Helium behaviour in implanted boron carbide

When boron carbide is used as a neutron absorber in nuclear power plants, large quantities of helium are produced. To simulate the gas behaviour, helium implantations were carried out in boron carbide. The samples were then annealed up to 1500 °C in order to observe the influence of temperature and...

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Main Authors: Motte Vianney, Gosset Dominique, Miro Sandrine, Doriot Sylvie, Surblé Suzy, Moncoffre Nathalie
Format: Article
Language:English
Published: EDP Sciences 2015-01-01
Series:EPJ Nuclear Sciences & Technologies
Online Access:http://dx.doi.org/10.1051/epjn/e2015-50007-5
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spelling doaj-139fa95fd40842faa98131495485f41b2021-02-02T04:59:10ZengEDP SciencesEPJ Nuclear Sciences & Technologies2491-92922015-01-0111610.1051/epjn/e2015-50007-5epjn150007Helium behaviour in implanted boron carbideMotte VianneyGosset DominiqueMiro SandrineDoriot SylvieSurblé SuzyMoncoffre NathalieWhen boron carbide is used as a neutron absorber in nuclear power plants, large quantities of helium are produced. To simulate the gas behaviour, helium implantations were carried out in boron carbide. The samples were then annealed up to 1500 °C in order to observe the influence of temperature and duration of annealing. The determination of the helium diffusion coefficient was carried out using the 3He(d,p)4He nuclear reaction (NRA method). From the evolution of the width of implanted 3He helium profiles (fluence 1 × 1015/cm2, 3 MeV corresponding to a maximum helium concentration of about 1020/cm3) as a function of annealing temperatures, an Arrhenius diagram was plotted and an apparent diffusion coefficient was deduced (Ea = 0.52 ± 0.11 eV/atom). The dynamic of helium clusters was observed by transmission electron microscopy (TEM) of samples implanted with 1.5 × 1016/cm2, 2.8 to 3 MeV 4He ions, leading to an implanted slab about 1 μm wide with a maximum helium concentration of about 1021/cm3. After annealing at 900 °C and 1100 °C, small (5–20 nm) flat oriented bubbles appeared in the grain, then at the grain boundaries. At 1500 °C, due to long-range diffusion, intra-granular bubbles were no longer observed; helium segregates at the grain boundaries, either as bubbles or inducing grain boundaries opening.http://dx.doi.org/10.1051/epjn/e2015-50007-5
collection DOAJ
language English
format Article
sources DOAJ
author Motte Vianney
Gosset Dominique
Miro Sandrine
Doriot Sylvie
Surblé Suzy
Moncoffre Nathalie
spellingShingle Motte Vianney
Gosset Dominique
Miro Sandrine
Doriot Sylvie
Surblé Suzy
Moncoffre Nathalie
Helium behaviour in implanted boron carbide
EPJ Nuclear Sciences & Technologies
author_facet Motte Vianney
Gosset Dominique
Miro Sandrine
Doriot Sylvie
Surblé Suzy
Moncoffre Nathalie
author_sort Motte Vianney
title Helium behaviour in implanted boron carbide
title_short Helium behaviour in implanted boron carbide
title_full Helium behaviour in implanted boron carbide
title_fullStr Helium behaviour in implanted boron carbide
title_full_unstemmed Helium behaviour in implanted boron carbide
title_sort helium behaviour in implanted boron carbide
publisher EDP Sciences
series EPJ Nuclear Sciences & Technologies
issn 2491-9292
publishDate 2015-01-01
description When boron carbide is used as a neutron absorber in nuclear power plants, large quantities of helium are produced. To simulate the gas behaviour, helium implantations were carried out in boron carbide. The samples were then annealed up to 1500 °C in order to observe the influence of temperature and duration of annealing. The determination of the helium diffusion coefficient was carried out using the 3He(d,p)4He nuclear reaction (NRA method). From the evolution of the width of implanted 3He helium profiles (fluence 1 × 1015/cm2, 3 MeV corresponding to a maximum helium concentration of about 1020/cm3) as a function of annealing temperatures, an Arrhenius diagram was plotted and an apparent diffusion coefficient was deduced (Ea = 0.52 ± 0.11 eV/atom). The dynamic of helium clusters was observed by transmission electron microscopy (TEM) of samples implanted with 1.5 × 1016/cm2, 2.8 to 3 MeV 4He ions, leading to an implanted slab about 1 μm wide with a maximum helium concentration of about 1021/cm3. After annealing at 900 °C and 1100 °C, small (5–20 nm) flat oriented bubbles appeared in the grain, then at the grain boundaries. At 1500 °C, due to long-range diffusion, intra-granular bubbles were no longer observed; helium segregates at the grain boundaries, either as bubbles or inducing grain boundaries opening.
url http://dx.doi.org/10.1051/epjn/e2015-50007-5
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