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Nanostrukturen und Grenzflächen Poster: Do., 13:00–15:30 D-P312<br />

Heavy ion induced damage in alkali halide crystals<br />

irradiated at 8 and 300 K<br />

Kurt Schwartz 1 , Alexander Volkov 2 , Christina Trautmann 1 , Kay-Obbe<br />

Voss 1 , Maik Lang 1 , Michael Sorokin 2 , Reinhard Neumann 1<br />

1 Gesellschaft für Schwerionenforschung (GSI), Planckstr. 1, D 64291 Darmstadt, Germany<br />

– 2 Russian Research Centre Kurchatov Institute, Kurchatov Sq. 1, 123182<br />

Moscow, Russia<br />

Radiation damage in alkali halides induced by swift heavy ions is investigated by optical<br />

spectroscopy, optical bleaching, thermo-stimulated luminescence (TSL), and scanning<br />

force microscopy (SFM). Single crystals of LiF and NaCl were irradiated at the UNI-<br />

LAC linear accelerator of GSI with different heavy ions (from carbon to uranium) in<br />

the energy range between 50 and 2600 MeV. The irradiations were performed from 8<br />

K up to room temperature (RT) using a cryostat that allows additionally in situ absorption<br />

and TSL measurements. The evolution of various color centers was studied<br />

as a function of ion fluence and irradiation temperature [1, 2].<br />

The efficiency of F-center creation strongly depends on the energy loss of the ions and<br />

is related to electron-hole recombination processes [1, 2]. In LiF and NaCl crystals<br />

irradiated at 8 K primary hole centers were observed which are thermally annealed<br />

between 10 and 140 K. In LiF, crystals the ion induced damage changes the electronic<br />

structure of anion excitons [3].<br />

On the surface of irradiated ionic crystals each ion produces a nanometric hillock [4].<br />

The size (height and diameter) of the hillocks depends on the energy loss of the ion<br />

but is independent of the irradiation temperature (8 K, RT) which is in contrast to the<br />

creation of color centers.<br />

The efficiency of color center creation is related to local heating and thermally stimulated<br />

separation of primary color centers in ion tracks. Thermal spike calculations are<br />

performed to describe the heat propagation in the track [2].<br />

[1] K. Schwartz, C. Trautmann, A.S. El-Said, R. Neumann, M. Toulemonde, W.Knolle,<br />

Phys. Rev. B 70 (2004) 184104.<br />

[2] K. Schwartz, A.E. Volkov, K.-O. Voss, M. Sorokin, C. Trautmann, R. Neumann,<br />

Nucl. Instr. Meth. B 245 (2006) 204.<br />

[3] A. Luschchik, A. Kotlov, Ch. Lushchik, V. Nagirnyi, K. Schwartz, E. Vasil´chenko,<br />

Annual Report DESY 2005, Hamburg, 2006, pp. 257 258.<br />

[4] C. Müller, M. Cranney, A.. El-Said, N. Ishikawa, A. Iwase, M. Lang, R. Neumann,<br />

Nucl. Instr. Meth. B 191 (2002) 246.

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