• High Power Laser and Particle Beams
  • Vol. 34, Issue 10, 104005 (2022)
Chuwen Luo, Gangwen Liu, Weiwei Li, Nan Hu, Weimin Li, Zhenghe Bai, and Lin Wang*
Author Affiliations
  • National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230026, China
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    DOI: 10.11884/HPLPB202234.220140 Cite this Article
    Chuwen Luo, Gangwen Liu, Weiwei Li, Nan Hu, Weimin Li, Zhenghe Bai, Lin Wang. Parameters optimization considering intra-beam scattering in HALF lattice design[J]. High Power Laser and Particle Beams, 2022, 34(10): 104005 Copy Citation Text show less
    Magnet layout and linear optical functions of one period 7BA lattice
    Fig. 1. Magnet layout and linear optical functions of one period 7BA lattice
    Change of emittance and emittance growth rate with natural emittance
    Fig. 2. Change of emittance and emittance growth rate with natural emittance
    Equilibrium emittance vs SR damping time
    Fig. 3. Equilibrium emittance vs SR damping time
    Parameter optimization of storage ring circumference
    Fig. 4. Parameter optimization of storage ring circumference
    Magnet layout and linear optical functions of one period 6BAlattice
    Fig. 5. Magnet layout and linear optical functions of one period 6BAlattice
    Change of energy spread and horizontal emittance with beam current
    Fig. 6. Change of energy spread and horizontal emittance with beam current
    parametervalue
    beam energy2.4 GeV
    circumference672 m
    natural emittance24.7 pm·rad
    tune (H, V)71.30, 23.30
    natural chromaticity (H, V)−97, −110
    momentum compaction factor5×10−5
    natural energy spread7.97×10−4
    natural damping time (H, V, L)(37.7,58.8,40.8) ms
    energy loss per turn182.9 keV
    RF frequency500 MHz
    Table 1. Main parameters of the 7BA storage ring
    $ \kappa /\mathrm{{\text{%}}} $$ {\varepsilon }_{0} $/(pm·rad) $ \mathrm{\varepsilon } $/(pm·rad) $ {\sigma }_{\mathrm{p}0}/{10}^{-4} $$ {\sigma }_{\mathrm{p}}/{10}^{-4} $$ {\varepsilon }_{{x}0} $/(pm·rad) $ {\varepsilon }_{{x}} $/(pm·rad) $ ({\varepsilon }_{{x}}-{\varepsilon }_{{x}0})/{\varepsilon }_{{x}0} $
    1024.798.47.9711.523.292.52.99
    10024.777.77.9710.515.047.32.15
    Table 2. Equilibrium emittance of the storage ring under IBS effects
    parametervalue
    beam energy2.2 GeV
    circumference480 m
    natural emittance85.1 pm·rad
    tune (H, V)48.175,17.175
    natural chromaticity (H, V)−75, −59
    momentum compaction factor6.3×10−5
    natural energy spread6.6×10−4
    damping time (H, V, L)(22, 32.4, 21.2) ms
    energy loss per turn217.5 keV
    RF frequency500 MHz
    Table 3. Main parameters of the 6BA storage ring
    $ \kappa /\mathrm{{\text{%}}} $$ {\varepsilon }_{0} $/(pm·rad) $ \mathrm{\varepsilon } $/(pm·rad) $ {\sigma }_{\mathrm{p}0}/{10}^{-4} $$ {\sigma }_{\mathrm{p}}/{10}^{-4} $$ {\varepsilon }_{x0} $/(pm·rad) $ {\varepsilon }_{x} $/(pm·rad) $ ({\varepsilon }_{x}-{\varepsilon }_{x0})/{\varepsilon }_{x0} $
    1085.1185.46.69.1979.6173.41.178
    10085.1153.46.68.3550.290.50.803
    Table 4. Equilibrium emittance of the HALF storage ring under IBS effects
    $ \kappa /\mathrm{{\text{%}}} $$ {\varepsilon }_{0} $/(pm·rad) $ \mathrm{\varepsilon } $/(pm·rad) $ {\sigma }_{\mathrm{p}0}/{10}^{-4} $$ {\sigma }_{\mathrm{p}}/{10}^{-4} $$ {\varepsilon }_{x0} $/(pm·rad) $ {\varepsilon }_{x} $/(pm·rad) $ ({\varepsilon }_{x}-{\varepsilon }_{x0})/{\varepsilon }_{x0} $
    1084.21296.947.9878.5120.30.53
    10084.2110.56.947.5648.663.80.31
    Table 5. Equilibrium emittance of the HALF storage ring under IBS effects
    Chuwen Luo, Gangwen Liu, Weiwei Li, Nan Hu, Weimin Li, Zhenghe Bai, Lin Wang. Parameters optimization considering intra-beam scattering in HALF lattice design[J]. High Power Laser and Particle Beams, 2022, 34(10): 104005
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