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The microscopic mechanism of nuclear irradiation creep is centered on the evolution of point defects and dislocation motion induced by irradiation, and can be divided into three core levels.: Generation and non-equilibrium evolution of point defects The collision of high-energy neutrons with lattice atoms will produce a large number of supersaturated vacancies and self-interstitial atoms. The concentration of such non-equilibrium point defects is much higher than the thermal equilibrium state, providing a material basis for subsequent dislocation motion. Two types of core mechanisms of dislocation motion irradiation enhancement paths: Supersaturated point defects greatly increase the dislocation climbing rate. Dislocations originally pinned by obstacles can bypass the obstacles through absorption/emission point defects, directly accelerating the creep process. irradiation induced pathways: Point defects diffuse directionally under a stress field. Dislocations with different orientations will preferentially absorb corresponding types of point defects, triggering directional movement of dislocations and causing anisotropic deformation of the material along the stress direction. Auxiliary contribution of dislocation loops Under the action of stress, gap-type dislocation loops will preferentially nucleate on the crystal planes perpendicular to the tensile stress, while vacancy-type dislocation loops will preferentially nucleate on the crystal planes parallel to the tensile stress. This asymmetric distribution will directly drive the material to elongate along the stress direction, further contributing to creep strain.
Thank you to the author for sharing such a detailed review, which clearly explains the three-layer mechanism of radiation creep, especially the distinction between the two paths of "irradiation enhancement" and "irradiation induction", which is very helpful for understanding the microscopic mechanism. I would like to add some details that are easily overlooked in actual operation.: The evolution path of point defects actually depends heavily on the irradiation temperature and dose rate. For example, at low temperature and high dose rate, self-interstitial atoms easily form clusters, which may inhibit dislocation climbing and lead to non-monotonic changes in the creep rate. It would be more intuitive if the poster could discuss it later based on the irradiation data of specific materials (such as zirconium alloy or austenitic stainless steel). In addition, experimental data in this field are greatly limited by the reactor environment, and many mechanism derivation still rely on simulation. It is recommended that interested forum friends pay attention to whether the operating condition parameter range is given in the literature when citing relevant conclusions to avoid excessive extrapolation.