A novel method for quantifying irradiation damage in nuclear graphite using Raman spectroscopy
A novel method for quantifying irradiation damage in nuclear graphite using Raman spectroscopy
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DOI:
10.1016/j.carbon.2023.118181
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发表时间:
2023-09
期刊:
影响因子:
10.9
通讯作者:
Ming Jiang;K. Ammigan;George Lolov;Frederique Pellemoine;Dong Liu
中科院分区:
文献类型:
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作者:
Ming Jiang;K. Ammigan;George Lolov;Frederique Pellemoine;Dong Liu
Raman spectroscopy has long been used in studying irradiation damage in carbon/graphite materials. It is however unclear if the measurements from different types of materials are directly comparable. Further, decoupling the contribution from irradiation temperature and fluence to the total damage in nuclear graphite possessing irradiation damage gradient is currently not readily feasible as it requires a complete set of test reactor irradiation experiments over the relevant temperature and fluence range. A novel methodology has therefore been proposed and developed to quantify total irradiation damage evolution at crystal level based on graphite Raman G-band position shift. Specifically, G-band positions derived from a large number of spectra collected from the fractured surface of microfine-grained POCO ZXF-5Q graphite possessing proton irradiation damage gradient were plotted with open literature Raman data on HOPG, BEPO (AXGP graphite), PCEA and IG-110 graphite as a function of dpa. The total damage level within 2σ beam radius in this POCO graphite was estimated to be equivalent to ∼2–5 dpa at ∼350–370 °C. Derived G-band positions were then mapped to the three-stage amorphization trajectory model indicating beam centre area has entered the second stage, i.e., transitioning from nanocrystalline graphite into amorphous carbon. G-band position relative shift (ΔG) curve with a ‘turn-around’ peak as a function of total damage can be used for in-service lifetime prediction. The developed methodology has the potential to ‘unify’ total damage levels across different grades of nuclear graphite caused by ion, neutron and proton irradiation at different temperatures.