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THE ENERGY DEPOSITION DISTRIBUTION AT THE MICRO AND NANO-SCALE FOR MOLECULAR TARGETED RADIOTHERAPY: COMPARISON BETWEEN 125I, 99MTc AND 64Cu
S. Di Maria , A. Belchior, Y. Romanets, P. Vaz
Pages: 175-180
DOI: 10.21175/RadJ.2017.03.036
Received: 24 FEB 2017, Received revised: 16 MAY 2017, Accepted: 5 JUL 2017, Published online: 23 DEC 2017
Abstract |
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Given the very short range (micrometers to few nanometers) of Auger electrons (AE), Coster-Kronig (CK) and internal conversion (IC) electrons emitted by several radionuclides, they are nowadays considered as promising solutions for molecular targeted radiotherapy. The aforementioned electrons can locally deposit their energy near the radionuclide decay site, reducing the radiotoxicity of the surrounding healthy tissues in this way. 125I (T1/2=59 days, 23 Auger electrons emitted per decay, ĒAuger= 520 eV) and 99mTc (T1/2=6 h, 4.4 Auger electrons emitted per decay, ĒAuger=213 eV) are two radionuclides that are largely studied for their potential use in theranostic, even if the effectiveness of the 99mTc Auger emissions in inducing DNA double strand break (DSB) is still controversial. However, in recent years the use of 64Cu (T1/2=12.7 h, 1.80 Auger electrons emitted per decay, ĒAuger=1134 eV) emerged and became a burning issue, because, in addition to its imaging capabilities, some studies showed that 64Cu has cytotoxicity capabilities when incorporated in radiopharmaceuticals targeted at tumor cells. Therefore, for 64Cu the accurate assessment of the energy deposition pattern near the radionuclide decay site and how this energy varies with the radionuclide-DNA center distance is of paramount importance in order to better design therapeutic strategies based on the Auger electrons emitted by this radionuclide. For this reason, the aim of this work is to study the absorbed dose in the DNA and cell volumes considering the aforementioned three radionuclides described above and for the different spectra emissions of A, CK, IC and β radiation. In order to reach these goals, the state-of-the-art Monte Carlo (MC) radiation transport program MCNP6 was used. For the modeling and simulation purposes, a simplified geometry for the DNA segment, the cytoplasm and the cell, composed of liquid water, was considered and an isotropic-like source was modeled. Emission data (photons were neglected) were obtained from the International Commission on radiological Protection (ICRP) publication ICRP-107. This study shows to what extent the deposited energy pattern distribution is affected when several spectra qualities are considered (Auger, Conversion and β emissions); the discussion and comparison of results (also in terms of S-values calculated in this work and reported by MIRD) obtained for 64Cu with those obtained for 125I and 99mTc are reported.
- R. W. Howell, “Auger processes in the 21st century,” Int. J. Radiat. Biol., vol. 84, no. 12, pp. 959 – 975, Dec. 2008.
DOI: 10.1080/09553000802395527 PMid: 19061120 PMCid: PMC3459331
- P. L. Olive, “The role of DNA Single- and Double Strand Breaks in cell killing by Ionizing Radiation,” Radiat. Res., vol. 150, no. 5, pp. S42-S51, Nov. 1998.
DOI: 10.2307/3579807 PMid: 9806608
- N. Falzone, J. M. Fernández-Varea, G. Flux, K. A. Vallis, “Monte Carlo Evaluation of Auger Electron–Emitting Theranostic Radionuclides,” J. Nucl. Med., vol. 56, no. 9, pp. 1441 – 1446, Sep. 2015.
DOI: 10.2967/jnumed.114.153502 PMid: 26205298
- P. Balagurumoorthy et al., “Effect of distance between decaying 125I and DNA on Auger electron induced double-strand break yield,” Int. J. Radiat. Biol., vol. 88, no. 12, pp. 998 – 1008, Dec. 2012.
DOI: 10.3109/09553002.2012.706360 PMid: 22732063 PMCid: PMC3755766
- A. N. Asabella et al., “The Copper Radioisotopes: A Systematic Review with Special Interest to 64Cu,” BioMed Res. Int., vol. 2014, 786463, 2014.
