INCREASE OF BEAM PROJECTIVE EMITTANCE IN SYSTEM WITH DISPERSION

  • In this paper, the increase of beam projective emittance caused by the momentum dispersion in the transport systems is discussed, and the incrementary ratio is derived. If the bending plane is (XOZ), the incrementary ratio of the transversal emittance is

    and the longitudinal one is

    Here εx0 and εz0 are original emittances in the x-direction and z-direction respectively, (Δp/p)maxis beam momentum spread βxf, αxf, γxf being acceptance parameters of the system in x-direction for betatron oscillations, η and η' are dispersion function and its derivative.
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  • [1] K. L. Brown, SL.AC-TS (1972),[2] K. L. Brown, et. al. CERN-73-16 (1973).[3] 魏开煌、陈伯飞等, 束流输运系统计算程序《TR(1)》汇编, 中国科学院高能物理研究所(1979).[4] 魏开爆, 带电束流传输理论, 北京电机工程学会(1980).
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WEI Kai-Yu. INCREASE OF BEAM PROJECTIVE EMITTANCE IN SYSTEM WITH DISPERSION[J]. Chinese Physics C, 1983, 7(5): 589-597.
WEI Kai-Yu. INCREASE OF BEAM PROJECTIVE EMITTANCE IN SYSTEM WITH DISPERSION[J]. Chinese Physics C, 1983, 7(5): 589-597. shu
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Received: 1900-01-01
Revised: 1900-01-01
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INCREASE OF BEAM PROJECTIVE EMITTANCE IN SYSTEM WITH DISPERSION

    Corresponding author: WEI Kai-Yu,
  • Institute of High Energy Physics, Academia sinica

Abstract: In this paper, the increase of beam projective emittance caused by the momentum dispersion in the transport systems is discussed, and the incrementary ratio is derived. If the bending plane is (XOZ), the incrementary ratio of the transversal emittance is

and the longitudinal one is

Here εx0 and εz0 are original emittances in the x-direction and z-direction respectively, (Δp/p)maxis beam momentum spread βxf, αxf, γxf being acceptance parameters of the system in x-direction for betatron oscillations, η and η' are dispersion function and its derivative.

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