Year 2021,
Issue: 047, 197 - 206, 31.12.2021
Yiğit Ali Üncü
,
Onur Karaman
,
Aycan Şengül
,
Gizem Şişman
,
Kadir Akgüngör
References
- [1] World Health Organization (WHO) (2020). report on cancer: setting priorities, investing wisely and providing care for all. Geneva: World Health Organization;. Licence: CC BY-NC-SA 3.0 IGO.
- [2] Darestani, H., et al. (2011). Measurement of neutron dose component in central axis absorbed dose of 18 MV photon beam by TLD600 and TLD700 dosimeters. Basic & Clinical Cancer Research, 3(3&4): 22-29.
- [3] ICRP. (2019). Proceedings of the Fifth International Symposium on the System of Radiological Protection. Ann. ICRP49(S1): 32-34.
- [4] Khan, F.M., Gibbons, J.P. (2014). Khan's the physics of radiation therapy: Lippincott Williams & Wilkins.
- [5] Vylet, V., Liu, J. C. (2001). Radiation protection at high energy electron accelerators. Radiation protection dosimetry, 2001. 96(4): p. 333-343.
- [6] ICRP. (1991). Recommendations of the International Commission on Radiological Protection. ICRP Publication 60. Ann. ICRP21: 1-3.
- [7] Howell, R.M., et al. (2005). Investigation of secondary neutron dose for dynamic MLC IMRT delivery. Medical physics, 32(3): 786-793.
- [8] Ma, A., et al. (2008). Monte Carlo study of photoneutron production in the Varian Clinac 2100C linac. Journal of Radioanalytical and Nuclear Chemistry, 276(1): 119-123.
- [9] Jahangiri, M., et al. (2015). The effect of field size and distance from the field center on neutron contamination in medical linear accelerator. International Journal of Advanced Biological and Biomedical Research (IJABBR), 3(1): 97-104.
- [10] Carrier, J.F., et al. (2004). Validation of GEANT4, an object‐ oriented Monte Carlo toolkit, for simulations in medical physics. Medical physics, 31(3): 484-492.
- [11] Arce, P., et al. (2008). GAMOS: A Geant4-based easy and flexible framework for nuclear medicine applications. in 2008 IEEE Nuclear Science Symposium Conference Record, IEEE.
- [12] Karaman, O., Tanir A.G., Karaman C., (2019). Investigation of photoneutron contamination from the 18-MV photon beam in a medical linear accelerator, Materiali In Tehnologije, 55(3): 699-704.
- [13] Karaman, O., et al. (2020). Investigation of the effects of different composite materials on neutron contamination caused by medical LINAC/Untersuchung der Auswirkungen verschiedener Verbundmaterialien auf die Neutronenkontamination durch medizinische LINAC. Kerntechnik, 85(5): 401-407.
- [14] Karaman, O., Tanir, A.G. (2020). Radyoterapı̇ Odasının Farklı Noktalarında Nötron Kirliliğinin Ölçülmesi. Süleyman Demirel Üniversitesi Fen Edebiyat Fakültesi Fen Dergisi, 15(1): 36-44.
- [15] Özdoğan, H., Şekerci, M., Kaplan, A. Photo-neutron cross-section calculations of 54, 56Fe, 90, 91, 92, 94Zr, 93Nb and 107Ag Isotopes with newly obtained Giant Dipole Resonance parameters. Applied Radiation and Isotopes, 165: 109356-0.
- [16] Özdoğan, H., Şekerci, M., Kaplan, A. (2021). Production cross–section and reaction yield calculations for 123-126I isotopes on 123Sb (α, xn) reactions. Kuwait Journal of Science, 48(2): 1-11.
- [17] Şekerci, M., Özdoğan, H., Kaplan, A. (2020). Level density model effects on the production cross-section calculations of some medical isotopes via (α, xn) reactions where x= 1–3. Modern Physics Letters A, 35(24): 2050202-0.
- [18] Şekerci, M., Özdoǧan, H., Kaplan, A. (2020). Astrophysical S-Factor Calculations under the Effects of Gamma-Ray Strength Functions for Some Alpha Capture Reactions. Moscow University Physics Bulletin, 75(6): 585-589.
- [19] Özdoğan, H., Çapalı, V., Kaplan, A. (2015). Reaction Cross-Section, Stopping Power and Penetrating Distance Calculations for the Structural Fusion Material 54 Fe in Different Reactions. Journal of Fusion Energy, 34(2): 379-385.
- [20] Kalbach, C. (1986). Two-component exciton model: basic formalism away from shell closures. Physical Review C, 33(3): 818-833.
- [21] Ignatyuk, A.V., Istekov, K.K., Smirenkin, G.N., (1979). The role of collective effects in the systematics of nuclear level densities. Yad. Fiz. 29, 875–883.
- [22] TALYS–1.8 (2019). A Nuclear Reaction Program, User Manual, NRG, The Netherlands., A. 1st ed.Koning, Hilaire, S., Goriely, S.
