Dergiler / Communications Faculty of Sciences University of Ankara Series A2-A3 Physical Sciences and Engineering / 2021 / Cilt: 63 - Sayı: 1

Analysis of Bragg curve parameters and lateral straggle for proton and carbon beams

Sayfa
32–41
Yayın Tarihi
2021-06-30
DOI
—
🏛️Bu makalenin bibliyografik verileri ve tam metin bağlantısı DergiPark üzerinden sağlanmıştır.
DergiPark Kaydı ↗
✨

Yapay Zeka Hızlı Bakış & Çıkarımlar

AI Insight
⚡ TL;DR(1 Cümlede Hızlı Çıkarım)

In line with all these results, the most commonly used proton and carbon heavy ions in hadron therapy applications were compared.

📌 3 Maddede Bu Makale

🎯
Amaç & Hipotez:Öz Heavy ions have varying effects on the target.
📊
Temel Bulgular & Veri:This loss of energy increases along the way, and the maximum energy loss is reached at the end of the range.
💡
Sonuç & Katkı:In line with all these results, the most commonly used proton and carbon heavy ions in hadron therapy applications were compared.
🔬Tür:Araştırma Makalesi
📍Kapsam:Genişletilmiş Akademik Örneklem
⚙️Değişkenler:Anahtar Kelimeler Carbon and proton ion radiotherapy · ion beam · Bragg curve

Özet

Öz Heavy ions have varying effects on the target. The most important factor in comparing this effect is Linear Energy Transfer (LET). Protons and carbons are heavy ions with high LET. Since these ions lose energy through collisions as they move through the tissue, their range is not long. This loss of energy increases along the way, and the maximum energy loss is reached at the end of the range. This whole process is represented by the Bragg curve. The input dose of the Bragg curve, full width at half maximum (FWHM) value, Bragg peak amplitude and position, and Penumbra thickness are important factors in determining which particle is advantageous in tumor treatment. While heavy ions move through the tissue, small deviations occur in their direction of travel due to Coulomb collisions. These small deviations cause lateral straggle in the dose profile. Lateral straggle is important in determining the type and energy of the particle used in tumor treatments close to critical organs. In our study, when the water phantom of protons and carbon beams with different energies is taken into consideration, the input dose, FWHM value, peak amplitude and position, penumbra thickness and lateral straggle are calculated using the TRIM code and the results are compared with Monte Carlo (MC) simulation. It was found that the proton has an average of 63% more FWHM and 53% more Penumbra than the carbon ion. The carbon ion has an average of 28-45 times greater Bragg peak amplitude at the same Bragg peak location than the proton. It was observed that the proton scattered approximately 70% more in lateral straggle. The difference was found to be around 1.32 mm. In line with all these results, the most commonly used proton and carbon heavy ions in hadron therapy applications were compared.

🔖

Bu Makaleye Atıf Yap

EKİNCİ, F., BOSTANCI, G. E., DAĞLI, Ö., GÜZEL, M. S. (2021). Analysis of Bragg curve parameters and lateral straggle for proton and carbon beams. Communications Faculty of Sciences University of Ankara Series A2-A3 Physical Sciences and Engineering, Cilt: 63 - Sayı: 1, 32–41. https://ajindex.com/articles/215740

📄 Tam Metin PDF Okuyucu

📄

PDF görüntüleyici hazırlanıyor...

Kaynakça (12)

  1. PTCOG, Particle Therapy Co-Operative Group, (2020). http://ptcog.web.psi.ch. Date of Access: 15.07.2020. ICRU Report 49 (1993). International Commission on Radiation Units and Measurements: Stopping Powers and Ranges for Protons and Alpha Particles. Niemierko, A., Urie, M., and Goitein, M., Optimization of 3D Radiation Therapy with both Physical and Biological End Points and Constraints, Int. J. Radiat. Oncol. Bio. Phys., 23 (1992), 99-108.
  2. Dowdell, S. J., Pencil beam scanning proton therapy: the significance of secondary particles, University of Wollongong, Australia, 2011.
  3. Bragg, W., On the a-particles of radium and their loss of range in passing through various atoms and molecules, Philos. Mag.,10 (1905), 318-340.
  4. Vachani, C., Proton Therapy: The Basics, (2012). oncolink.org/treatment/article.cfm. Date of Access: 15.05.2017.
  5. Brown, A. and Suit, H., The centenary of the discovery of the Bragg peak, Radiother. oncol.,73 (3) (2004), 265-268.
  6. Ziegler, J. F., SRIM, (2018). http://www.srim.org/. Date of Access: 01.09.2020.
  7. Winterborn, L. N., Reports 4829 (1972)., 4832 (1972)., especially CRNL-1817 (1978). Available from the Chalk River Nuclear Laboratory, Chalk River, Ontorio, Canada, KOJ-IJO. Foster, D., Artur, G., Average neutronic properties of “prompt” fission products, Los Alamos National Laboratory Report LA-9168-MS, 1982.
  8. Ziegler, J. F., The stopping and range of ions in matter, (1996). http.//www.srim.org/. Date of Access: 01.09.2018.
  9. Behrens, R., and Hupe, O., Influence of the phantom shape (slab, cylinder or alderson) on the performance of an hp(3) eye dosemeter, Radiat. Prot. Dosimetry, 168 (4) (2016), 441–449.
  10. Tang, S. B., Yin, Z. J., Huang, H., Cheng, Y., Cheng, F. H. and Mao, F. H., Geant4 used in medical physics and hadrontherapy technique, Nucl. Sci. Tech., 17 (2006), 276–279. https://doi:10.1016/S1001-8042(06)60051-1
  11. Jia, X., Schumann, J., Paganetti, H. and Jiang, S. B., GPU-based fast Monte Carlo dose calculation for proton therapy, Phys. Med. Biol., 57 (2012), 7783–7797. https://doi:10.1088/0031-9155/57/23/7783
  12. Yang, Z.-Y., Tsai, P.-E., Lee, S.-C., Liu, Y.-C., Chen, C.-C., Sato, T., et al., Inter-comparison of dose distributions calculated by FLUKA, GEANT4, MCNP, and PHITS for proton therapy, EPJ Web Conf (ICRS-13 RPSD-2016), 153 (2017), 04011. https:/doi:10.1051/epjconf/201715304011 Jia, S. B., Hadizadeh, M. H., Mowlavi, A. A. and Loushaba, M. E., Evaluation of energy deposition and secondary particle production in proton therapy of brain