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Background Simulation of a Fission Fragment Chamber in the Experiment of ^(209)Bi(e,e’K^+)^(209)_ ΛPb

Background Simulation of a Fission Fragment Chamber in the Experiment of ^(209)Bi(e,e’K^+)^(209)_ ΛPb
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摘要 An experiment for measuring the hyperon-related fission rate was carried out with the reaction 209^Bi(e, e'K^+)209^hPb at the Thomas Jefferson National Laboratory (Jlab). In the experiment, the performance of the fission fragment detector (FFD) was dramaticlly crashed by the background particles in comparison with that during the test without beam. The scattering of the high intensity (500 nA) primary electrons was the dominant cause. Using the GEANT4 toolkit, this report simulates the experimental situation of the target chamber in which the FFD was located. The simulation results indicate that the background particles were dominantly (~ electrons, and protons and alpha particles were the important heavy background particles. The performance of the multi-wire proportional chambers (MWPCs) depends not only on the background-particle intensity but also the current density, which was also given by the simulation code. Furthermore, the measures to suppress the background particles were also investigated with the simulation code. An experiment for measuring the hyperon-related fission rate was carried out with the reaction 209^Bi(e, e'K^+)209^hPb at the Thomas Jefferson National Laboratory (Jlab). In the experiment, the performance of the fission fragment detector (FFD) was dramaticlly crashed by the background particles in comparison with that during the test without beam. The scattering of the high intensity (500 nA) primary electrons was the dominant cause. Using the GEANT4 toolkit, this report simulates the experimental situation of the target chamber in which the FFD was located. The simulation results indicate that the background particles were dominantly (~ electrons, and protons and alpha particles were the important heavy background particles. The performance of the multi-wire proportional chambers (MWPCs) depends not only on the background-particle intensity but also the current density, which was also given by the simulation code. Furthermore, the measures to suppress the background particles were also investigated with the simulation code.
出处 《Plasma Science and Technology》 SCIE EI CAS CSCD 2012年第5期415-418,共4页 等离子体科学和技术(英文版)
基金 supported by the Fundamental Research Funds for the Central Universities of China (No.HEUCF101501) the Fundamental Research Funds of Harbin Engineering University of China (No.002150260713)
关键词 fission fragments HYPERON background particles Monte Carlo simulation fission fragments, hyperon, background particles, Monte Carlo simulation
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  • 1Cohen J. 1990, Prog. Part. Nucl. Phys., 25:139.
  • 2Kumagai-Fuse I, Okabe I, Akaishi Y. 1995, Phys. Lett. B, 345:386.
  • 3Osetand E, Ramos A. 1998, Prog. Part. Nucl. Phys., 41:191.
  • 4Schiavilla R, Carlson J, Paris M. 2004, Phys. Rev. C, 70:044007.
  • 5Wood C S, Bennett S C, Cho D, et al. 1997, Science, 275:1759.
  • 6Kamys B, Kulessa P, Ohm H, et al. 2001, Eur. Phys. J. A, 11:1.
  • 7Kulessa P, Rudy Z, Hartmann M. 1998, Phys. Lett. B, 427:403.
  • 8Kulessa P, Cassing W, Jarczyk L. 2002, ACTA PHYSIC APOLONICA B, 33:603.
  • 9Briickner W. 1978, Phys. Lett. B, 79:157.
  • 10May M, Piekarz H, Chrien R E. 1981, Phys. Rev. Lett., 47:1106.

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