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Mammographic x‐ray unit kilovoltage test tool based on k ‐edge absorption effect
Author(s) -
Napolitano Mary E.,
Trueblood Jon H.,
Hertel Nolan E.,
David George
Publication year - 2002
Publication title -
medical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.473
H-Index - 180
eISSN - 2473-4209
pISSN - 0094-2405
DOI - 10.1118/1.1501472
Subject(s) - inflection point , attenuation , imaging phantom , photon energy , optics , monte carlo method , photon , k edge , attenuation coefficient , computational physics , physics , materials science , absorption spectroscopy , mathematics , geometry , statistics
A simple tool to determine the peak kilovoltage (kVp) of a mammographic x‐ray unit has been designed. Tool design is based on comparing the effect of k ‐edge discontinuity of the attenuation coefficient for a series of element filters. Compatibility with the mammography accreditation phantom (MAP) to obtain a single quality control film is a second design objective. When the attenuation of a series of sequential elements is studied simultaneously, differences in the absorption characteristics due to the k ‐edge discontinuities are more evident. Specifically, when the incident photon energy is higher than the k ‐edge energy of a number of the elements and lower than the remainder, an inflection may be seen in the resulting attenuation data. The maximum energy of the incident photon spectra may be determined based on this inflection point for a series of element filters. Monte Carlo photon transport analysis was used to estimate the photon transmission probabilities for each of the sequential k ‐edge filter elements. The photon transmission corresponds directly to optical density recorded on mammographic x‐ray film. To observe the inflection, the element filters chosen must have k ‐edge energies that span a range greater than the expected range of the end point energies to be determined. For the design, incident x‐ray spectra ranging from 25 to 40 kVp were assumed to be from a molybdenum target. Over this range, the k ‐edge energy changes by approximately 1.5 keV between sequential elements. For this design 21 elements spanning an energy range from 20 to 50 keV were chosen. Optimum filter element thicknesses were calculated to maximize attenuation differences at the k ‐edge while maintaining optical densities between 0.10 and 3.00. Calculated relative transmission data show that the kVp could be determined to within ±1 kV. To obtain experimental data, a phantom was constructed containing 21 different elements placed in an acrylic holder. MAP images were used to determine appropriate exposure techniques for a series of end point energies from 25 to 35 kVp. The average difference between the kVp determination and the calibrated dial setting was 0.8 and 1.0 kV for a Senographe 600 T and a Senographe DMR, respectively. Since the k ‐edge absorption energies of the filter materials are well known, independent calibration or a series of calibration curves is not required.