2014
DOI: 10.1016/j.apradiso.2013.01.016
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Updated model for dielectric response function of liquid water

Abstract: A modified and updated version of the model of the dielectric response function of liquid water as currently implemented in the PARTRAC code is presented. The updated version takes advantage of the newer experimental information from the Sendai group and implements some improvements in modeling and usability.

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Cited by 28 publications
(29 citation statements)
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“…Thus, the only nontrivial parameter for calculating ionization and excitation cross sections (in the Born approximation) for liquid water is the dielectric function, ε(E,q), which accounts for the screening and polarization properties of the condensed phase. It is recognized 10,11 that there are three major models of the dielectric function of liquid water developed and refined through a series of studies: the Ritchie et al model, 12 the Dingfelder et al model, [13][14][15] and the Emfietzoglou et al model. [16][17][18][19][20] All these models are based on an analytic parameterization of the experimental data (those of Heller et al 21 or Hayashi et al 22 ) for the dielectric function of liquid water at the optical limit (q ≈ 0) using a linear superposition of Drude-like functions, and a set of dispersion relations to extend the dielectric function to q 0.…”
Section: A Dielectric Response Functionmentioning
confidence: 99%
“…Thus, the only nontrivial parameter for calculating ionization and excitation cross sections (in the Born approximation) for liquid water is the dielectric function, ε(E,q), which accounts for the screening and polarization properties of the condensed phase. It is recognized 10,11 that there are three major models of the dielectric function of liquid water developed and refined through a series of studies: the Ritchie et al model, 12 the Dingfelder et al model, [13][14][15] and the Emfietzoglou et al model. [16][17][18][19][20] All these models are based on an analytic parameterization of the experimental data (those of Heller et al 21 or Hayashi et al 22 ) for the dielectric function of liquid water at the optical limit (q ≈ 0) using a linear superposition of Drude-like functions, and a set of dispersion relations to extend the dielectric function to q 0.…”
Section: A Dielectric Response Functionmentioning
confidence: 99%
“…This may be attributed to their strong material dependence, along with the limited experimental data at k ≠ 0. On the other hand, for liquid water, the availability of experimental data for finite k has made possible the development of a consistent set of empirical dispersion relations for this material …”
Section: The ‘Standard’ Modelsmentioning
confidence: 99%
“…This equation for the DIMP provides a theoretical basis for the models for low energy ( < ∼ 100 eV) electron inelastic scatter in water that are used in modern Monte Carlo radiation transport codes. 16,19,20 For liquid water, which best represents the soft condensed matter phase of biological tissue, the dielectric response function should take into account the excitation and ionization energy levels in that thermodynamic phase. Experimental data for scattering off a liquid water target are scarce and the available data that is used to validate Drude oscillator models for (ω, q) is in the optical limit, q → 0.…”
Section: Dielectric Response Approachmentioning
confidence: 99%
“…These same electron inelastic cross-section models are also implemented in PARTRAC. 20 In Geant4, the liquid-water cross-section models are available in the module known as Geant4-DNA. 28 …”
Section: Monte Carlo Radiation Transport Modelingmentioning
confidence: 99%