DOI: 10.1155/2014/786463
- K. Eckerman et al., “ICRP Publication 107. Nuclear decay data for dosimetric calculations,” Ann. ICRP, vol. 38, pp. 7 – 96, 2008.
PMid: 19285593
- T. Goorley et al., “Initial MCNP6 release overview MCNP6 version 1.0,” Los Alamos National Laboratory, Los Alamos (NM), USA, Rep. LA-UR-13-22934, 2013.
Retrieved from: http://permalink.lanl.gov/object/tr?what=info:lanl-repo/lareport/LA-UR-13-22934; Retrieved on: Aug. 7, 2017
- G. Hughes, “Recent developments in low-energy electron/photon transport for MCNP6,” Prog. Nuc. Sci. Tech.,vol. 4, pp. 454 – 458, 2014.
DOI: 10.15669/pnst.4.454
- H. Nikjoo et al., “Track-structure codes in radiation research,” Radiat. Meas., vol. 41, no. 9-10, pp. 1052 – 1074, Oct-Nov. 2006.
DOI: 10.1016/j.radmeas.2006.02.001
- C. Champion et al., “Comparison between Three Promising ß-emitting Radionuclides, 67Cu, 47Sc and 161Tb, with Emphasis on Doses Delivered to Minimal Residual Disease,” Theranostics, vol. 6, no. 10, 2016.
DOI: 10.7150/thno.15132 PMid: 27446495 PMCid: PMC4955060
- S. M. Goddu, MIRD Cellular S-values, Reston (VA), USA: Society of Nuclear Medicine, 1997.
- M. A. Tajik-Mansoury, H. Rajabi and H. Mazdarani, “A comparison between track-structure, condensed-history Monte Carlo simulations and MIRD cellular S-values,” Phys. Med. Biol., vol. 62, no. 5, pp. N90 – N106, Mar. 2017.
DOI: 10.1088/1361-6560/62/5/N90 PMid: 28181480
- A. Taborda et al., “Dosimetry at the sub-cellular scale of Auger-electron emitter 99mTc in a mouse single thyroid follicle,” Appl. Radiat. Isot., vol. 108, pp. 58 – 63, Feb. 2016.
DOI: 10.1016/j.apradiso.2015.12.010 PMid: 26704702
- P. Lazakaris et al., “Comparison of nanodosimetric parameters of track structure calculated by the Monte Carlo codes Geant4-DNA and PTra,” Phys. Med. Biol.,vol. 57, no. 5, pp. 1231 – 1250, Mar.2012.
DOI: 10.1088/0031-9155/57/5/1231 PMid: 22330641
- M. Dingfelder et al., “Comparisons of Calculations with PARTRAC and NOREC: Transport of Electrons in Liquid Water,” Radiat. Res., vol. 169, no. 5, pp. 584 – 594, May 2008.
DOI: 10.1667/RR1099.1 PMid: 18439039 PMCid: PMC3835724
- E. Pereira et al., “Evaluation of Acridine Orange Derivatives as DNA-Targeted Radiopharmaceuticals for Auger Therapy: Influence of the Radionuclide and Distance to DNA,” Sci. Rep., vol. 7, 42544, Feb. 2017.
DOI: 10.1038/srep42544
- L. Jiang et al., “In vitro and in vivo studies on radiobiological effects of prolonged fraction delivery time in A549 cells,” J. Radiat. Res., vol. 54, no. 2, pp. 230 – 234, Mar. 2013.
DOI: 10.1093/jrr/rrs093 PMid: 23090953 PMCid: PMC3589931
- J. F. Fowler et al., “Loss of biological effect in prolonged fraction delivery,” Int. J. Radiat. Oncol. Biol. Phys., vol. 59, no. 1, pp. 242 – 249, 2004.
DOI: 10.1016/j.ijrobp.2004.01.004 PMid: 15093921
- J. Carlsson et al., “Requirements regarding dose rate and exposure time for killing of tumour cells in beta particle radionuclide therapy,” Eur. J. Nucl. Med. Mol. Imaging, vol. 33, no. 10, pp. 1185 – 1195, Oct. 2006.
DOI: 10.1007/s00259-006-0109-3 PMid: 16718515 PMCid: PMC1998878
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