Format

Send to

Choose Destination
Phys Chem Chem Phys. 2019 Jul 10;21(27):14692-14700. doi: 10.1039/c9cp02302j.

Influence of Ti on the dissolution and migration of He in ZrCo based on first principles investigation.

Author information

1
Institute of Atomic and Molecular Physics, Sichuan University, Chengdu, 610064, China. gaotao@scu.edu.cn.
2
College of Optoelectronic Technology, Chengdu University of Information Technology, Chengdu 610225, China.
3
College of Mathematics, Sichuan University, Chengdu, 610064, China.
4
Science and Technology on Surface Physics and Chemistry Laboratory, P. O. Box 9071-35, Jiangyou 621907, China. angelsg1@126.com.
5
Hunan Key Laboratory for Super-Microstructure and Ultrafast Process, College of Physics and Electronics, Central South University, Changsha 410083, China.

Abstract

We have performed state-of-the-art ab initio calculations based on density functional theory to study the effect of Ti on helium dissolution and migration in a dilute Ti-doped ZrCo system. The formation energy of He-related defects predicts that it is preferable to occupy the VZr (Zr vacancy) at first. As for the Heint (interstitial site He), the results corroborate that Hetet (tetrahedral site He) is more stable than Heoct (octahedral site He) by 0.25 eV. The Heoct in the vicinity of Ti atoms becomes unstable, being relaxed into a nearby tetrahedral site, unlike in the pure ZrCo. We also reveal that ZrCo is susceptible to dopant Ti in terms of helium diffusion. The energy barrier for a Hetet to diffuse into a neighboring tetrahedral site is found to be about three times as large as the migration barrier between two adjacent octahedral interstitial sites (0.35 vs. 0.12 eV). In addition, the He atom can migrate from one octahedral site to another without going through a tetrahedral one in pure ZrCo. Furthermore, Hetet needs to overcome higher energy barriers of 0.27 eV and 0.58 eV in Ti-doped ZrCo than in the pure one (0.22 eV and 0.35 eV) along the 1nn (the first nearest neighbor) → 1nn → 2nn (the second nearest neighbor) pathway with the He atom escaping away from the Ti region. In addition, the dissociative energy barrier of the HeZr (Zr position substituted by the He atom) or HeCo (Co position substituted by the He atom) is somewhat higher in the presence of Ti than the pure one. All these conclusions elucidate that Ti acts as a trapping center for He impurities and blocks interstitial He mobility in ZrCo alloys.

PMID:
31215943
DOI:
10.1039/c9cp02302j

Supplemental Content

Full text links

Icon for Royal Society of Chemistry
Loading ...
Support Center