RF Electro Magnetic Field Effects on the 571.2MHz Normal Conducting Subharmonic Buncher

PEI Shi-Lun; WANG Shu-Hong

Chinese Physics C> 2005, Vol. 29> Issue(9) : 912-917

RF Electro Magnetic Field Effects on the 571.2MHz Normal Conducting Subharmonic Buncher

PEI Shi-Lun ^, ,
WANG Shu-Hong

Institute of High Energy Physics, CAS, Beijing 100049, China2 Graduate School of Chinese Academy of Sciences, Beijing 100049, China

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Abstract：
Usually, the RF electro-magnetic field can affect the resonant cavity in two ways. One is the heat loading to the cavity due to the RF power dissipation, and another is the Lorenz force due to the high RF surface field. In this paper, the RF electro-magnetic field effects on the Sub-harmonic Buncher 2 (SHB2) are described and some results presented and discussed. The analyses of the RF electro-magnetic field effects were performed by coupled simulations with finite difference method software-Superfish and finite element method software--ANSYS. In addition, the RF electro-magnetic field effects on the Sub-harmonic Buncher 1 (SHB1) are also described.

References

[1]

. PEI Shi-Lun, WANG Shu-Hong, GU Peng-Da et al. High Energy Phys. and Nucl. Phys., 2004, 28(5): 549(in Chinses)(裴士伦,王书鸿,顾鹏达等.高能物理与核物理,2004, 28(5):(549)2. Joshi S C, Paramonov V, Skassyrskaya A et al. The Complete 3-D Coupled RF-Thermal-Structural-RF Analysis Procedure for a Normal Conducting Accelerating Structure for High Intensity Hadron Linac. Proc. of LINAC 2002.Gyeongju, Korea. 2163. Billen J H, Young L M . Possion Superfish: LA-UR-96-1834. Los Alamos National Laboratory, 20024. ANSYS Collaboration. Manual of Electromagnetic Field Analysis in ANSYS. America: ANSYS Inc., 20005. Hartman N, Rimmer R A. Electromagnetic, Thermal, and Structural Anasysis of RF Cavities Using ANSYS. Proc. of the 2001 Particle Accelerator Conference. Chicago, America6. ZHOU Ke-Ding, ZHANG Su-Wen, DONG Tian-Lin et al. Electromagnetic Field Theory Fundamentals. Beijing:China Machine Press, 2000. 214(in Chinses)(周克定,张肃文,董天临等.北京:机械工业出版社, 2000.214)7. XU Zhao-Jun. Heat Transfer Theory. Beijing: China Ma-chine Press, 1980. 57(in Chinses)(许肇钧.北京:机械工业出版社,1980. 57) 8. David M. Pozar. Microwave Engineering(2nd Edition). New York: John Wiley Sons, 1998. 3419. PEI Shi-Lun, WANG Shu-Hong, GU Peng-Da. Atomic Energy Science and Technology, Accepted(in Chinses)(裴士伦,王书鸿,顾鹏达.原子能科学技术;已接收)10. PEI Shi-Lun, WANG Shu-Hong, GU Peng-da et al. High Power Laser and Particle Beams, 2004, 16(6): 795(in Chinses)(裴士伦,王书鸿,顾鹏达等.强激光与粒子束,2004, 16(6):795) 11. PEI Shi-Lun. Some Topics of BEPC/ Linac: IHEP-AC-MW-Note/2004-02. Internal Report, IHEP, March, 2004

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PEI Shi-Lun and WANG Shu-Hong. RF Electro Magnetic Field Effects on the 571.2MHz Normal Conducting Subharmonic Buncher[J]. Chinese Physics C, 2005, 29(9): 912-917.

PEI Shi-Lun and WANG Shu-Hong. RF Electro Magnetic Field Effects on the 571.2MHz Normal Conducting Subharmonic Buncher[J]. Chinese Physics C, 2005, 29(9): 912-917. shu

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Received: 2005-01-05
Revised: 1900-01-01

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通讯作者: 陈斌, bchen63@163.com

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沈阳化工大学材料科学与工程学院沈阳 110142

RF Electro Magnetic Field Effects on the 571.2MHz Normal Conducting Subharmonic Buncher

Corresponding author: PEI Shi-Lun,

Institute of High Energy Physics, CAS, Beijing 100049, China2 Graduate School of Chinese Academy of Sciences, Beijing 100049, China

Received Date: 2005-01-05

Accepted Date: 1900-01-01

Available Online: 2005-09-05

Abstract: Usually, the RF electro-magnetic field can affect the resonant cavity in two ways. One is the heat loading to the cavity due to the RF power dissipation, and another is the Lorenz force due to the high RF surface field. In this paper, the RF electro-magnetic field effects on the Sub-harmonic Buncher 2 (SHB2) are described and some results presented and discussed. The analyses of the RF electro-magnetic field effects were performed by coupled simulations with finite difference method software-Superfish and finite element method software--ANSYS. In addition, the RF electro-magnetic field effects on the Sub-harmonic Buncher 1 (SHB1) are also described.

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RF Electro Magnetic Field Effects on the 571.2MHz Normal Conducting Subharmonic Buncher

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