Abstract

A full energy range primary radiation damage model is presented here. It is based on the athermal recombination corrected displacements per atom (arc-dpa) model but includes a proper treatment of the near threshold conditions for metallic materials. Both ab initio (AIMD) and classical molecular dynamics (MD) simulations are used here for various metals with body-centered cubic (bcc), face-centered cubic (fcc), and hexagonal close-packed (hcp) structures to validate the model. For bcc and hcp metals, the simulation results fit very well with the model. For fcc metals, although there are slight deviations between the model and direct simulation results, it is still a clear improvement on the arc-dpa model. The deviations are due to qualitative differences in the threshold energy surfaces of fcc metals with respect to bcc and hcp metals according to our classical MD simulations. We introduce the minimum threshold displacement energy (TDE) as a term in our damage model. We calculated minimum TDEs for various metal materials using AIMD. In general, the calculated minimum TDEs are in very good agreement with experimental results. Moreover, we noticed a discrepancy in the literature for fcc Ni and estimated the average TDE of Ni using both classical MD and AIMD. It was found that the average TDE of Ni should be \ensuremath{\sim}70 eV based on simulation and experimental data, not the commonly used literature value of 40 eV. The most significant implications of introducing this full energy range damage model will be for estimating the effect of weak particle-matter interactions, such as for \ensuremath{\gamma}- and electron-radiation-induced damage.

Highlights

  • Radiation damage is a very general phenomenon that affects many scientific branches and areas of application, with examples from medicine [1], particle physics [2], applied computer science [3], space and aerospace [4], and not the least nuclear energy production, where intense neutron irradiation is in many cases life limiting for components due to radiation-induced degradation [5].The mechanism of radiation damage production in crystalline materials can be divided into two stages based on time scale

  • While both the modified model and experimental results show that the increase of damage production probability is essentially linear, there is a nonlinear relationship in the molecular dynamics (MD) simulation results

  • We modified the arc-dpa model with a lowenergy extension to make it suitable for near threshold displacement energy (TDE) primary damage events and provide a simple analytical damage model valid for all energy ranges

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Summary

INTRODUCTION

Radiation damage is a very general phenomenon that affects many scientific branches and areas of application, with examples from medicine [1], particle physics [2], applied computer science [3], space and aerospace [4], and not the least nuclear energy production, where intense neutron irradiation is in many cases life limiting for components due to radiation-induced degradation [5]. For low-energy events, such as those from electron and γ -ray interactions, none of the current models give reasonable estimates of the number of induced defects This is because the damage energies of the primary knock-on atom (PKA) transferred from electron and γ rays are close to the TDE of many materials, and the effect of the sharp threshold in the KP, NRT, and arc-dpa models risk giving unphysical results. It is well known from both experiments and MD simulations [4,10,11,12,13] that each lattice direction has its own TDE. Ab initio MD (AIMD) simulations are performed to calculate the TDE of various body-centered cubic (bcc), face-centered cubic (fcc), and hexagonal close-packed (hcp) metal materials in specific lattice directions in comparison with TDE obtained from MD simulations and with experiments

Analytical damage model
Classical MD simulation
AIMD simulation
Near TDE damage in fcc Cu
AIMD calculation of minimum TDEs of metals
Revising the TDE of fcc Ni
CONCLUSIONS
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