100SrStrontium
Z:  
Z = 38N = 62
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
572.77e+12015-11-11238U 345MeVBe 0.1mm7.160064.264.2 ---
1071.49e-32014-11-06238U 345MeVBe 4mm8.087064.264.2 ---
1081.85e-32014-11-03238U 345MeVBe 4mm8.087064.264.2 ---
2504.54e+12008-11-21238U 345MeVBe 3mm7.990064.264.2 ---
2529.63e+22007-05-28238U 345MeVBe 7mm7.250021.021.0J. Phys. Soc. Jpn. 77, 083201 (2008)
2533.01e+12007-05-26238U 345MeVBe 7mm7.634042.042.0J. Phys. Soc. Jpn. 77, 083201 (2008)
2545.74e+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
Prominence of Pairing in Inclusive (p,2p) and (p,pn) Cross Sections from Neutron-Rich NucleiPhys. Rev. Lett. 122, 162503 (2019)N. Paul


 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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