Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy Ions

Natural monoclinic zirconia (baddeleyite) was irradiated with 340 MeV Au ions, and the irradiation-induced nanostructures (i.e., ion tracks and nanohillocks) were observed using transmission electron microscopy. The diameter of the nanohillocks was approximately 10 nm, which was similar to the maxim...

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Main Authors: Norito Ishikawa, Shoma Fukuda, Toru Nakajima, Hiroaki Ogawa, Yuki Fujimura, Tomitsugu Taguchi
Format: Article
Language:English
Published: MDPI AG 2024-01-01
Series:Materials
Subjects:
Online Access:https://www.mdpi.com/1996-1944/17/3/547
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author Norito Ishikawa
Shoma Fukuda
Toru Nakajima
Hiroaki Ogawa
Yuki Fujimura
Tomitsugu Taguchi
author_facet Norito Ishikawa
Shoma Fukuda
Toru Nakajima
Hiroaki Ogawa
Yuki Fujimura
Tomitsugu Taguchi
author_sort Norito Ishikawa
collection DOAJ
description Natural monoclinic zirconia (baddeleyite) was irradiated with 340 MeV Au ions, and the irradiation-induced nanostructures (i.e., ion tracks and nanohillocks) were observed using transmission electron microscopy. The diameter of the nanohillocks was approximately 10 nm, which was similar to the maximum molten region size calculated using the analytical thermal spike model. Ion tracks were imaged as strained regions that maintained their crystalline structure. The cross-sections of most of the ion tracks were imaged as rectangular contrasts as large as 10 nm. These results strongly indicated that the molten region was recrystallized anisotropically, reflecting the lattice structure. Furthermore, low-density track cores were formed in the center of the ion tracks. The formation of low-density track cores can be attributed to the ejection of molten matter toward the surface. A comparison of the ion tracks in the synthetic zirconia nanoparticles and those in larger natural zirconia samples showed that the interface between the strained track contrast and the matrix was less clear in the former than in the latter. These findings suggest that the recrystallization process was affected by the size of the irradiated samples.
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spelling doaj.art-3598b6a4a46f4bbd8c06203dc71262112024-02-09T15:17:02ZengMDPI AGMaterials1996-19442024-01-0117354710.3390/ma17030547Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy IonsNorito Ishikawa0Shoma Fukuda1Toru Nakajima2Hiroaki Ogawa3Yuki Fujimura4Tomitsugu Taguchi5Nuclear Science and Engineering Center, Japan Atomic Energy Agency (JAEA), Tokai 319-1195, Ibaraki, JapanTono Geoscience Center, Japan Atomic Energy Agency (JAEA), Toki 509-5102, Gifu, JapanTono Geoscience Center, Japan Atomic Energy Agency (JAEA), Toki 509-5102, Gifu, JapanNuclear Science and Engineering Center, Japan Atomic Energy Agency (JAEA), Tokai 319-1195, Ibaraki, JapanNuclear Science and Engineering Center, Japan Atomic Energy Agency (JAEA), Tokai 319-1195, Ibaraki, JapanFoundational Quantum Technology Research Directorate, National Institutes for Quantum Science and Technology (QST), Takasaki 370-1292, Gunma, JapanNatural monoclinic zirconia (baddeleyite) was irradiated with 340 MeV Au ions, and the irradiation-induced nanostructures (i.e., ion tracks and nanohillocks) were observed using transmission electron microscopy. The diameter of the nanohillocks was approximately 10 nm, which was similar to the maximum molten region size calculated using the analytical thermal spike model. Ion tracks were imaged as strained regions that maintained their crystalline structure. The cross-sections of most of the ion tracks were imaged as rectangular contrasts as large as 10 nm. These results strongly indicated that the molten region was recrystallized anisotropically, reflecting the lattice structure. Furthermore, low-density track cores were formed in the center of the ion tracks. The formation of low-density track cores can be attributed to the ejection of molten matter toward the surface. A comparison of the ion tracks in the synthetic zirconia nanoparticles and those in larger natural zirconia samples showed that the interface between the strained track contrast and the matrix was less clear in the former than in the latter. These findings suggest that the recrystallization process was affected by the size of the irradiated samples.https://www.mdpi.com/1996-1944/17/3/547swift heavy ionhillocksion tracksion irradiationTEM
spellingShingle Norito Ishikawa
Shoma Fukuda
Toru Nakajima
Hiroaki Ogawa
Yuki Fujimura
Tomitsugu Taguchi
Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy Ions
Materials
swift heavy ion
hillocks
ion tracks
ion irradiation
TEM
title Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy Ions
title_full Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy Ions
title_fullStr Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy Ions
title_full_unstemmed Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy Ions
title_short Ion Tracks and Nanohillocks Created in Natural Zirconia Irradiated with Swift Heavy Ions
title_sort ion tracks and nanohillocks created in natural zirconia irradiated with swift heavy ions
topic swift heavy ion
hillocks
ion tracks
ion irradiation
TEM
url https://www.mdpi.com/1996-1944/17/3/547
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AT shomafukuda iontracksandnanohillockscreatedinnaturalzirconiairradiatedwithswiftheavyions
AT torunakajima iontracksandnanohillockscreatedinnaturalzirconiairradiatedwithswiftheavyions
AT hiroakiogawa iontracksandnanohillockscreatedinnaturalzirconiairradiatedwithswiftheavyions
AT yukifujimura iontracksandnanohillockscreatedinnaturalzirconiairradiatedwithswiftheavyions
AT tomitsugutaguchi iontracksandnanohillockscreatedinnaturalzirconiairradiatedwithswiftheavyions