13]  C. Martens,et al.  Development of a RF-driven ion source for the ITER NBI system , 2009 .

[14]  Y. Yamashita,et al.  Investigation of beam deflection reduction and multi-beamlet focus at a large-area negative ion source for a neutral beam injector with 3-D beam trajectory simulation , 2000 .

[15]  L. Grisham,et al.  Beamlet deflection due to beamlet-beamlet interaction in a large-area multiaperture negative ion source for JT-60U. , 2008, The Review of scientific instruments.

[16]  U. Fantz,et al.  Long pulse H- beam extraction with a rf driven ion source on a high power level. , 2010, The Review of scientific instruments.

[17]  R. S. Hemsworth,et al.  Design of neutral beam system for ITER-FEAT , 2001 .

[18]  O. Kaneko,et al.  Multibeamlet focusing of intense negative ion beams by an aperture displacement technique , 1995 .

[19]  V. Antoni,et al.  IRES: a code evaluating the beamlet beamlet interaction for multi-aperture electrostatic accelerators , 2009, 2009 23rd IEEE/NPSS Symposium on Fusion Engineering.

[20]  E. Hooper Large Ion Beams: Fundamentals of Generation and Propagation , 1990 .

[21]  Nicola Pilan,et al.  Simulation, code benchmarking and optimization of the magnetic field configuration in a Negative Ion Accelerator , 2011 .

[22]  U. Fantz,et al.  Physical and Experimental Background of the Design of the ELISE Test Facility , 2009 .

[23]  G. Fubiani,et al.  Analysis of the two accelerator concepts foreseen for the neutral beam injector of the International Thermonuclear Experimental Reactor , 2009 .

[24]  G. Serianni,et al.  Negative Ion Extraction With Finite Element Solvers and Ray Maps , 2008, IEEE Transactions on Plasma Science.

[25]  Kazuhiro Watanabe,et al.  Beamlet–beamlet interaction in a multi-aperture negative ion source , 2000 .

[26]  Ernest J. Sternglass,et al.  Backscattering of Kilovolt Electrons from Solids , 1954 .

[27]  T. Matsukawa,et al.  Measurements of the energy distribution of backscattered kilovolt electrons with a spherical retarding-field energy analyser , 1974 .

[28]  E. Thompson,et al.  Beam steering in tetrode extraction systems , 1981 .

[29]  K. Jousten Wutz Handbuch Vakuumtechnik : Theorie und Praxis , 2004 .

[30]  A. Luchetta,et al.  ANALYSIS OF THE CONTROL SYSTEM OF ICE , THE INSULATION AND COOLING TEST FACILITY FOR THE DEVELOPMENT OF THE ITER NEUTRAL BEAM INJECTOR * , 2010 .

[31]  Kazuhiro Watanabe,et al.  Recent progress on high power negative ion sources at JAERI , 1994 .

[32]  Piero Agostinetti Methods for the Thermo-mechanical Analysis and Design of High Power Ion Sources , 2008 .

[33]  Madhan Shridhar Phadke,et al.  Quality Engineering Using Robust Design , 1989 .

[34]  O. Kaneko,et al.  Negative hydrogen ion source development for large helical device neutral beam injector (invited) , 2000 .

[35]  P. Spädtke,et al.  Investigation of extraction systems with low aberrations , 1992 .

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

[37]  U. Fantz,et al.  Spectroscopy—a powerful diagnostic tool in source development , 2006 .

[38]  B. Heinemann,et al.  Long Pulse H− Beam Extraction With A RF Driven Ion Source With Low Fraction Of Co‐Extracted Electrons , 2009 .

[39]  P. Sonato,et al.  Design of a low voltage, high current extraction system for the ITER Ion Source , 2009 .

[40]  V. Antoni,et al.  Compensation of beamlet deflection by mechanical offset of the grids apertures in the SPIDER ion source , 2009, 2009 23rd IEEE/NPSS Symposium on Fusion Engineering.

[41]  P. Staub Bulk target backscattering coefficient and energy distribution of 0.5-100 keV electrons : an empirical and synthetic study , 1994 .

[42]  B. Heinemann,et al.  Design of the half-size ITER neutral beam source for the test facility ELISE , 2009 .

[43]  R. S. Hemsworth,et al.  Status of the ITER heating neutral beam system , 2009 .

[44]  P. Sonato,et al.  Optimisation of the magnetic field configuration for the negative ion source of ITER neutral beam injectors , 2008 .

[45]  Brian W. Barrett,et al.  Oak Ridge National Laboratory , Oak Ridge , TN , 2022 .

[46]  V. Toigo,et al.  The ITER full size plasma source device design , 2009 .

[47]  Jérôme Paméla,et al.  A model for negative ion extraction and comparison of negative ion optics calculations to experimental results , 1991 .

[48]  N Pilan,et al.  IRES: A Code to Calculate the Beamlet–Beamlet Interaction for Multiaperture Electrostatic Accelerators , 2010, IEEE Transactions on Plasma Science.