2013
DOI: 10.1007/s00601-013-0605-5
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Status of Rare Isotope Science Project in Korea

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Cited by 24 publications
(8 citation statements)
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“…The G4-BIN predictions at the energy of $200 MeV/u agree well with the 950 MeV/u data regardless of the atomic number Z. If the aforementioned experimentally observed energy-independence of the cross section still holds down to 200 MeV/u, we expect a good agreement will be obtained between the data and the G4-BIN predictions at 200 MeV/u, for which the beam energy is being planned for RAON [11][12][13]. In fact, G4-BIN shows a small energy-dependence.…”
Section: Benchmark Test Of Simulation Methods For the Production Crosmentioning
confidence: 63%
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“…The G4-BIN predictions at the energy of $200 MeV/u agree well with the 950 MeV/u data regardless of the atomic number Z. If the aforementioned experimentally observed energy-independence of the cross section still holds down to 200 MeV/u, we expect a good agreement will be obtained between the data and the G4-BIN predictions at 200 MeV/u, for which the beam energy is being planned for RAON [11][12][13]. In fact, G4-BIN shows a small energy-dependence.…”
Section: Benchmark Test Of Simulation Methods For the Production Crosmentioning
confidence: 63%
“…Their results indicate that TSRS can be indeed effective in producing more exotic medium-mass neutron-rich isotopes. According to the design summary of RAON in Korea [11][12][13], the expected intensity of 132 Sn can be as large as about 10 8 particles per second (pps). It is the unique feature of RAON that the isotopes generated by ISOL can be post-accelerated and injected to the IFF facility for producing more exotic RIBs.…”
Section: Introductionmentioning
confidence: 99%
“…Fortunately, several facilities are expected to be constructed in the near future, and one of them is currently underway at South Korea [6]. The development of the RISP SR facility is starting from only an exclusive muon beam line for SR.…”
Section: Introductionmentioning
confidence: 99%
“…The production target is located at the beginning of this stage (F0). While the stable beam will be provided by the superconducting linear accelerator, SCL1, the RI beam will be provided by the post-accelerator (SCL3) with the ISOL facility [5]. The secondary RI beam will be mainly produced by transfer reaction, but quasi-projectile fragmentation is also phase-space is 5th order and window sizes for (x,a) and (y,b) are 2 cm×200 mrad and 2 cm×400 mrad, respectively.…”
Section: Stage 1: In-flight Separatormentioning
confidence: 99%