2017
DOI: 10.1016/j.nimb.2017.02.032
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Design of the gas cell for the IGISOL facility at ELI-NP

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Cited by 14 publications
(14 citation statements)
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“…The optimal foil thickness is t ≈ 2µm. This value remains approximate when the other target geometry parameters change [16].…”
Section: Target Geometry Optimizationmentioning
confidence: 82%
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“…The optimal foil thickness is t ≈ 2µm. This value remains approximate when the other target geometry parameters change [16].…”
Section: Target Geometry Optimizationmentioning
confidence: 82%
“…Because of the space constraints at the first CSC location, the target length is fixed at its maximum value L t = 1 m [16]. Meanwhile, L t = 2 m is chosen for the second location.…”
Section: Target Geometry Optimizationmentioning
confidence: 99%
“…Accurate calculations for production cross sections of fragments produced by 238 U photofission at low energies over the whole energy region of the giant dipole resonance (GDR) are required for estimating the production yields of neutron-rich fragments and optimizing nuclear physics experiments at the planned IGISOL facility at ELI-NP. The gamma beam used at this IGISOL facility will cover a wide energy range between about 10 and 18.5 MeV [1][2][3].…”
Section: Calculations For the Production Of Neutron-rich Exotic Nuclementioning
confidence: 99%
“…As an example, production rates of 132 Sn and 134 Te in the 238 U targets with a total thickness of 251 µm are about 2×10 4 and 2×10 5 ions/s, respectively, according to calculations by the GIF 238 U parametrization for the IGISOL facility at ELI-NP. At the gamma production point, the total intensity of the gamma beam with a broad energy distribution between 10 and 18.5 MeV is conservatively estimated to be 5×10 10 γ/s for the above calculations of day-one experiments, while it can be improved to be around 1×10 12 γ/s for future experiments [1][2][3]. The 238 U target in the gas cell is placed around 7 m after this gamma production point.…”
Section: Z 62 and 80mentioning
confidence: 99%
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