Abstract
The mean excitation energy, \( \overline{I} \), appears in the logarithmic term of the soft collision stopping power. In practice, it is determined through extraction from measurements of the energy loss of a charged particle traversing a medium. However, there remains significant interest in understanding the theoretical aspects of the parameter, including deriving it ab initio and discovering that quite simplistic models can recreate the fundamental physical properties of \( \overline{I} \). In this chapter, theoretical models of increasing complexity are considered in the calculation of the mean excitation energy. The chapter is concluded with a review of the mechanisms of experimental determination of \( \overline{I} \) and parameterisations of the quantity. Although the latter are of limited practical use since tabulated values of \( \overline{I} \) exist, it is of historical interest to consider them.
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Notes
- 1.
However, we must still recall the caveats articulated in Chap. 5 of the approximate nature of the Thomas–Fermi model, particular with respect to the minimum number of atomic electrons required to provide a statistically valid result.
Bibliography and Further Reading
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McParland, B.J. (2014). Mean Excitation Energy. In: Medical Radiation Dosimetry. Springer, London. https://doi.org/10.1007/978-1-4471-5403-7_11
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DOI: https://doi.org/10.1007/978-1-4471-5403-7_11
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