Ontology type: schema:ScholarlyArticle Open Access: True
2021-09-27
AUTHORSV. Michalopoulou, M. Axiotis, S. Chasapoglou, Z. Eleme, G. Gkatis, A. Kalamara, M. Kokkoris, A. Lagoyannis, N. Patronis, A. Stamatopoulos, A. Tsantiri, R. Vlastou
ABSTRACTThe fission cross section of 232\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{232}$$\end{document}Th has been measured at fast neutron energies, using a setup based on Micromegas detectors. The experiment was performed at the 5.5 MV Van de Graaff Tandem accelerator in the neutron beam facility of the National Centre for Scientific Research “Demokritos”. The quasi-monoenergetic neutron beams were produced via the 3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{3}$$\end{document}H(p,n), 2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{2}$$\end{document}H(d,n) and 3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{3}$$\end{document}H(d,n) reactions, while the 238\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{238}$$\end{document}U(n,f) and 235\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{235}$$\end{document}U(n,f) reactions were used as references, in order to acquire cross-section data points in the energy range 2–18 MeV. The characterization of the actinide samples was performed via α\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha $$\end{document}-spectroscopy with a Silicon Surface Barrier (SSB) detector, while Monte Carlo simulations with the FLUKA code were used to achieve the deconvolution of the 232\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{232}$$\end{document}Th α\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha $$\end{document} peak from the α\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha $$\end{document} background of its daughter nuclei present in the spectrum. Special attention was given to the study of the parasitic neutrons present in the experimental area, produced via charged particle reactions induced by the particle beam and from neutron scattering. Details on the data analysis and results are presented. More... »
PAGES277
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| 27 | ″ | ″ | area |
| 28 | ″ | ″ | attention |
| 29 | ″ | ″ | background |
| 30 | ″ | ″ | barrier detectors |
| 31 | ″ | ″ | beam |
| 32 | ″ | ″ | beam facility |
| 33 | ″ | ″ | center |
| 34 | ″ | ″ | characterization |
| 35 | ″ | ″ | code |
| 36 | ″ | ″ | cross section data points |
| 37 | ″ | ″ | cross sections |
| 38 | ″ | ″ | data analysis |
| 39 | ″ | ″ | data points |
| 40 | ″ | ″ | daughter nuclei |
| 41 | ″ | ″ | deconvolution |
| 42 | ″ | ″ | detail |
| 43 | ″ | ″ | detector |
| 44 | ″ | ″ | energy |
| 45 | ″ | ″ | energy range 2 |
| 46 | ″ | ″ | experimental area |
| 47 | ″ | ″ | experiments |
| 48 | ″ | ″ | facilities |
| 49 | ″ | ″ | fast neutron energies |
| 50 | ″ | ″ | fission cross sections |
| 51 | ″ | ″ | measurements |
| 52 | ″ | ″ | neutron beam |
| 53 | ″ | ″ | neutron beam facility |
| 54 | ″ | ″ | neutron energy |
| 55 | ″ | ″ | neutron scattering |
| 56 | ″ | ″ | neutrons |
| 57 | ″ | ″ | nucleus |
| 58 | ″ | ″ | order |
| 59 | ″ | ″ | particle beams |
| 60 | ″ | ″ | peak |
| 61 | ″ | ″ | point |
| 62 | ″ | ″ | quasi-monoenergetic neutron beams |
| 63 | ″ | ″ | range 2 |
| 64 | ″ | ″ | reaction |
| 65 | ″ | ″ | reference |
| 66 | ″ | ″ | research |
| 67 | ″ | ″ | results |
| 68 | ″ | ″ | samples |
| 69 | ″ | ″ | scattering |
| 70 | ″ | ″ | scientific research |
| 71 | ″ | ″ | sections |
| 72 | ″ | ″ | setup |
| 73 | ″ | ″ | silicon surface barrier detector |
| 74 | ″ | ″ | simulations |
| 75 | ″ | ″ | special attention |
| 76 | ″ | ″ | spectra |
| 77 | ″ | ″ | spectroscopy |
| 78 | ″ | ″ | study |
| 79 | ″ | ″ | surface barrier detector |
| 80 | ″ | ″ | tandem accelerator |
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