| 136Sn | Tin | | Z: | ≪ | ≫ | |
| Z = 50 | N = 86 | | N: | ≪ | ≫ | |
| Setting ID1 | Yield 2 [pps/pnA] | Measurement date | Beam | Target | Brho01 [Tm] | F1 slit L [mm] | F1 slit R [mm] | Data from |
|---|---|---|---|---|---|---|---|---|
| 137 | 2.83e-1 | 2012-12-03 | 238U 345MeV | Be 3mm | 8.0040 | 43.0 | 64.2 | --- |
| 138 | 7.04e-5 | 2012-11-26 | 238U 345MeV | Be 3mm | 7.9310 | 22.0 | 64.2 | --- |
| 249 | 3.15e+0 | 2008-11-23 | 238U 345MeV | Pb+Al 1.0+0.3mm | 7.7070 | 64.2 | 64.2 | --- |
| 254 | 4.72e-1 | 2007-05-23 | 238U 345MeV | Be 7mm | 7.3960 | 21.0 | 21.0 | J. Phys. Soc. Jpn. 77, 083201 (2008) |
| Title | Journal | First Author | Position of the single-particle 3/2− state in 135Sn and the 𝑁=90 subshell closure | Phys. Lett. B 851, 138561 (2024) | A. Jungclaus | Evolution of proton single-particle states in neutron-rich Sb isotopes beyond N = 82 | Phys. Rev. C 102, 034324 (2020) | A. Jungclaus | Yrast 6+ Seniority Isomers of 136,138Sn | Phys. Rev. Lett. 113, 132502 (2014) | G. S. Simpson | Collectivity evolution in the neutron-rich Pd isotopes toward the N = 82 shell closure | Phys. Rev. C 88, 054318 (2013) | H. Wang |
|---|
| Proposal No. | Spokesperson | Start-Date | End-Date | Beam | Course | NP1612-RIBF149 | A. Jungclaus | 2018-11-01 | 2018-11-04 | 238U 345 MeV/u | ZeroDegree | MS-EXP15-01 | N. Inabe | 2015-10-20 | 2015-10-21 | 238U 345 MeV/u | BigRIPS | MS-EXP12-04 | T. Kubo | 2012-12-11 | 2012-12-12 | 238U 345 MeV/u | BigRIPS | NP1112-RIBF85 | G. Simpson | 2012-11-30 | 2012-12-05 | 238U 345 MeV/u | ZeroDegree |
|---|