Medical Dosimetry
Volume 31, Issue 4 , Pages 249-258, Winter 2006

Study on surface dose generated in prostate intensity-modulated radiation therapy treatment

  • James C.L. Chow, Ph.D., MCCPM

      Affiliations

    • Medical Physics Department, Grand River Regional Cancer Center, Grand River Hospital, Kitchener, Ontario, Canada
    • Department of Physics, University of Waterloo, Waterloo, Ontario, Canada
    • Corresponding Author InformationReprint requests to: James C. L. Chow, Radiation Medicine Program, Princess Margaret Hospital, University Health Network, 610 University Avenue, Toronto, ON M5G 2M9 Canada
  • ,
  • Grigor N. Grigorov, Ph.D.

      Affiliations

    • Medical Physics Department, Grand River Regional Cancer Center, Grand River Hospital, Kitchener, Ontario, Canada
    • Department of Physics, University of Waterloo, Waterloo, Ontario, Canada
  • ,
  • Rob B. Barnett, Ph.D., FCCPM

      Affiliations

    • Medical Physics Department, Grand River Regional Cancer Center, Grand River Hospital, Kitchener, Ontario, Canada
    • Department of Physics, University of Waterloo, Waterloo, Ontario, Canada

Received 11 July 2005; accepted 11 July 2005.

Abstract 

The surface doses of 6- and 15-MV prostate intensity-modulated radiation therapy (IMRT) irradiations were measured and compared to those from a 15-MV prostate 4-beam box (FBB). IMRT plans (step-and-shoot technique) using 5, 7, and 9 beams with 6- and 15-MV photon beams were generated from a Pinnacle treatment planning system (version 6) using computed tomography (CT) scans from a Rando Phantom (ICRU Report 48). Metal oxide semiconductor field effect transistor detectors were used and placed on a transverse contour line along the Phantom surface at the central beam axis in the measurement. Our objectives were to investigate: (1) the contribution of the dynamic multileaf collimator (MLC) to the surface dose during the IMRT irradiation; (2) the effects of photon beam energy and number of beams used in the IMRT plan on the surface dose. The results showed that with the same number of beams used in the IMRT plan, the 6-MV irradiation gave more surface dose than that of 15 MV to the phantom. However, when the number of beams in the plan was increased, the surface dose difference between the above 2 photon energies became less. The average surface dose of the 15-MV IMRT irradiation increased with the number of beams in the plan, from 0.86% to 1.19%. Conversely, for 6 MV, the surface dose decreased from 1.33% to 1.24% as the beam number increased from 7 to 9. Comparing the 15-MV FBB and 6-MV IMRT plans with 2 Gy/fraction, the IMRT irradiations gave generally more surface dose, from 15% to 30%, depending on the number of beams in the plan. It was found that the increase in surface dose for the IMRT technique compared to the FBB plan was predominantly due to the number of beams and the calculated monitor units required to deliver the same dose at the isocenter in the plans. The head variation due to the dynamic MLC movement changing the surface dose distribution on the patient was reflected by the IMRT dose-intensity map. Although prostate IMRT in this study had an average higher surface dose than that of FBB, the more even distribution of relatively lower surface dose in IMRT field could avoid the big dose peaks at the surface positions directly under the FBB fields. Such an even and low surface dose distribution surrounding the patient in IMRT is believed to give less skin complication than that of FBB with the same prescribed dose.

Key Words: Prostate IMRT, Surface dose, MOSFET detector, IMRT planning

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PII: S0958-3947(06)00049-5

doi:10.1016/j.meddos.2005.07.002

Medical Dosimetry
Volume 31, Issue 4 , Pages 249-258, Winter 2006