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Measured and Monte Carlo simulated surface dose reduction for superficial X‐rays incident on tissue with underlying air or bone
Author(s) -
Baines John,
Zawlodzka Sylwia,
Markwell Tim,
Chan Millicent
Publication year - 2018
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 - 10.1002/mp.12725
Subject(s) - monte carlo method , imaging phantom , backscatter (email) , percentage depth dose curve , materials science , beam (structure) , ionization chamber , optics , nuclear medicine , physics , medicine , ion , telecommunications , statistics , mathematics , quantum mechanics , computer science , wireless , ionization
Purpose Measurement of surface dose reduction effects for superficial x‐rays incident on tissue with underlying air or bone and comparison with Monte Carlo simulations of such effects. Further to investigate the correlation between surface dose reduction and changes in Compton backscatter spectra with tissue‐bone separation. Methods An Advanced Markus chamber with entrance window facing downstream on the surface of a solid water phantom was used to investigate changes in surface dose with an underlying air or bone interface located at various depths below the surface. Chamber readings were obtained for interface depths ranging from 1 to 100 mm using the 50 kV , 100 kV and 150 kV beams of an Xstrahl 150 x‐ray unit, with field diameters ( ϕ ) = 2.5 cm and 5 cm. For each beam quality and field size the dose correction factor, DCF (t), namely the ratio of measured dose (t) to dose (t = 100 mm) was determined. Monte Carlo simulations of DCF (t) for air and bone interfaces in tissue are used to validate corresponding measured data. For a given beam and field size, the difference between simulated spectra with an air or bone interface at t = 3 mm was used to determine the Compton backscatter from bone at the surface. Results For air, DCF (t < 40 mm) is less than unity and for a given t DCF (t) decreases as beam energy increases from 50 kV to 150 kV . Conversely for bone DCF (t < 40 mm) increases for a given t with increasing beam energy. In particular for t = 1 mm, ϕ = 5 cm, DCF for air(bone) are 0.90(0.92) and 0.86(0.96) for 50 kV and 150 kV , respectively. For the same tube potentials corresponding factors, ϕ = 2.5 cm, for air(bone) are 0.94(0.96) and 0.92(0.99). Calculated DCF (t) based on Monte Carlo simulations are consistent with experimental observations to within 2%. Monte Carlo simulations of x‐ray spectra demonstrate the presence of Compton backscatter from underlying bone in tissue. With bone at 3 mm depth calculated backscatter spectra at the tissue surface suggest that surface dose is influenced by the proximity of bone and that this effect depends on beam quality. Conclusions This work demonstrates the feasibility of using an Advanced Markus chamber with entrance window facing downstream to investigate surface dose reduction with underlying air or bone in tissue. As the field size decreases and beam quality increases surface dose with underlying bone tends to full backscatter values even though tissue thicknesses are below those normally associated with full backscatter. Conversely with underlying bone close to the surface dose will increasingly fall below full backscatter values as the beam energy is reduced and field size is increased.