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Nuclear Fushion
Validation of 2D and measurements made with Helium imaging spectroscopy in the volume of the TCV divertor
article
B.L. Linehan1  A. Perek2  B.P. Duval2  F. Bagnato2  P. Blanchard2  C. Colandrea2  H. De Oliveira2  O. Février2  E. Flom4  S. Gorno2  M. Goto5  E. Marmar1  L. Martinelli2  A. Mathews1  J. Muñoz-Burgos6  D. Mykytchuk2  N. Offeddu2  D.S. Oliveira2  H. Reimerdes2  D. Reiter7  O. Schmitz4  J.L. Terry1  C. Theiler2  C.K. Tsui8  B. Vincent2  T. Wijkamp3  C. Wüthrich2  W. Zholobenko9 
[1] Massachusetts Institute of Technology;Ecole Polytechnique Fédérale de Lausanne ,(EPFL), Swiss Plasma Center;DIFFER-Dutch Institute for Fundamental Energy Research;University of Wisconsin Madison;National Institute for Fusion Science;Astro Fusion Spectre LLC;Institut für Laser- und Plasmaphysik, Heinrich-Heine-Universität;Center for Energy Research ,(CER), University of California-San Diego;Max-Planck-Institut für Plasmaphysik
关键词: scrape-off layer;    multi-spectral imaging;    TCV;    helium collisional radiative modeling;    plasma boundary physics;    tokamak divertor;    tokamak diagnostics;   
DOI  :  10.1088/1741-4326/acb5b0
来源: Institute of Physics Publishing Ltd.
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【 摘 要 】

Multi-spectral imaging of helium atomic emission (HeMSI) has been used to create 2D poloidal maps of {{T}}_{mathrm{e}}and {{n}}_{mathrm{e}}in TCV's divertor. To achieve these measurements, TCV's MANTIS multispectral cameras (Pereket al2019Rev. Sci. Instrum.90123514) simultaneously imaged four He I lines (two singlet and two triplet) and a He II line (468 nm) from passively present He and He+. The images, which were absolutely calibrated and covered the whole divertor region, were inverted through the assumption of toroidal symmetry to create emissivity profiles and, consequently, line-ratio profiles. A collisional-radiative model (CRM) was applied to the line-ratio profiles to produce 2D poloidal maps of {{T}}_{mathrm{e}}and {{n}}_{mathrm{e}} . The collisional-radiative modeling was accomplished with the Goto helium CRM code (Zholobenkoet al2018Nucl. Fusion58126006, Zholobenkoet al2018Technical Report , Goto 2003J. Quant. Spectrosc. Radiat. Transfer76331–44) which accounts for electron-impact excitation (EIE) and deexcitation, and electron–ion recombination (EIR) with {extrm{He}}^{+} . The HeMSI {{T}}_{mathrm {e}}and {{n}}_{mathrm{e}}measurements were compared with co-local Thomson scattering measurements. The two sets of measurements exhibited good agreement for ionizing plasmas: ({5 ,{extrm{eV}} leqslant {{T}}_{mathrm{e}} leqslant 60 ,{extrm{eV}}} , and {2 imes 10^{18}, {extrm{m}}^{-3} leqslant{{n}}_{mathrm{e}} leqslant 3 imes 10^{19},{extrm{m}}^{-3}})in the case of majority helium plasmas, and ({10 ,{extrm{eV}} leqslant {{T}}_{mathrm{e}} leqslant 40 ,{extrm{eV}}},{2 imes 10^{18},{extrm{m}}^{-3} leqslant{{n}}_{mathrm{e}} leqslant 3 imes 10^{19} ,{extrm{m}}^{-3}})in the case of majority deuterium plasmas. However, there were instances where HeMSI measurements diverged from Thomson scattering. When {{T}}_{mathrm{e}} leqslant 10 ,{extrm{eV}}in majority deuterium plasmas, HeMSI deduced inaccurately high values of {{T}}_{mathrm{e}}{} . This disagreement cannot be rectified within the CRM's EIE and EIR framework. Second, on sporadic occasions within the private flux region, HeMSI produced erroneously high measurements of {{n}}_{mathrm{e}} . Multi-spectral imaging of Helium emission has been demonstrated to produce accurate 2D poloidal maps of {{T}}_{mathrm{e}}and {{n}}_{mathrm{e}}within the divertor of a tokamak for plasma conditions relevant to contemporary divertor studies.

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