Litcius/Paper detail

Direct determination of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>k</mml:mi> <mml:mrow> <mml:mover> <mml:mi>B</mml:mi> <mml:mo></mml:mo> </mml:mover> <mml:mo>,</mml:mo> <mml:mi>Q</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:msub> <mml:mi>Q</mml:mi> <mml:mn>0</mml:mn> </mml:msub> </mml:mrow> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> for cylindrical ionization chambers in a 6 MV 0.35 T MR-linac

A. Krauss, C.K. Spindeldreier, Sebastian Klüter

2020Physics in Medicine and Biology19 citationsDOI

Abstract

Abstract To ensure accurate reference dosimetry with ionization chambers in magnetic resonance linear accelerators (MR-linacs), the influence of the magnetic field on the response of the ionization chambers must be considered. The most direct method considering the influence of magnetic fields in dosimetry is to apply an appropriate absorbed-dose-to-water primary standard. At PTB, a new water calorimeter has been designed which is capable to determine D w,Q in an MR-linac. The new device allows the direct calibration of ionization chambers in terms of absorbed dose to water for MR-linac irradiation conditions. Hence, the correction factors <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mtext/> </mml:mrow> <mml:mrow> <mml:msub> <mml:mi>k</mml:mi> <mml:mrow> <mml:mover> <mml:mi>B</mml:mi> <mml:mo>⃗</mml:mo> </mml:mover> <mml:mo>,</mml:mo> <mml:mi>Q</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:msub> <mml:mi>Q</mml:mi> <mml:mn>0</mml:mn> </mml:msub> </mml:mrow> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> can be determined which replace the current radiation-quality dependent correction factors <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mi>k</mml:mi> <mml:mrow> <mml:mi>Q</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:msub> <mml:mi>Q</mml:mi> <mml:mn>0</mml:mn> </mml:msub> </mml:mrow> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> for dosimetry in the presence of magnetic fields. In cooperation with Heidelberg University Hospital, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mtext> </mml:mtext> </mml:mrow> <mml:mrow> <mml:msub> <mml:mi>k</mml:mi> <mml:mrow> <mml:mover> <mml:mi>B</mml:mi> <mml:mo>⃗</mml:mo> </mml:mover> <mml:mo>,</mml:mo> <mml:mi>Q</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:msub> <mml:mi>Q</mml:mi> <mml:mn>0</mml:mn> </mml:msub> </mml:mrow> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> factors were measured at the 6 MV 0.35 T Viewray MR-linac for different cylindrical ionization chambers with sensitive volumes ranging from 0.015 cm 3 to 0.65 cm 3 . The chambers were placed both perpendicular and parallel in respect to the magnetic field. Standard uncertainties of about 0.5% were achieved.

Topics & Concepts

Linear particle acceleratorDosimetryIonization chamberIonizationPhysicsMagnetic fieldAbsorbed dosePerpendicularPrimary standardCalibrationNuclear magnetic resonanceOpticsAtomic physicsNuclear medicineRadiationIonMathematicsMedicineBeam (structure)Quantum mechanicsGeometryRadiation Effects and DosimetryRadiation Detection and Scintillator TechnologiesRadiation Therapy and Dosimetry
Direct determination of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>k</mml:mi> <mml:mrow> <mml:mover> <mml:mi>B</mml:mi> <mml:mo></mml:mo> </mml:mover> <mml:mo>,</mml:mo> <mml:mi>Q</mml:mi> <mml:mo>,</mml:mo> <mml:mrow> <mml:msub> <mml:mi>Q</mml:mi> <mml:mn>0</mml:mn> </mml:msub> </mml:mrow> </mml:mrow> </mml:msub> </mml:mrow> </mml:math> for cylindrical ionization chambers in a 6 MV 0.35 T MR-linac | Litcius