4.6 Article

Radiation damage by light-and heavy-ion bombardment of single-crystal LiNbO3

Journal

OPTICAL MATERIALS EXPRESS
Volume 5, Issue 5, Pages 1071-1088

Publisher

OPTICAL SOC AMER
DOI: 10.1364/OME.5.001071

Keywords

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Funding

  1. Department of the Defense, Defense Threat Reduction Agency (DTRA) [HDTRA1-11-1-0022]
  2. National Science Foundation (NSF) [ECCS-1302488]
  3. Department of Energy's Office of Biological and Environmental Research and located at Pacific Northwest National Laboratory
  4. U.S. Department of Energy, Office of Basic Energy Sciences [DE-AC02-98CH10886]

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In this work, a battery of analytical methods including in situ RBS/C, confocal micro-Raman, TEM/STEM, EDS, AFM, and optical microscopy were used to provide a comparative investigation of light-and heavy-ion radiation damage in single-crystal LiNbO3. High (similar to MeV) and low (similar to 100s keV) ion energies, corresponding to different stopping power mechanisms, were used and their associated damage events were observed. In addition, sequential irradiation of both ion species was also performed and their cumulative depth-dependent damage was determined. It was found that the contribution from electronic stopping by high-energy heavy ions gave rise to a lower critical fluence for damage formation than for the case of low-energy irradiation. Such energy-dependent critical fluence of heavy-ion irradiation is two to three orders of magnitude smaller than that for the case of light-ion damage. In addition, materials amorphization and collision cascades were seen for heavy-ion irradiation, while for light ion, crystallinity remained at the highest fluence used in the experiment. The irradiation-induced damage is characterized by the formation of defect clusters, elastic strain, surface deformation, as well as change in elemental composition. In particular, the presence of nanometric-scale damage pockets results in increased RBS/C backscattered signal and the appearance of normally forbidden Raman phonon modes. The location of the highest density of damage is in good agreement with SRIM calculations. (C) 2015 Optical Society of America

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