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G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M. Saboor / International
Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622
www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp.1477-1479
1477 | P a g e
The Optimization of Gamma Camera Using Changed the Area of
Semiconductor Detectors by MCNP Code
G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M.
Saboor
Department of Physics, Payam Noor University of Mashhad, Mashhad, Iran
Abstract
In this paper we tried to substitute an
appropriate detector instead of NaI. The features
of semiconductor detectors were studied to find a
detector which works at the ordinary
temperature, has less FWHM and more
resolution. Therefore HgI2 and CZT detectors
were selected and studied. The gamma camera
with three difference detectors (NaI, HgI2 and
CZT detectors) were simulated. We have shown
that the resolution of HgI2 and CZT detectors are
better than NaI. Studding of area variation of
CZT, HgI2 and NaI detectors, the minimum
FWHM and maximum resolution obtained at4.8
mm × 4.8 mm area. Finally the area of detectors
hole were modified in order to gain the best
possible pictures.
Keywords-:Semiconductor; gamma camera;
detector.
I. Introduction
In this paper we tried to substitute an
appropriate detector instead of NaI that has better
qualities as follows.
a- It should have more sensitivity by comparison with
NaI.
b- It should record more radiations for a given
radioactivity and decrease the patient’s exposure by
improving the detector efficiency , practically.
c- It should be able to do detection at the ordinary
room temperature.
d- It should has better efficiency.
e- It should has better resolution relative to NaI or in
other word its FWHM is smaller than NaI FWHM.
II. Simulating gamma camera by NaI
detector
In this experiment, we have simulated a
gamma camera that consists of a tungesten
collimator, NaI(TL) detector and a photomultiplier
tube [1].
talium impurity in NaI(TL) detector results in more
light in photography and because the amount of
talium in sodium crystal was negligible it has been
left out.
We have defined some parameters in simulation
programs as the following: the collimator is 2.504 cm
high, every wall is of 0.16 cm tick with octagon holes
that the distance between two sides is 0.111 cm. the
NaI detector has a rectangular cubic shape. It is 61.4
cm long, 61.4 cm width and 0.95 cm high. After the
detector there is a photomultiplier tube and this
arrangement comprises the gamma camera [1-6].
While taking pictures the gamma camera is placed 10
cm above the capillary tube and NaI detector is
supposed as a lattice structure crystal that consists of
128*128 single crystals [1].
Figure 1. The cross section of the SIEMENS
gamma camera.
III. The comparison between NaI, CZT
and HgI2 simulation results
By comparing the results that are gained by
simulating NaI, CZT and HgI2 detectors it can be
shown that the FWHM of CZT and HgI2 detectors
are lower than sodium iodide FWHM and therefor
the resolution of them is more than sodium iodide.
Table 1. The results of gamma camera with
different detectors.
The FWHM of
photopeak(KeV)
Detector type
23.3
16.5
10.5
NaI
HgI2
CZT
In this stage the size, the shape and the
material type of collimator and also the detector
height(thickness) are constant but the size (area) of
detector is variable [4,5].
IV. The investigation of the variations in
the size of HgI2 Detector
By keeping the height of HgI2 detector
constant we investigate the variations of the detector
size[5].
G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M. Saboor / International
Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622
www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp.1477-1479
1478 | P a g e
Table 2. The results of gamma camera simulation
by changing the size of HgI2 detector.
The
FWHM of
photopeak
(KeV)
the size and the
height of detector
(mm)
the sizes of
collimator
(mm)
18.5
16.5
42.5
3.6×3.6 and the
height 9.5
4.8×4.86 and the
height 9.5
9.6×9.6 6 and the
height 9.5
The Aperture (hole)
diameter 1.11, the
height 24.05
The Aperture (hole)
diameter 1.11, the
height 24.05
The Aperture (hole)
diameter 1.11, the
height 24.05
0 20 40 60 80 100
15
20
25
30
35
40
45
FWHM(KeV)
Area(mm2)
Figure 2. FWHM versus the area of HgI2
detector.
V. The investigation of the variations in
the size of CZT detector
By keeping the height of CZT detector we
study the variations of the detector size [2,3].
Table 3. the results of gamma camera simulation
by changing the size of CZT detector.
The
FWHM of
photopeak
(KeV)
the size and the
height of
detector
(mm)
the sizes of
collimator
(mm)
26.1
10.5
21
3.6×3.6 and the
height 9.5
4.8×4.86 and the
height 9.5
9.6×9.6 6 and the
height 9.5
The Aperture
(hole) diameter
1.11, the height
24.05
The Aperture
(hole) diameter
1.11, the height
24.05
The Aperture
(hole) diameter
1.11, the height
24.05
0 20 40 60 80 100
10
12
14
16
18
20
22
24
26
28
FWHM(KeV)
Area(mm2)
Figure 3. FWHM versus the area of CZT
detector.
VI. The investigation of the variations in
the size of NaI detector
By keeping the height of NaI detector
constant we study the variations of the detector size
[1].
