89SeSelenium
Z:  
Z = 34N = 55
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
611.43e+32015-10-22238U 345MeVBe 2mm6.741442.842.8 ---
621.64e+32015-10-22238U 345MeVBe 2mm6.816542.842.8 ---
1074.99e-12014-11-06238U 345MeVBe 4mm8.087064.264.2 ---
1084.35e-12014-11-03238U 345MeVBe 4mm8.087064.264.2 ---
2511.20e+22008-11-08238U 345MeVBe 5mm7.901064.264.2J. Phys. Soc. Jpn. 79, 073201 (2010)
2521.06e+32007-05-28238U 345MeVBe 7mm7.250021.021.0J. Phys. Soc. Jpn. 77, 083201 (2008)
2534.14e+12007-05-26238U 345MeVBe 7mm7.634042.042.0 ---
2547.32e+22007-05-23238U 345MeVBe 7mm7.396021.021.0J. Phys. Soc. Jpn. 77, 083201 (2008)



Publication
Title Journal First Author
Sequential Nature of (p,3p) Two-Proton Knockout from Neutron-Rich NucleiPhys. Rev. Lett. 125, 012501 (2020)A. Frotscher
Low-lying structure and shape evolution in neutron-rich Se isotopesPhys. Rev. C 95, 041302R (2017)S. Chen


 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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