The investigation of distribution on size and concentration of helium bubbles in Y-bearing ODS steel using by SAXS and GIXRD
- 1. University of Chinese Academy of Sciences, Beijing 100039 (China)
- 2. Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049 (China)
- 3. Sino-French Institute of Nuclear Engineering and Technology, Sun Yat-Sen University, Zhuhai 519082, Guangdong (China)
Description
The nucleation and growth of the helium bubble in the structure material usually were subjected to temperature in a thermodynamic environment. In this study, Y-bearing oxide dispersed strengthened (ODS) ferritic/martensitic steels were used as the research material. The Y-bearing ODS steel samples with a thickness of 30 microns were irradiated successively by helium ions with three energies of 300 keV, 400 keV and 550 keV at room temperature and 450°C respectively. Firstly, the evolution of defects caused by irradiation is analyzed by using slow positron beam Doppler broadening spectroscopy (DBS) in positron annihilation spectroscopy technology (PAS). The formation and growth of helium bubbles are deduced from the changes in the concentration of vacancy-type defects. The increase in the size of the helium bubbles at high temperatures leads to a certain distortion of the crystal lattice, which is also verified by analyzing the grazing incidence X-ray diffraction (GIXRD) patterns. The characterization of radius and concentration of helium bubbles in samples irradiated at room temperature and 450°C have been studied by Small Angle X-ray Scattering (SAXS) and Transmission Electron Microscopy (TEM). The results showed that the intensity (I) ~ q-vector (q) curves of samples vary with irradiation temperature over ranges of 0.13 ≤ q ≤ 4.6 nm−1, which is attributed to the growth of helium bubbles at different irradiation temperature. It is found that the average size of helium bubbles under room temperature irradiation is about 1.78 nm, and the size distribution is narrow, while at the irradiation temperature of 450°C, the size of helium bubbles increases to 2.9 nm, and the size distribution is wider. This result is also verified from the TEM analysis. Besides, the shape of helium bubbles was assumed roughly and tends to spherical with higher temperatures.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.jnucmat.2021.153083Additional details
Identifiers
- DOI
- 10.1016/j.jnucmat.2021.153083;
- PII
- S0022311521003068;
Publishing Information
- Journal Title
- Journal of Nuclear Materials
- Journal Volume
- 554
- Journal Page Range
- vp.
- ISSN
- 0022-3115
- CODEN
- JNUMAM
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 54086350
- Subject category
- S36: MATERIALS SCIENCE;
- Descriptors DEI
- CRYSTAL LATTICES; DOPPLER BROADENING; FERRITIC STEELS; HELIUM IONS; MARTENSITIC STEELS; POSITRON ANNIHILATION SPECTROSCOPY; POSITRON BEAMS; SMALL ANGLE SCATTERING; SPHERICAL CONFIGURATION; THERMODYNAMICS; THICKNESS; TRANSMISSION ELECTRON MICROSCOPY; VACANCIES; VECTORS; X-RAY DIFFRACTION
- Descriptors DEC
- ALLOYS; BEAMS; CARBON ADDITIONS; CHARGED PARTICLES; COHERENT SCATTERING; CONFIGURATION; CRYSTAL DEFECTS; CRYSTAL STRUCTURE; DIFFRACTION; DIMENSIONS; ELECTRON MICROSCOPY; IONS; IRON ALLOYS; IRON BASE ALLOYS; LEPTON BEAMS; LINE BROADENING; MICROSCOPY; PARTICLE BEAMS; POINT DEFECTS; SCATTERING; SPECTROSCOPY; STEELS; TENSORS; TRANSITION ELEMENT ALLOYS
Optional Information
- Copyright
- Copyright (c) 2021 Elsevier B.V. All rights reserved.