Cyclotrons2016 - List of Authors (Mousavinia, M.)

Paper	Title	Page
MOP03	Developed Numerical Code Based on the Effects of Space Charge in Central Region of 10 MeV Cyclotron	49
	M. Afkhami Karaei, H. Afarideh, S. Azizpourian, M. Mousavinia, R. Solhju, F. Taft AUT, Tehran, Iran J.-S. Chai, M. Ghergherehchi SKKU, Suwon, Republic of Korea
	To study of space charge effects in 10 MeV cyclotron of Amirkabir University of Technology the C++ code is developed. This cyclotron is designed to accelerate H⁻ up to 10MeV energy. The important components of cyclotron that effect on calculations of space charge include four sector magnets, 2 RF cavities with 71MHz frequency and internal PIG ion source. Equations of motion and effects of charged particles in electromagnetic field of accelerator are integrated in C++ code. The conventional method, 4-order Runge-Kutta, is used to solve the equations. The results of calculations show space charge effects of beam particles on each other in accelerating process.
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MOP22	Simulation of Optimum Thickness and Configuration of 10 MeV Cyclotron Shield	110
	S. Azizpourian, H. Afarideh, M. Afkhami Karaei, M. Mousavinia AUT, Tehran, Iran F. Abbasi Davani Shahid Beheshti University, Tehran, Iran
	Baby Cyclotrons that made in Self-shield type have been employed for use in Medical center for the diagnosis of cancer diseases by positron emission tomography (PET) system. Here in we have done a discussion on gamma and neutron dose rates at a distance of one meter outside of the cyclotron shielding. This shield consist of Lead, polyethylene borated (10% Boron) layers from inside to outside respectively. With increasing the thickness of lead and polyethylene we will see a decrease in the gamma and neutron dose which received by the water phantom at a distance of one meter outside from the surface of the shield of the cyclotron. Note that the gamma and neutron dose at the beginning (without any shielding) was on the order of several thousand μSv per hour that by achieve to a certain amount of thickness of the shield, the dose was reduced to below of the limited level. In this study, the MCNPX Code has been used. In MCNPX Code that used the variance reduction techniques for decreasing relative errors of calculation which was a good method for this case study.
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WEB03	Design and Simulation of Cavity for 18 MeV Cyclotron	267
	M. Mousavinia, H. Afarideh AUT, Tehran, Iran M. Ghergherehchi SKKU, Suwon, Republic of Korea
	RF system is the key part of cyclotron and cavity is the key part of RF system. The basic parameters of cavity design are the resonant frequency , dee voltage , RF phase and RF power. Proper operation of cavity depends on the suitable voltage distribution in accelerating gap, phase stability in cavity and as well as optimal scattering parameters. In this simulation by using CST MWS, different parts of cavity such as stam and dee are optimized to achieved optimum dimesnsions for desired resonant freq, dee voltage and RF power. Properties of designed cavity including: resonant frequency at 64.3 MHz, dee voltage is 45 kV and RF power is 11 kW.
	Slides WEB03 [3.767 MB]
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Paper

Title

Page

Developed Numerical Code Based on the Effects of Space Charge in Central Region of 10 MeV Cyclotron

49

M. Afkhami Karaei, H. Afarideh, S. Azizpourian, M. Mousavinia, R. Solhju, F. Taft
AUT, Tehran, Iran
J.-S. Chai, M. Ghergherehchi
SKKU, Suwon, Republic of Korea

To study of space charge effects in 10 MeV cyclotron of Amirkabir University of Technology the C++ code is developed. This cyclotron is designed to accelerate H⁻ up to 10MeV energy. The important components of cyclotron that effect on calculations of space charge include four sector magnets, 2 RF cavities with 71MHz frequency and internal PIG ion source. Equations of motion and effects of charged particles in electromagnetic field of accelerator are integrated in C++ code. The conventional method, 4-order Runge-Kutta, is used to solve the equations. The results of calculations show space charge effects of beam particles on each other in accelerating process.

Export •

reference for this paper using ※ BibTeX, ※ LaTeX, ※ Text/Word, ※ RIS, ※ EndNote (xml)

MOP22

Simulation of Optimum Thickness and Configuration of 10 MeV Cyclotron Shield

110

S. Azizpourian, H. Afarideh, M. Afkhami Karaei, M. Mousavinia
AUT, Tehran, Iran
F. Abbasi Davani
Shahid Beheshti University, Tehran, Iran

Baby Cyclotrons that made in Self-shield type have been employed for use in Medical center for the diagnosis of cancer diseases by positron emission tomography (PET) system. Here in we have done a discussion on gamma and neutron dose rates at a distance of one meter outside of the cyclotron shielding. This shield consist of Lead, polyethylene borated (10% Boron) layers from inside to outside respectively. With increasing the thickness of lead and polyethylene we will see a decrease in the gamma and neutron dose which received by the water phantom at a distance of one meter outside from the surface of the shield of the cyclotron. Note that the gamma and neutron dose at the beginning (without any shielding) was on the order of several thousand μSv per hour that by achieve to a certain amount of thickness of the shield, the dose was reduced to below of the limited level. In this study, the MCNPX Code has been used. In MCNPX Code that used the variance reduction techniques for decreasing relative errors of calculation which was a good method for this case study.

Export •

reference for this paper using ※ BibTeX, ※ LaTeX, ※ Text/Word, ※ RIS, ※ EndNote (xml)

WEB03

Design and Simulation of Cavity for 18 MeV Cyclotron

267

M. Mousavinia, H. Afarideh
AUT, Tehran, Iran
M. Ghergherehchi
SKKU, Suwon, Republic of Korea

RF system is the key part of cyclotron and cavity is the key part of RF system. The basic parameters of cavity design are the resonant frequency , dee voltage , RF phase and RF power. Proper operation of cavity depends on the suitable voltage distribution in accelerating gap, phase stability in cavity and as well as optimal scattering parameters. In this simulation by using CST MWS, different parts of cavity such as stam and dee are optimized to achieved optimum dimesnsions for desired resonant freq, dee voltage and RF power. Properties of designed cavity including: resonant frequency at 64.3 MHz, dee voltage is 45 kV and RF power is 11 kW.

Slides WEB03 [3.767 MB]

Export •

reference for this paper using ※ BibTeX, ※ LaTeX, ※ Text/Word, ※ RIS, ※ EndNote (xml)