Table 4. the results of gamma camera simulation
by changing the size of NaI detector.
The
FWHM of
photopeak
(KeV)
the size and the
height of
detector
(mm)
the sizes of
collimator
(mm)
24
23.3
32.3
3.6×3.6 and the
height 9.5
4.8×4.86 and the
height 9.5
9.6×9.6 6 and the
height 9.5
The Aperture
(hole) diameter
1.11, the height
24.05
The Aperture
(hole) diameter
1.11, the height
24.05
The Aperture
(hole) diameter
1.11, the height
24.05
0 20 40 60 80 100
22
24
26
28
30
32
34
FWHM(KeV)
Area(mm2)
Figure 4. The FWHM against the size NaI
detector
G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M. Saboor / International
Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622
www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp.1477-1479
1479 | P a g e
VII. Conclusion
According to the obtained results , the full
width at half maximum of CZT and HgI2 is less than
NaI detector and therefor their resolution. Also by
studying the size variations in these three detectors,
the least FWHM and the highest resolution for the
size of 4.8mm ×4.8mm was gained. In the new
generation of gamma cameras that are designed for
taking pictures of a human’s whole body, the
standard size of detector crystal is 4.8mm×4.8mm in
order to the gamma rays scatter just one time and
there exist a high probability for leaving off the
crystal before they could react again. and this
conforms to the obtained result. Finally the best
picture was obtained after optimizing the detector
features.
References
[1]. Mc Connell M.L & et al , "Three-Dimential
imaging efficiency performance of coplanar
cdznte strip detectors", proceeding of SPIE
vol. 414/(2000).
[2]. Scheiberch & et al,"Medical applications of
cdte and cdznte detectors", Nuclear
Instruments and Metods in physics Research
A 458 (2001) 12-25.
[3]. EisenY & et al, CdTe and CdTeZnMaterial
D.J, Smith R, Collins D.A, Phillips S.W, "
Evaluation of small cadmium zink Telluride
detector for scintimammography". The
Journal of Nuclear Medicine Vol. 440 NO
40 (April 2003).
[4]. Scheir.C" CdTe and CdTeZn detectors in
nuclear medicin", Nuclear Instruments and
Metods in Physics Research A 448
(2000)513-524.
[5]. Fred P. Vaccaro & et al, The Long-term
Spectral Stability of HgI2 Gamma-ray
detectors, Proc. SPIE Vol. 4507, p. 108-
118(2001).
[6]. Sanaei Nameghi. A, “the study of
appropriate semiconductor detectors as a
substitute for gamma camera detector by
using montecarlo simulation’’,thesis fo r
master of science degree, Department of
Physics, payam noor University of
Mashhad,2010.

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Ia3414771479

  • 1. G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M. Saboor / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp.1477-1479 1477 | P a g e The Optimization of Gamma Camera Using Changed the Area of Semiconductor Detectors by MCNP Code G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M. Saboor Department of Physics, Payam Noor University of Mashhad, Mashhad, Iran Abstract In this paper we tried to substitute an appropriate detector instead of NaI. The features of semiconductor detectors were studied to find a detector which works at the ordinary temperature, has less FWHM and more resolution. Therefore HgI2 and CZT detectors were selected and studied. The gamma camera with three difference detectors (NaI, HgI2 and CZT detectors) were simulated. We have shown that the resolution of HgI2 and CZT detectors are better than NaI. Studding of area variation of CZT, HgI2 and NaI detectors, the minimum FWHM and maximum resolution obtained at4.8 mm × 4.8 mm area. Finally the area of detectors hole were modified in order to gain the best possible pictures. Keywords-:Semiconductor; gamma camera; detector. I. Introduction In this paper we tried to substitute an appropriate detector instead of NaI that has better qualities as follows. a- It should have more sensitivity by comparison with NaI. b- It should record more radiations for a given radioactivity and decrease the patient’s exposure by improving the detector efficiency , practically. c- It should be able to do detection at the ordinary room temperature. d- It should has better efficiency. e- It should has better resolution relative to NaI or in other word its FWHM is smaller than NaI FWHM. II. Simulating gamma camera by NaI detector In this experiment, we have simulated a gamma camera that consists of a tungesten collimator, NaI(TL) detector and a photomultiplier tube [1]. talium impurity in NaI(TL) detector results in more light in photography and because the amount of talium in sodium crystal was negligible it has been left out. We have defined some parameters in simulation programs as the following: the collimator is 2.504 cm high, every wall is of 0.16 cm tick with octagon holes that the distance between two sides is 0.111 cm. the NaI detector has a rectangular cubic shape. It is 61.4 cm long, 61.4 cm width and 0.95 cm high. After the detector there is a photomultiplier tube and this arrangement comprises the gamma camera [1-6]. While taking pictures the gamma camera is placed 10 cm above the capillary tube and NaI detector is supposed as a lattice structure crystal that consists of 128*128 single crystals [1]. Figure 1. The cross section of the SIEMENS gamma camera. III. The comparison between NaI, CZT and HgI2 simulation results By comparing the results that are gained by simulating NaI, CZT and HgI2 detectors it can be shown that the FWHM of CZT and HgI2 detectors are lower than sodium iodide FWHM and therefor the resolution of them is more than sodium iodide. Table 1. The results of gamma camera with different detectors. The FWHM of photopeak(KeV) Detector type 23.3 16.5 10.5 NaI HgI2 CZT In this stage the size, the shape and the material type of collimator and also the detector height(thickness) are constant but the size (area) of detector is variable [4,5]. IV. The investigation of the variations in the size of HgI2 Detector By keeping the height of HgI2 detector constant we investigate the variations of the detector size[5].
