1972
DOI: 10.2307/3573409
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Measurement of Ionization Distributions in Tissue-Equivalent Gas

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Cited by 22 publications
(5 citation statements)
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“…It should be noticed that the size of the target volume used in this work is markedly smaller than the target volumes used in previous experiments, which ranged from 125 nm to 1.3 µm at a density of 1 g cm −3 (Glass and Roesch 1972, Gross and Rodgers 1972, Kliauga and Rossi 1976, Toburen et al 1990, Schmollack et al 2000. These previous experiments were based on the measuring technique developed by Rossi and Rosenzweig (1955) using movable wall-less proportional counters immersed in a large container filled with a tissue-equivalent gas mixture to measure the fluctuation of energy which is absorbed in a target volume due to charged particles penetrating through or passing by.…”
Section: Discussionmentioning
confidence: 77%
“…It should be noticed that the size of the target volume used in this work is markedly smaller than the target volumes used in previous experiments, which ranged from 125 nm to 1.3 µm at a density of 1 g cm −3 (Glass and Roesch 1972, Gross and Rodgers 1972, Kliauga and Rossi 1976, Toburen et al 1990, Schmollack et al 2000. These previous experiments were based on the measuring technique developed by Rossi and Rosenzweig (1955) using movable wall-less proportional counters immersed in a large container filled with a tissue-equivalent gas mixture to measure the fluctuation of energy which is absorbed in a target volume due to charged particles penetrating through or passing by.…”
Section: Discussionmentioning
confidence: 77%
“…The quantity ?~D then results from Eq.. (7). This method is to derive the function t (x) directly for the mixed field of recoil protons, and then to derive the quantity yD.…”
Section: Large Sltesmentioning
confidence: 99%
“…(7). These measurements have b, from the center of a spherical [8,22,23] or cylindrical [7] wall-less proportional counter. In conclusion we will consider a special situation which corresponds to recent microdosimetric measurements [7,8,22,23].…”
Section: T(x) = Tô(x)+ Te(x)l (21)mentioning
confidence: 99%
“…Note that the frequency of zeros is high because the actual proton path length within the site is zero. Also, the relative widths of the distributions are significantly larger than for diametric tracks, a behavior which was first observed experimentally and explained by Glass and Roesch (1972) • The calculated frequency of zero ionization for diametric tracks produced by 1.0-MeV protons is shown in Figure 35. Straight lines join successive points merely to aid the eye.…”
Section: Calculation Of Distributions For Energymentioning
confidence: 66%
“…A description of the primary interaction model and initial tests of the code for ion track structure calculations, including comparisons with experimentally measured ionization frequency distributions (Glass and Roesch 1972), were reported previously Wil son 1977).…”
Section: Calculation Of Distributions For Energymentioning
confidence: 99%