Research Papers in Physics and Astronomy

 

Date of this Version

September 1991

Comments

Published in: RADECS 91--Radiation Effects on Computation and Systems: First European Conference on Radiation and its Effects on Devices and Systems : La Grande-Motte, near Montpellier, France, September 9-12,1991 (European Space Agency, Institute of Electrical and Electronics Engineers, & Université des sciences et techniques du Languedoc, 1992). [ISBN: 0-7803-0208-7] Pages: 558 - 560 Online at http://ieeexplore.ieee.org/xpl/tocresult.jsp?isnumber=5570&isYear=1991 Article @ http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5570&arnumber=213538&count=110&index=7 Digital Object Identifier: 10.1109/RADECS.1991.213538
Copyright (c) 1992 IEEE. Used by permission.

Abstract

Radiation effects induced by heavy ions in many materials with diverse end points are well described by the conceptual structure and equations of track physics, first developed for heavy ion tracks in nuclear emulsions. The model describes scintillators, biological cell inactivation and mutation, radiation chemistry, latent tracks in insulators, the response of resists to heavy ions, and other systems. A detector is taken to be composed of small targets whose response to ionizing radiation is principally to secondary electrons. The response is calibrated through determination of the probability of target (in)activation as a function of the absorbed dose of γ rays. This is then translated into the radial distribution of the probability of target (in)activation about the path of heavy ion through knowledge of the radial distribution of dose from δ rays. Radial integration yields the action cross-section σ, from which the response as a function of fluence of heavy ions is calculated. The author asks whether the track physics model is needed to describe single event upsets, or the effects produced in bulk matter by HZE particles.

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