Nuclear Science and Techniques

《核技术》(英文版) ISSN 1001-8042 CN 31-1559/TL     2019 Impact factor 1.556

Nuclear Science and Techniques ›› 2015, Vol. 26 ›› Issue (4): 040501 doi: 10.13538/j.1001-8042/nst.26.040501

• NUCLEAR PHYSICS AND INTERDISCIPLINARY RESEARCH • Previous Articles     Next Articles

Simulation of (p,d) reaction on RIBLL2 for study of tensor force

GUO Chen-Lei,1, 2, 3 ZHANG Gao-Long,1, 2, 3 QU Wei-Wei,2, 3 Satoru Terashima,2, 3 Isao Tanihata,2, 3, 4 LE Xiao-Yun 2, 3   

  1. 1State Key Laboratory of Software Development Environment, Beihang University, Beijing 100191, China
    2School of Physics and Nuclear Energy Engineering, Beihang University, Beijing 100191, China
    3International Research Center for Nuclei and Particles in the Cosmos, Beihang University, Beijing 100191, China
    4Research Center for Nuclear Physics, Osaka University, Osaka 567-0047, Japan
  • Contact: ZHANG Gao-Long E-mail:zgl@buaa.edu.cn
  • Supported by:

    Supported by National Natural Science Foundation of China (Nos.11475013, 11035007 and 11175011), State Key Laboratory of Software Development Environment (No. SKLSDE-2014ZX-08) as well as Fundamental Research Funds for the Central Universities and the Key Laboratory of High Precision Nuclear Spectroscopy, Institute of Modern Physics, Chinese Academy of Sciences

PDF ShareIt Export Citation
GUO Chen-Lei, ZHANG Gao-Long, QU Wei-Wei, Satoru Terashima, Isao Tanihata, LE Xiao-Yun . Simulation of (p,d) reaction on RIBLL2 for study of tensor force.Nuclear Science and Techniques, 2015, 26(4): 040501     doi: 10.13538/j.1001-8042/nst.26.040501

Abstract:

In order to study the effect of tensor force, we plan to perform a (p,d) reaction with a 400–1600MeV proton beam on the RIBLL2 at Lanzhou. Based on the experimental conditions of RIBLL2, a Monte Carlo method is used to simulate (p,d) reaction process. The distributions of primary beam and scattered deuterons are given on the target and at the F1, F2, F3, and F4 positions. Considering the yield of the deuteron, to separate the produced deuteron from the background particles, the target thickness is optimized. To obtain a clear particle identification spectrum by time of flight (TOF) and energy loss (ΔE), the distance between the two detectors, as well as the energy and timing resolution of detectors are simulated. As a result, the distance between F2 and F4 is fit for that of TOF. After taking into account the particle distribution at F4, both sizes of Multi-Wire Drift Chamber, namely MWDC2 and MWDC3, are selected to be 50mm ×50 mm.

Key words: Tensor force, Monte Carlo simulation, RIBLL2