  • 2. G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M. Saboor / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp.1477-1479 1478 | P a g e Table 2. The results of gamma camera simulation by changing the size of HgI2 detector. The FWHM of photopeak (KeV) the size and the height of detector (mm) the sizes of collimator (mm) 18.5 16.5 42.5 3.6×3.6 and the height 9.5 4.8×4.86 and the height 9.5 9.6×9.6 6 and the height 9.5 The Aperture (hole) diameter 1.11, the height 24.05 The Aperture (hole) diameter 1.11, the height 24.05 The Aperture (hole) diameter 1.11, the height 24.05 0 20 40 60 80 100 15 20 25 30 35 40 45 FWHM(KeV) Area(mm2) Figure 2. FWHM versus the area of HgI2 detector. V. The investigation of the variations in the size of CZT detector By keeping the height of CZT detector we study the variations of the detector size [2,3]. Table 3. the results of gamma camera simulation by changing the size of CZT detector. The FWHM of photopeak (KeV) the size and the height of detector (mm) the sizes of collimator (mm) 26.1 10.5 21 3.6×3.6 and the height 9.5 4.8×4.86 and the height 9.5 9.6×9.6 6 and the height 9.5 The Aperture (hole) diameter 1.11, the height 24.05 The Aperture (hole) diameter 1.11, the height 24.05 The Aperture (hole) diameter 1.11, the height 24.05 0 20 40 60 80 100 10 12 14 16 18 20 22 24 26 28 FWHM(KeV) Area(mm2) Figure 3. FWHM versus the area of CZT detector. VI. The investigation of the variations in the size of NaI detector By keeping the height of NaI detector constant we study the variations of the detector size [1]. Table 4. the results of gamma camera simulation by changing the size of NaI detector. The FWHM of photopeak (KeV) the size and the height of detector (mm) the sizes of collimator (mm) 24 23.3 32.3 3.6×3.6 and the height 9.5 4.8×4.86 and the height 9.5 9.6×9.6 6 and the height 9.5 The Aperture (hole) diameter 1.11, the height 24.05 The Aperture (hole) diameter 1.11, the height 24.05 The Aperture (hole) diameter 1.11, the height 24.05 0 20 40 60 80 100 22 24 26 28 30 32 34 FWHM(KeV) Area(mm2) Figure 4. The FWHM against the size NaI detector
  • 3. G. Robatjazi, A. Sanaei Nameghi, P. Parvaresh, M. R. Benam and M. Saboor / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp.1477-1479 1479 | P a g e VII. Conclusion According to the obtained results , the full width at half maximum of CZT and HgI2 is less than NaI detector and therefor their resolution. Also by studying the size variations in these three detectors, the least FWHM and the highest resolution for the size of 4.8mm ×4.8mm was gained. In the new generation of gamma cameras that are designed for taking pictures of a human’s whole body, the standard size of detector crystal is 4.8mm×4.8mm in order to the gamma rays scatter just one time and there exist a high probability for leaving off the crystal before they could react again. and this conforms to the obtained result. Finally the best picture was obtained after optimizing the detector features. References [1]. Mc Connell M.L & et al , "Three-Dimential imaging efficiency performance of coplanar cdznte strip detectors", proceeding of SPIE vol. 414/(2000). [2]. Scheiberch & et al,"Medical applications of cdte and cdznte detectors", Nuclear Instruments and Metods in physics Research A 458 (2001) 12-25. [3]. EisenY & et al, CdTe and CdTeZnMaterial D.J, Smith R, Collins D.A, Phillips S.W, " Evaluation of small cadmium zink Telluride detector for scintimammography". The Journal of Nuclear Medicine Vol. 440 NO 40 (April 2003). [4]. Scheir.C" CdTe and CdTeZn detectors in nuclear medicin", Nuclear Instruments and Metods in Physics Research A 448 (2000)513-524. [5]. Fred P. Vaccaro & et al, The Long-term Spectral Stability of HgI2 Gamma-ray detectors, Proc. SPIE Vol. 4507, p. 108- 118(2001). [6]. Sanaei Nameghi. A, “the study of appropriate semiconductor detectors as a substitute for gamma camera detector by using montecarlo simulation’’,thesis fo r master of science degree, Department of Physics, payam noor University of Mashhad,2010.