Characterization of irradiation-induced novel voids in α-quartz

The macroscopic volume expansion of minerals subjected to high-energy irradiation typically occurs because of structural disordering. However, the mechanisms involved in this swelling associated with structural disordering have not been fully clarified. In particular, the role of the voids resulting...

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Main Authors: Naoki Okada, Takahiro Ohkubo, Ippei Maruyama, Kenta Murakami, Kiyoteru Suzuki
Format: Article
Language:English
Published: AIP Publishing LLC 2020-12-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0029299
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spelling doaj-affc21edf9ed49b6b4a5e425f2c8ff6b2021-01-05T15:00:07ZengAIP Publishing LLCAIP Advances2158-32262020-12-011012125212125212-1010.1063/5.0029299Characterization of irradiation-induced novel voids in α-quartzNaoki Okada0Takahiro Ohkubo1Ippei Maruyama2Kenta Murakami3Kiyoteru Suzuki4Graduate School of Engineering, Chiba University, 1-33 Yayoi-cho Inage-ku, Chiba 263-8522, JapanGraduate School of Engineering, Chiba University, 1-33 Yayoi-cho Inage-ku, Chiba 263-8522, JapanGraduate School of Environmental Studies, Nagoya University, ES-546, Furo-cho, Chikusa-ku, Nagoya, JapanInstitute of Gigaku, Nagaoka University of Technology, 1603-1 Kamitomioka, Nagaoka, Niigata 940-2188, JapanMitsubishi Research Institute, Inc., 10-3, Nagatacho 2-Chome, Chiyoda-Ku, Tokyo 100-8141, JapanThe macroscopic volume expansion of minerals subjected to high-energy irradiation typically occurs because of structural disordering. However, the mechanisms involved in this swelling associated with structural disordering have not been fully clarified. In particular, the role of the voids resulting from the aggregation of defects (which, in contrast to irradiated materials, are not observed in disordered melt-quenched amorphous glass) is still poorly understood. Here, we employ molecular dynamics simulations of α-quartz to examine a model that involves three stages of amorphization and volume expansion. The collapse of the crystalline structure is directly evaluated in terms of structural ordering based on symmetry operations, which enables the estimation of isolated defects. In the first stage, with increasing deposited energy, crystallinity decreases sharply compared with the decrease in density, which is linked to the formation of under- and over-coordinated atomic structures. Large voids (≥7.0 Å), which are not present in melt-quenched glass, are created at a deposition energy of 4 eV/atom, and in the second stage, the volume fractions of the large voids increase during subsequent irradiation from this energy up to 25 eV/atom. In the final stage, at higher deposited energies, the volume fraction of the large voids and the density fluctuate and become saturated owing to the balance between generation and annihilation of the large voids.http://dx.doi.org/10.1063/5.0029299
collection DOAJ
language English
format Article
sources DOAJ
author Naoki Okada
Takahiro Ohkubo
Ippei Maruyama
Kenta Murakami
Kiyoteru Suzuki
spellingShingle Naoki Okada
Takahiro Ohkubo
Ippei Maruyama
Kenta Murakami
Kiyoteru Suzuki
Characterization of irradiation-induced novel voids in α-quartz
AIP Advances
author_facet Naoki Okada
Takahiro Ohkubo
Ippei Maruyama
Kenta Murakami
Kiyoteru Suzuki
author_sort Naoki Okada
title Characterization of irradiation-induced novel voids in α-quartz
title_short Characterization of irradiation-induced novel voids in α-quartz
title_full Characterization of irradiation-induced novel voids in α-quartz
title_fullStr Characterization of irradiation-induced novel voids in α-quartz
title_full_unstemmed Characterization of irradiation-induced novel voids in α-quartz
title_sort characterization of irradiation-induced novel voids in α-quartz
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2020-12-01
description The macroscopic volume expansion of minerals subjected to high-energy irradiation typically occurs because of structural disordering. However, the mechanisms involved in this swelling associated with structural disordering have not been fully clarified. In particular, the role of the voids resulting from the aggregation of defects (which, in contrast to irradiated materials, are not observed in disordered melt-quenched amorphous glass) is still poorly understood. Here, we employ molecular dynamics simulations of α-quartz to examine a model that involves three stages of amorphization and volume expansion. The collapse of the crystalline structure is directly evaluated in terms of structural ordering based on symmetry operations, which enables the estimation of isolated defects. In the first stage, with increasing deposited energy, crystallinity decreases sharply compared with the decrease in density, which is linked to the formation of under- and over-coordinated atomic structures. Large voids (≥7.0 Å), which are not present in melt-quenched glass, are created at a deposition energy of 4 eV/atom, and in the second stage, the volume fractions of the large voids increase during subsequent irradiation from this energy up to 25 eV/atom. In the final stage, at higher deposited energies, the volume fraction of the large voids and the density fluctuate and become saturated owing to the balance between generation and annihilation of the large voids.
url http://dx.doi.org/10.1063/5.0029299
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AT ippeimaruyama characterizationofirradiationinducednovelvoidsinaquartz
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