Thermal evolution of helium bubbles in tungsten by GISAXS and TDS

Grazing-incidence small-angle x-ray scattering (GISAXS) and thermal desorption spectroscopy (TDS) were used to study the thermal evolution of helium (He) bubbles in tungsten (W). W samples were exposed to a low ion energy (∼20 eV, sheath accelerated) He plasma at two sample temperatures: 573 K (low-temperature) and 1050 K (high-temperature). They were then annealed to temperatures of 773 K, 873 K and 998 K. GISAXS analysis showed an increase in the median bubble radius of the high-temperature samples from 6.42 Å to 12.87 Å as a result of annealing to 998 K. No changes in the bubble radii distributions were observed for the low-temperature samples and the median radius remained at ∼4 Å even after annealing. TDS showed that the desorption behaviour of He in W has a dependence on the sample temperature during plasma irradiation. The higher-temperature sample experienced a maximum desorption rate that is an order of magnitude larger than the low-temperature sample. The desorption profile of the high-temperature sample spanned a wider temperature range, 500 K - 1500 K, than the low-temperature sample, 500 K - 750 K. The formation and thermal evolution of He bubbles in W have a clear dependence on sample temperature during plasma exposure. The differences in annealing behaviour observed in this work agree with prior in-situ TEM annealing experiments and help explain macroscopic plasma-material interaction effects such as recrystallisation suppression. • Annealing causes growth in He bubbles in W exposed to plasma at 1050 K. • No growth in He bubbles after annealing W exposed to He plasma at 573 K. • He desorption by annealing is higher in W exposed at 1050 K than at 573 K. • He desorption in W exposed to 1050 K is a symptom of the bubble growth mechanism. • GISAXS trends agree with prior in-situ TEM annealing experiments.

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Publication Details

Journal
Journal of Nuclear Materials
Published
2024-11-19
DOI
https://doi.org/10.1016/j.jnucmat.2024.155524
Citations
2
Primary Topic
Fusion materials and technologies
Type
article
Field-Weighted Citation Impact
0.23

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article

Thermal evolution of helium bubbles in tungsten by GISAXS and TDS

N. Ohno, Matt Thompson, H. Tanaka, Nigel Kirby et al.
2 citations
Journal of Nuclear Materials
Fusion materials and technologies
0.23
article

Thermal evolution of helium bubbles in tungsten by GISAXS and TDS

N. Ohno, Matt Thompson, H. Tanaka, Nigel Kirby, S.H.B. Teo, A. Khan, Paul Mummery, Sarah L. Harmer, Cormac Corr, Danielle Hughes, N. Hammoud
article en
2 citations

Abstract

Grazing-incidence small-angle x-ray scattering (GISAXS) and thermal desorption spectroscopy (TDS) were used to study the thermal evolution of helium (He) bubbles in tungsten (W). W samples were exposed to a low ion energy (∼20 eV, sheath accelerated) He plasma at two sample temperatures: 573 K (low-temperature) and 1050 K (high-temperature). They were then annealed to temperatures of 773 K, 873 K and 998 K. GISAXS analysis showed an increase in the median bubble radius of the high-temperature samples from 6.42 Å to 12.87 Å as a result of annealing to 998 K. No changes in the bubble radii distributions were observed for the low-temperature samples and the median radius remained at ∼4 Å even after annealing. TDS showed that the desorption behaviour of He in W has a dependence on the sample temperature during plasma irradiation. The higher-temperature sample experienced a maximum desorption rate that is an order of magnitude larger than the low-temperature sample. The desorption profile of the high-temperature sample spanned a wider temperature range, 500 K - 1500 K, than the low-temperature sample, 500 K - 750 K. The formation and thermal evolution of He bubbles in W have a clear dependence on sample temperature during plasma exposure. The differences in annealing behaviour observed in this work agree with prior in-situ TEM annealing experiments and help explain macroscopic plasma-material interaction effects such as recrystallisation suppression. • Annealing causes growth in He bubbles in W exposed to plasma at 1050 K. • No growth in He bubbles after annealing W exposed to He plasma at 573 K. • He desorption by annealing is higher in W exposed at 1050 K than at 573 K. • He desorption in W exposed to 1050 K is a symptom of the bubble growth mechanism. • GISAXS trends agree with prior in-situ TEM annealing experiments.

Journal of Nuclear MaterialsVol. 604
Australian National University (AU), Flinders University (AU), Australian Synchrotron (AU), University of Manchester (GB), Nagoya University (JP)
Australian Nuclear Science and Technology Organisation, Diamond Light Source, Australian National University, Australian Synchrotron, Australian Research Council
Openalex Percentile: Top 50%
Fusion materials and technologies
0.23
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