2017
DOI: 10.1088/1361-6560/aa7016
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Air kerma calculation in Monte Carlo simulations for deriving normalized glandular dose coefficients in mammography

Abstract: The estimation of the mean glandular dose in mammography using Monte Carlo simulations requires the calculation of the incident air kerma evaluated on the breast surface. In such a calculation, caution should be applied in considering explicitly the presence of the top compression paddle, since Compton scattering in this slab may produce a large spread of the incidence angles of x-ray photons on the scoring surface. Then, the calculation of the incident air kerma should contain the 'effective' area of the scor… Show more

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Cited by 19 publications
(17 citation statements)
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“…The factor G was evaluated at energy E of the photon which deposits energy or, in case of the electron energy loss, at the energy of the photon which generated such an electron through a photoelectric or incoherent interaction. K was evaluated under the compression paddle, in a square region of interest ( S ) of area 0.8 × 0.8 cm 2 at the entrance breast skin surface attached to the chest wall using:K=iEi×μennormalρ)(EinormalairS×cositalicθiwhere E i is the photon energy of the i‐th photon crossing the scoring surface, [μ en /ρ]( E i ) air is the mass energy absorption coefficient of dry air and θ i is the angle between the photon direction and the vector normal to the scoring plane. In the evaluation of K , both primary radiation and scatter from the compression paddle were taken into account, but backscatter from the breast was not included.…”
Section: Methodsmentioning
confidence: 99%
“…The factor G was evaluated at energy E of the photon which deposits energy or, in case of the electron energy loss, at the energy of the photon which generated such an electron through a photoelectric or incoherent interaction. K was evaluated under the compression paddle, in a square region of interest ( S ) of area 0.8 × 0.8 cm 2 at the entrance breast skin surface attached to the chest wall using:K=iEi×μennormalρ)(EinormalairS×cositalicθiwhere E i is the photon energy of the i‐th photon crossing the scoring surface, [μ en /ρ]( E i ) air is the mass energy absorption coefficient of dry air and θ i is the angle between the photon direction and the vector normal to the scoring plane. In the evaluation of K , both primary radiation and scatter from the compression paddle were taken into account, but backscatter from the breast was not included.…”
Section: Methodsmentioning
confidence: 99%
“…A MC code for MGD calculation in X-ray breast imaging was developed and presented in previous papers [19,[21][22][23][24]. It is based on GEANT4 ver.…”
Section: Codementioning
confidence: 99%
“…To normalize the photon fluence in the MC simulation to that used in the experiments, a scale factor was used, defined as the ratio between the experimentally used air kerma (measured by the IOC) and the simulated incident air kerma (analytically evaluated in the MC code) in a square region of area 3 × 3 cm 2 placed 4 cm from the chest wall, laterally centered and under the compression paddle, as suggested by Sarno et al…”
Section: Methodsmentioning
confidence: 99%
“…To normalize the photon fluence in the MC simulation to that used in the experiments, a scale factor was used, defined as the ratio between the experimentally used air kerma (measured by the IOC) and the simulated incident air kerma (analytically evaluated in the MC code) in a square region of area 3 9 3 cm 2 placed 4 cm from the chest wall, laterally centered and under the compression paddle, as suggested by Sarno et al 34 The W/Rh spectrum at 28 kV was modeled using the TASMICS model 35 by adjusting the thickness of the modeled rhodium filter to minimize the difference between the predicted and the measured attenuation of the seven different aluminum layers previously obtained.…”
Section: F Geant4 Monte Carlo Simulationsmentioning
confidence: 99%