Document Type : Research paper
Authors
1 K. N. Toosi University of Technology
2 K. N. Toosi university of Technology
Abstract
In this work, the feasibility study on using a Coded-Aperture Imaging based on a Modified Uniformly Redundant Array coded mask in Single Photon Emission Computed Tomography (SPECT) was investigated for boron dose measurement in Boron Neutron Capture Therapy (BNCT). In this preliminary study, a MURA rank 13 with a 2×2 mosaic configuration, and a CZT detector array mounted in a single mask were investigated using Monte Carlo Simulation Code, MCNPX2.7. This is the first investigation on the use of Coded-Aperture Imaging for BNCT purposes for boron dose measurement during treatment. Also, the Maximum Likelihood-Expectation Maximization method was used for image reconstruction for boron dose estimation in the tissue. The results were examined for the recommended therapeutic neutron beam in the Tehran research reactor. Preliminary results show that SPECT with Modified Uniformly Redundant Array masks can be an efficient and precise tool for boron dose measurement in BNCT, and results show the superiority of this method in comparison to the conventional SEPCT in BNCT.
Keywords
- Boron dose imaging
- Single Photon Emission Computed Tomography
- Modified Uniformly Redundant Array
- Boron Neutron Capture Therapy
- Maximum Likelihood-Expectation Maximum
Main Subjects
therapy. TECDOC-1223. 2001.
[2] Babaeian K, Rahmani F, Kasesaz Y. Conceptual
design of prompt gamma neutron activation
analysis facility at Tehran Research Reactor
for BNCT application. Nuclear Instruments
and Methods in Physics Research Section A:
Accelerators, Spectrometers, Detectors and
Associated Equipment. 2019 Aug 11;935:185-
90.
[3] Murata I, Mukai T, Ito M, Miyamaru H, Yoshida
S. Feasibility study on BNCT-SPECT using a
CdTe detector. Progress in Nuclear Science
and Technology. 2011 Feb 15;1.
[4] Cieślak MJ, Gamage KA, Glover R. Codedaperture
imaging systems: Past, present and
future development–A review. Radiation
Measurements. 2016 Sep 1;92:59-71.
[5] Goorley T, James M, Booth T, Brown F, Bull J,
Cox LJ, Durkee J, Elson J, Fensin M, Forster RA,
Hendricks J. Initial MCNP6 release overview.
Nuclear technology. 2012 Dec 1;180(3):298-
315.
[6] Kasesaz Y, Khalafi H, Rahmani F, Ezzati A,
Keyvani M, Hossnirokh A, Shamami MA, Amini
S. Design and construction of a thermal
neutron beam for BNCT at Tehran Research
Reactor. Applied Radiation and Isotopes. 2014
Dec 1;94:149-51.
[7] Kasesaz Y, Khalafi H, Rahmani F. Design of an
epithermal neutron beam for BNCT in thermal
column of Tehran research reactor. Annals of
Nuclear Energy. 2014 Jun 1;68:234-8.
[8] Van Audenhaege K, Van Holen R,
Vandenberghe S, Vanhove C, Metzler SD,
Moore SC. Review of SPECT collimator
selection, optimization, and fabrication for
clinical and preclinical imaging. Medical
physics. 2015 Aug;42(8):4796-813.
[9] Murata I, Mukai T, Nakamura S, Miyamaru H,
Kato I. Development of a thick CdTe detector
for BNCT–SPECT. Applied Radiation and
Isotopes. 2011 Dec 1;69(12):1706-9.
[10] Minsky DM, Valda AA, Kreiner AJ, Green S,
Wojnecki C, Ghani Z. Experimental feasibility
studies on a SPECT tomograph for BNCT
dosimetry. Applied Radiation and Isotopes.
2009 Jul 1;67(7-8):S179-82.
[11] Caroli E, Stephen JB, Di Cocco G, Natalucci L,
Spizzichino A. Coded aperture imaging in
X-and gamma-ray astronomy. Space Science
Reviews. 1987 Sep;45(3):349-403.
[12] Grindlay JE, Hong J. Optimizing wide-field
coded aperture imaging: radial mask holes
and scanning. InOptics for EUV, X-Ray, and
Gamma-Ray Astronomy 2004 Jan 29 (Vol.
5168, pp. 402-410). SPIE.
[13] Gottesman SR, Fenimore EE. New family of
binary arrays for coded aperture imaging.
Applied optics. 1989 Oct 15;28(20):4344-52.
[14] Lee T, Lee W. Compact hybrid gamma camera
with a coded aperture for investigation of
nuclear materials. Nuclear Instruments and
Methods in Physics Research Section A:
Accelerators, Spectrometers, Detectors and
Associated Equipment. 2014 Dec 11;767:5-13.
[15] Cieślak MJ, Gamage KA, Glover R, Taylor CJ.
Gamma-ray modulation properties of
tungsten coded apertures for a novel mixedfield
imaging system. Journal of
Instrumentation. 2019 Feb 8;14(02):P02007.
[16] Knoll GF. Radiation detection and
measurement. John Wiley & Sons; 2010 Aug
16.
[17] Golub GH, Hansen PC, O'Leary DP. Tikhonov
regularization and total least squares. SIAM
journal on matrix analysis and applications.
1999;21(1):185-94.
F. Rahmani, P. Mansouri Journal of Nuclear Research and Applications Volume 4 Number 4 Autumn (2024) 11-19
19
[18] Katsikis VN, Pappas D, Petralias A. An
improved method for the computation of the
Moore–Penrose inverse matrix. Applied
Mathematics and Computation. 2011 Aug
1;217(23):9828-34.
[19] Cui J, Pratx G, Meng B, Levin CS. Distributed
MLEM: An iterative tomographic image
reconstruction algorithm for distributed
memory architectures. IEEE transactions on
medical imaging. 2013 Mar 15;32(5):957-67.
[20] Mihlin A, Levin CS. An MLEM method for joint
tissue activity distribution and photon
attenuation map reconstruction in PET.
In2013 IEEE nuclear science symposium and
medical imaging conference (2013 NSS/MIC)
2013 Oct 27 (pp. 1-3). IEEE.
[21] Carmi R, Shapiro O, Braunstein D. Resolution
enhancement of X-ray CT by spatial and
temporal MLEM deconvolution correction. In
IEEE Symposium Conference Record Nuclear
Science 2004. 2004 Oct 16 (Vol. 5, pp. 2765-
2768). IEEE.