THE EFFECTS of DIFFERENT RATIO for GADOLINIUM (GD) and TUNGSTEN (W) on NEUTRON CONTAMINATION CAUSED by MEDICAL LINAC COLLIMATOR
Year 2021,
Issue: 047, 197 - 206, 31.12.2021
Yiğit Ali Üncü
,
Onur Karaman
,
Aycan Şengül
,
Gizem Şişman
,
Kadir Akgüngör
Abstract
The linear accelerators (LINACs) produce high-energy X-rays and electron beams for the treatment of cancer patients. The basis of radiation therapy is based on the interaction between substance and radiation. LINAC as External beam radiotherapy, neutron contamination is produced in electron beams of medical LINAC by the contribution of the primary and the secondary collimators are founded. Consequently, the resulting photoneutrons can easily be scattered and spread into the clinical room. Thus, it is recommended that treatment planning performed should not be ignored in the tumor volume of the patient and areas outside this volume. The contribution of the primary collimator and the secondary collimators to the neutron contamination was found to be approximately 52% and 30%, respectively. This paper’s objective is to determine the neutron dose contamination from different materials in a LINAC. The effects of using different material ratios such as Gadolinium (Gd) and Tungsten (W) in secondary collimators on neutron contamination have been investigated by using Geant4-based Architecture for Medicine-Oriented Simulations (GAMOS) and TALYS 1.95 codes.
References
- [1] World Health Organization (WHO) (2020). report on cancer: setting priorities, investing wisely and providing care for all. Geneva: World Health Organization;. Licence: CC BY-NC-SA 3.0 IGO.
- [2] Darestani, H., et al. (2011). Measurement of neutron dose component in central axis absorbed dose of 18 MV photon beam by TLD600 and TLD700 dosimeters. Basic & Clinical Cancer Research, 3(3&4): 22-29.
- [3] ICRP. (2019). Proceedings of the Fifth International Symposium on the System of Radiological Protection. Ann. ICRP49(S1): 32-34.
- [4] Khan, F.M., Gibbons, J.P. (2014). Khan's the physics of radiation therapy: Lippincott Williams & Wilkins.
- [5] Vylet, V., Liu, J. C. (2001). Radiation protection at high energy electron accelerators. Radiation protection dosimetry, 2001. 96(4): p. 333-343.
- [6] ICRP. (1991). Recommendations of the International Commission on Radiological Protection. ICRP Publication 60. Ann. ICRP21: 1-3.
- [7] Howell, R.M., et al. (2005). Investigation of secondary neutron dose for dynamic MLC IMRT delivery. Medical physics, 32(3): 786-793.
- [8] Ma, A., et al. (2008). Monte Carlo study of photoneutron production in the Varian Clinac 2100C linac. Journal of Radioanalytical and Nuclear Chemistry, 276(1): 119-123.
- [9] Jahangiri, M., et al. (2015). The effect of field size and distance from the field center on neutron contamination in medical linear accelerator. International Journal of Advanced Biological and Biomedical Research (IJABBR), 3(1): 97-104.
- [10] Carrier, J.F., et al. (2004). Validation of GEANT4, an object‐ oriented Monte Carlo toolkit, for simulations in medical physics. Medical physics, 31(3): 484-492.
- [11] Arce, P., et al. (2008). GAMOS: A Geant4-based easy and flexible framework for nuclear medicine applications. in 2008 IEEE Nuclear Science Symposium Conference Record, IEEE.
- [12] Karaman, O., Tanir A.G., Karaman C., (2019). Investigation of photoneutron contamination from the 18-MV photon beam in a medical linear accelerator, Materiali In Tehnologije, 55(3): 699-704.
- [13] Karaman, O., et al. (2020). Investigation of the effects of different composite materials on neutron contamination caused by medical LINAC/Untersuchung der Auswirkungen verschiedener Verbundmaterialien auf die Neutronenkontamination durch medizinische LINAC. Kerntechnik, 85(5): 401-407.
- [14] Karaman, O., Tanir, A.G. (2020). Radyoterapı̇ Odasının Farklı Noktalarında Nötron Kirliliğinin Ölçülmesi. Süleyman Demirel Üniversitesi Fen Edebiyat Fakültesi Fen Dergisi, 15(1): 36-44.
- [15] Özdoğan, H., Şekerci, M., Kaplan, A. Photo-neutron cross-section calculations of 54, 56Fe, 90, 91, 92, 94Zr, 93Nb and 107Ag Isotopes with newly obtained Giant Dipole Resonance parameters. Applied Radiation and Isotopes, 165: 109356-0.
- [16] Özdoğan, H., Şekerci, M., Kaplan, A. (2021). Production cross–section and reaction yield calculations for 123-126I isotopes on 123Sb (α, xn) reactions. Kuwait Journal of Science, 48(2): 1-11.
- [17] Şekerci, M., Özdoğan, H., Kaplan, A. (2020). Level density model effects on the production cross-section calculations of some medical isotopes via (α, xn) reactions where x= 1–3. Modern Physics Letters A, 35(24): 2050202-0.
- [18] Şekerci, M., Özdoǧan, H., Kaplan, A. (2020). Astrophysical S-Factor Calculations under the Effects of Gamma-Ray Strength Functions for Some Alpha Capture Reactions. Moscow University Physics Bulletin, 75(6): 585-589.
- [19] Özdoğan, H., Çapalı, V., Kaplan, A. (2015). Reaction Cross-Section, Stopping Power and Penetrating Distance Calculations for the Structural Fusion Material 54 Fe in Different Reactions. Journal of Fusion Energy, 34(2): 379-385.
- [20] Kalbach, C. (1986). Two-component exciton model: basic formalism away from shell closures. Physical Review C, 33(3): 818-833.
- [21] Ignatyuk, A.V., Istekov, K.K., Smirenkin, G.N., (1979). The role of collective effects in the systematics of nuclear level densities. Yad. Fiz. 29, 875–883.
- [22] TALYS–1.8 (2019). A Nuclear Reaction Program, User Manual, NRG, The Netherlands., A. 1st ed.Koning, Hilaire, S., Goriely, S.