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Dislocation loop formation by swift heavy ion irradiation of metals

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Dislocation loop formation by swift heavy ion irradiation of metals. / Khara, Galvin S.; Murphy, Samuel T.; Duffy, Dorothy M.
In: Journal of Physics: Condensed Matter, Vol. 29, No. 28, 285303, 12.06.2017.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Khara, GS, Murphy, ST & Duffy, DM 2017, 'Dislocation loop formation by swift heavy ion irradiation of metals', Journal of Physics: Condensed Matter, vol. 29, no. 28, 285303. https://doi.org/10.1088/1361-648X/aa74f8

APA

Khara, G. S., Murphy, S. T., & Duffy, D. M. (2017). Dislocation loop formation by swift heavy ion irradiation of metals. Journal of Physics: Condensed Matter, 29(28), Article 285303. https://doi.org/10.1088/1361-648X/aa74f8

Vancouver

Khara GS, Murphy ST, Duffy DM. Dislocation loop formation by swift heavy ion irradiation of metals. Journal of Physics: Condensed Matter. 2017 Jun 12;29(28):285303. Epub 2017 May 25. doi: 10.1088/1361-648X/aa74f8

Author

Khara, Galvin S. ; Murphy, Samuel T. ; Duffy, Dorothy M. / Dislocation loop formation by swift heavy ion irradiation of metals. In: Journal of Physics: Condensed Matter. 2017 ; Vol. 29, No. 28.

Bibtex

@article{4e091828744a4f8997a9bdd0d7b193a7,
title = "Dislocation loop formation by swift heavy ion irradiation of metals",
abstract = "A coupled two-temperature, molecular dynamics methodology is used to simulate the structural evolution of bcc metals (Fe and W) and fcc metals (Cu and Ni) following irradiation by swift heavy ions. Electronic temperature dependent electronic specific heat capacities and electron–phonon coupling strengths are used to capture the full effects of the variation in the electronic density of states. Tungsten is found to be significantly more resistant to damage than iron, due both to the higher melting temperature and the higher thermal conductivity. Very interesting defect structures, quite different from defects formed in cascades, are found to be created by swift heavy ion irradiation in the bcc metals. Isolated vacancies form a halo around elongated interstitial dislocation loops that are oriented along the ion path. Such configurations are formed by rapid recrystallization of the molten cylindrical region that is created by the energetic ion. Vacancies are created at the recrystallization front, resulting in excess atoms at the core which form interstitial dislocation loops on completion of crystallization. These unique defect structures could, potentially, be used to create metal films with superior mechanical properties and interesting nanostructures.",
keywords = "swift heavy ions, dislocation loops, ion tracks, tungsten, iron, electron-phonon coupling, two temperature molecular dynamics",
author = "Khara, {Galvin S.} and Murphy, {Samuel T.} and Duffy, {Dorothy M.}",
year = "2017",
month = jun,
day = "12",
doi = "10.1088/1361-648X/aa74f8",
language = "English",
volume = "29",
journal = "Journal of Physics: Condensed Matter",
issn = "0953-8984",
publisher = "IOP Publishing Ltd",
number = "28",

}

RIS

TY - JOUR

T1 - Dislocation loop formation by swift heavy ion irradiation of metals

AU - Khara, Galvin S.

AU - Murphy, Samuel T.

AU - Duffy, Dorothy M.

PY - 2017/6/12

Y1 - 2017/6/12

N2 - A coupled two-temperature, molecular dynamics methodology is used to simulate the structural evolution of bcc metals (Fe and W) and fcc metals (Cu and Ni) following irradiation by swift heavy ions. Electronic temperature dependent electronic specific heat capacities and electron–phonon coupling strengths are used to capture the full effects of the variation in the electronic density of states. Tungsten is found to be significantly more resistant to damage than iron, due both to the higher melting temperature and the higher thermal conductivity. Very interesting defect structures, quite different from defects formed in cascades, are found to be created by swift heavy ion irradiation in the bcc metals. Isolated vacancies form a halo around elongated interstitial dislocation loops that are oriented along the ion path. Such configurations are formed by rapid recrystallization of the molten cylindrical region that is created by the energetic ion. Vacancies are created at the recrystallization front, resulting in excess atoms at the core which form interstitial dislocation loops on completion of crystallization. These unique defect structures could, potentially, be used to create metal films with superior mechanical properties and interesting nanostructures.

AB - A coupled two-temperature, molecular dynamics methodology is used to simulate the structural evolution of bcc metals (Fe and W) and fcc metals (Cu and Ni) following irradiation by swift heavy ions. Electronic temperature dependent electronic specific heat capacities and electron–phonon coupling strengths are used to capture the full effects of the variation in the electronic density of states. Tungsten is found to be significantly more resistant to damage than iron, due both to the higher melting temperature and the higher thermal conductivity. Very interesting defect structures, quite different from defects formed in cascades, are found to be created by swift heavy ion irradiation in the bcc metals. Isolated vacancies form a halo around elongated interstitial dislocation loops that are oriented along the ion path. Such configurations are formed by rapid recrystallization of the molten cylindrical region that is created by the energetic ion. Vacancies are created at the recrystallization front, resulting in excess atoms at the core which form interstitial dislocation loops on completion of crystallization. These unique defect structures could, potentially, be used to create metal films with superior mechanical properties and interesting nanostructures.

KW - swift heavy ions

KW - dislocation loops

KW - ion tracks

KW - tungsten

KW - iron

KW - electron-phonon coupling

KW - two temperature molecular dynamics

U2 - 10.1088/1361-648X/aa74f8

DO - 10.1088/1361-648X/aa74f8

M3 - Journal article

VL - 29

JO - Journal of Physics: Condensed Matter

JF - Journal of Physics: Condensed Matter

SN - 0953-8984

IS - 28

M1 - 285303

ER -