134SnTin
Z:  
Z = 50N = 84
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
836.58e+22015-04-08238U 345MeVW 0.5mm7.500064.264.2 ---
843.55e+22015-04-08238U 345MeVBe 4mm7.500064.264.2 ---
855.37e+22015-04-08238U 345MeVBe 3mm7.500064.264.2 ---
1373.10e-12012-12-03238U 345MeVBe 3mm8.004043.064.2 ---
1383.99e-32012-11-26238U 345MeVBe 3mm7.931022.064.2 ---
2492.10e+22008-11-23238U 345MeVPb+Al 1.0+0.3mm7.707064.264.2 ---
2527.70e+12007-05-28238U 345MeVBe 7mm7.250021.021.0J. Phys. Soc. Jpn. 77, 083201 (2008)
2548.30e+02007-05-23238U 345MeVBe 7mm7.396021.021.0 ---



Publication
Title Journal First Author
Gamma Decay of Unbound Neutron-Hole States in 133SnPhys. Rev. Lett. 118, 202502 (2017)V. Vaquero
First spectroscopic information from even-even nuclei in the region “southeast” of 132Sn: Neutron-excitation dominance of the 2+1 state in 132CdPhys. Rev. C 94, 051301R (2016)H. Wang
Observation of New Isotope 131Ag via the Two-Step Fragmentation TechniqueChin. Phys. Lett. 30, 042501 (2013)H. Wang

Experiment
Proposal No. Spokesperson Start-Date End-Date Beam Course
NP1712-RIBF162A. Jungclaus2018-10-292018-11-01238U 345 MeV/u ZeroDegree


 Annotations:
1 Detailed BigRIPS setting is shown in the linked page.
2 The list of primary beam intensities is given in this page.
3 Error is only statistical one. Systematic error is estimated within 30%, which comes from uncertainly of primary beam intensity.


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