中国物理B ›› 2010, Vol. 19 ›› Issue (1): 10703-010703.doi: 10.1088/1674-1056/19/1/010703

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A new method for high-energy pulsed Gamma measurement within intense background x-rays

康克军1, 谭新建2, 欧阳晓平2, 王群书2, 宋朝晖3, 夏良斌3   

  1. (1)Department of Engineering Physics, Tsinghua University, Key Laboratory of Particle & Radiation Imaging (Tsinghua University), Ministry of Education, Beijing 100084, China; (2)Department of Engineering Physics, Tsinghua University, Key Laboratory of Particle & Radiation Imaging (Tsinghua University), Ministry of Education, Beijing 100084, China;Northwest Institute of Nuclear Technology, Xi'an 710024, China; (3)Northwest Institute of Nuclear Technology, Xi'an 710024, China
  • 收稿日期:2009-05-03 修回日期:2009-06-09 出版日期:2010-01-15 发布日期:2010-01-15

A new method for high-energy pulsed Gamma measurement within intense background x-rays

Tan Xin-Jian(谭新建)a)b), Ouyang Xiao-Ping(欧阳晓平) a)b)†, Wang Qun-Shu(王群书) a)b), Song Zhao-Hui(宋朝晖)b), Kang Ke-Jun(康克军) a), and Xia Liang-Bin(夏良斌)b)   

  1. a Department of Engineering Physics, Tsinghua University, Key Laboratory of Particle & Radiation Imaging (Tsinghua University), Ministry of Education, Beijing 100084, China; b Northwest Institute of Nuclear Technology, Xi'an 710024, China
  • Received:2009-05-03 Revised:2009-06-09 Online:2010-01-15 Published:2010-01-15

摘要: The accelerator-generating 6.13~MeV pulsed Gamma by 19F(p, αγ )160 reaction usually synchronizes with an intense bremsstrahlung x-ray which has a maximum energy of 1~MeV. This paper proposes a new method, named the scattering and absorbing method, to diagnose the 6.13~MeV Gamma. This method includes two parts: the detector and a scatterer placed in front of the detector. The detector converts the Gamma to electrons and then collects the electrons by a scintillator. In order to restrain the interference of the low-energy background, the scintillator collects the electrons at a small angle. The scintillator is wrapped with electro-absorbing material to absorb the low-energy electrons generated by background x-rays. The theoretical sensitivity ratio of 6.13~MeV Gamma to 1~MeV x-rays is greater than 150. The scatterer is a pretreatment tool to scatter some background x-rays away from the radial beam before they enter the detector. By varying the length, the scatterer can reduce the background x-rays to an acceptable level for the detector.

Abstract: The accelerator-generating 6.13 MeV pulsed Gamma by 19F(p, $\alpha\gamma$)160 reaction usually synchronizes with an intense bremsstrahlung x-ray which has a maximum energy of 1~MeV. This paper proposes a new method, named the scattering and absorbing method, to diagnose the 6.13 MeV Gamma. This method includes two parts: the detector and a scatterer placed in front of the detector. The detector converts the Gamma to electrons and then collects the electrons by a scintillator. In order to restrain the interference of the low-energy background, the scintillator collects the electrons at a small angle. The scintillator is wrapped with electro-absorbing material to absorb the low-energy electrons generated by background x-rays. The theoretical sensitivity ratio of 6.13 MeV Gamma to 1 MeV x-rays is greater than 150. The scatterer is a pretreatment tool to scatter some background x-rays away from the radial beam before they enter the detector. By varying the length, the scatterer can reduce the background x-rays to an acceptable level for the detector.

Key words: high energy pulsed Gamma, background, scattering, absorbing

中图分类号:  (X- and γ-ray sources, mirrors, gratings, and detectors)

  • 07.85.Fv
23.20.Lv (γ-transitions and level energies) 25.40.Lw (Radiative capture) 27.20.+n (6 ≤ A ≤ 19) 29.40.Mc (Scintillation detectors)