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陈伟, 万鑫淼, 李智慧. 不同薄膜材料对α束流性能影响的模拟研究[J]. 原子核物理评论, 2021, 38(2): 147-152. DOI: 10.11804/NuclPhysRev.38.2021001
引用本文: 陈伟, 万鑫淼, 李智慧. 不同薄膜材料对α束流性能影响的模拟研究[J]. 原子核物理评论, 2021, 38(2): 147-152. DOI: 10.11804/NuclPhysRev.38.2021001
Wei CHEN, Xinmiao WAN, Zhihui LI. Simulation Study about the Effects of Different Film Materials on α Beam Properties[J]. Nuclear Physics Review, 2021, 38(2): 147-152. DOI: 10.11804/NuclPhysRev.38.2021001
Citation: Wei CHEN, Xinmiao WAN, Zhihui LI. Simulation Study about the Effects of Different Film Materials on α Beam Properties[J]. Nuclear Physics Review, 2021, 38(2): 147-152. DOI: 10.11804/NuclPhysRev.38.2021001

不同薄膜材料对α束流性能影响的模拟研究

Simulation Study about the Effects of Different Film Materials on α Beam Properties

  • 摘要: 由于回旋加速器引出的束流能量固定,为了满足不同实验对束流能量的不同需求,需要对束流的能量进行调节。为此,研究了利用薄膜材料对束流能量进行改变的可行性。用SRIM程序分析计算了30 MeV α束流(回旋加速器引出能量)穿过金刚石、铝和铜材料后的射程,确定了材料厚度与所需能量之间的关系。利用G4Beamline程序计算了束流经过薄膜后的相空间分布,分析了束流经过不同材料、降低到相同能量(9 MeV)后的横向、纵向发射度的变化,结果显示:束流在经过薄膜材料后,束斑大小几乎不发生改变,束流横向发射度的增长主要由散角的增加引起,其中金刚石薄膜引起的束流发射度增长最小,散角的均方根值约为16 mrad左右,且与初始束流的散角大小没有明显的依赖关系(初始散角均方根值小于1 mrad);不同材料引起的纵向能散均约为1 MeV(半高宽),与材料无关,只与束流的最终能量有关,降能越多,能散越大。此外,对于30 MeV的初始α束流,与金刚石、铜、铝等材料作用后,均会产生约109/μA的中子及γ粒子,在实际应用中应考虑相关的辐射防护问题。

     

    Abstract: The beam energy extracted from cyclotron is fixed, it is necessary to adjust it to meet different demands of different experiments. This study focuses on the feasibility of using thin film materials to change the beam energy. The ranges of 30 MeV α beams (extracted from cyclotron) in materials include diamond, aluminum and copper are calculated by the SRIM program, and the relationship between material thickness and the required beam energy is determined. The horizontal and vertical emittances of α beams, after being reduced to 9 MeV by interacting with different materials, are calculated by G4Beamline program. The following results are obtained: After penetrating the thin film materials, the size of beam spot approximately remained the same. The growth of beam transverse emittances is mainly caused by the increase of the divergence angles, among which the diamond film causes the least increase of beam emittance, and the root mean square value of the divergence angle is about 16 mrad. There is no significant dependency on the value of initial beam divergence angle (the root mean square value of initial divergence angle is less than 1 mrad). Vertical energy spread caused by different materials is about 1 MeV (FWHM) that is only determined by the final beam energy and has no connection with the kind of material. The more energy has lost, the greater the energy spread would be. Besides, the 30 MeV initial α beams interacting with thin film materials (diamond, copper, aluminum etc.) could produce about 109/μA neutrons and γ particles, so radiation protection must be considered in practical applications.

     

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