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Struktur und Dynamik Poster: Mi., 14:00–16:30 M-P146<br />

Amorphization of Quasicrystalline Zr-Ti-Ni-Cu<br />

Stefan Mechler 1 , Gerhard Schumacher 1 , Siegfried Klaumünzer 1 , Thomas<br />

Zumkley 1 , Nelia Wanderka 1 , Michael-Peter Macht 1 , Christian Abromeit 1<br />

1 Hahn-Meitner-Institut Berlin, Glienicker Straße 100, D-14109 Berlin<br />

Au, Xe and Kr ions in the energetic range of 300-600 MeV were used to study the<br />

stability of quasicrystalline Zr-Ti-Ni-Cu under irradiation with swift heavy ions. Irradiation<br />

experiments have been performed at room temperature and at liquid nitrogen<br />

temperature at ISL. Prior to irradiation and after each fluence step the structure of<br />

the material was analyzed by means of X-ray diffraction. The X-ray measurements<br />

have been performed at room temperature under Bragg-Brentano geometry. Some<br />

specimens have also been analyzed by conventional and High Resolution Electron Microscopy<br />

(TEM and HRTEM, respectively) in the non-irradiated condition and after<br />

irradiation to moderate fluence steps. The structure of the specimens was completely<br />

quasicrystalline prior to irradiation. The relative decrease of the relative amount of<br />

the quasicrystalline phase under irradiation was determined by measuring the relative<br />

changes in X-ray peak intensity.<br />

Irradiation with 600 MeV Au ions lead to complete amorphization of the specimens<br />

already at fluence of 1x10 13 cm −2 . At lower fluences amorphous tracks inside the<br />

quasicrystals were visualized by the use of HRTEM. The track diameter near the surface<br />

determined by HREM was 12 nm. This value is in agreement with the value determined<br />

from X-ray diffraction measurements. Amorphization induced by 350 MeV Au ions<br />

and 600 MeV Au ions was assigned to the electronic energy loss while amorphization<br />

by 300 MeV Kr ions is predominantly due to the nuclear energy loss. Within the<br />

experimental uncertainty, there was no difference in amorphization between 350 MeV<br />

Au ions and 600 MeV Au ions. Irradiation at liquid nitrogen temperature results in<br />

slower amorphization compared to room-temperature irradiation. This result is in<br />

qualitative agreement with predictions of thermal spike models.

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