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Electronic sputtering of LiF by Krypton (10 MeV/u): size dependent energy distributions of Li+(LiF)n clusters

A combination of imaging techniques (XY) and time-of-flight (TOF) spectroscopy was used to measure the complete velocity vector of sputtered positive secondary ions in collisions of Kr 33+ (10.1 MeV/u) with well-prepared LiF single crystals in the electronic stopping regime. The energy distributions...

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Bibliographic Details
Published in:The European physical journal. D, Atomic, molecular, and optical physics Atomic, molecular, and optical physics, 2012-11, Vol.66 (11), Article 305
Main Authors: Hijazi, H., Rothard, H., Boduch, P., Alzaher, I., Langlinay, Th, Cassimi, A., Ropars, F., Been, T., Ramillon, J. M., Lebius, H., Ban-d’Etat, B., Farenzena, L. S., da Silveira, E. F.
Format: Article
Language:English
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Summary:A combination of imaging techniques (XY) and time-of-flight (TOF) spectroscopy was used to measure the complete velocity vector of sputtered positive secondary ions in collisions of Kr 33+ (10.1 MeV/u) with well-prepared LiF single crystals in the electronic stopping regime. The energy distributions N ( E ) of the cluster ions (LiF) n Li + ( n ≥ 0) depend on the size of the ejecta: the maximum is slightly shifted towards lower energy with increasing cluster size n . The measured energy distributions of emitted cluster ions can be fitted by a Maxwell-Boltzmann function N ( E ) = AE exp(− βE ). This could be an indication that the processes generating the sputtering are compatible with a thermal origin.
ISSN:1434-6060
1434-6079
DOI:10.1140/epjd/e2012-30252-8