doi:10.1016/S0168-9002(99)01303-0
Copyright © 2000 Elsevier Science B.V. All rights reserved.
Displacement energy for various ions in particle detector materials
A. Chilingarov
,
, D. Lipka, J. S. Meyer and T. Sloan
Department of Physics, University of Lancaster, Lancaster LA1 4YB, UK
Received 19 September 1999;
revised 9 November 1999;
accepted 2 December 1999.
Available online 6 July 2000.
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Abstract
The total displacement energy or total non-ionising energy loss has been calculated for a variety of ions during their slowing down to rest in the detector materials carbon, silicon and gallium arsenide. The calculations, based on the theory of Lindhard et al., have been performed using a Monte Carlo method and a simple parameterisation of the results is presented. Such a parameterisation will simplify considerably the future computation of the differential non-ionising energy loss by fast particles in particle detectors.
Author Keywords: Lindhard; Silicon; Diamond; Gallium arsenide; Detectors
PACS classification codes: 07.77−n; 85.30.−z
Fig. 1. Dependence of (dE/dx)el for Si ions in Si and Ge ions in GaAs on normalised velocity β. The rise at small β is described by Eq. (2) and the fall at large β by Eq. (1). The curved region between comes from the polynomial approximation described in the appendix.
Fig. 2. Displacement energy for several ions in C as a function of the incident ion kinetic energy. The smooth curves show the results of the parameterisation described in the text.
Fig. 3. The same as Fig. 2 for several ions in Si.
Fig. 4. The same as Fig. 2 for several ions in GaAs.
Fig. 5. Displacement energy for protons in three materials as a function of their kinetic energies. The smooth curves show the results of the parameterisation described in the text.
Fig. 6. The same as Fig. 5 for α-particles.
Fig. 7. Comparison of the displacement energies from our Monte Carlo (solid lines) with other calculations (dashed lines) for ions with various values of A and Z in (a) gallium arsenide [3], (b) silicon [5], and (c) carbon [4].
Table 1. Table of fitted ions with normalized χ2 between the data and the parameterisation

Table 2. Table of parameters for heavy ions

Table 3. Table of the parameters for protons and α-particles
