104SnTin
Z:  
Z = 50N = 54
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
1782.30e+22011-12-15124Xe 345MeVBe 4mm5.417042.842.8Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)
1792.80e+22011-12-15124Xe 345MeVBe 3mm5.468042.842.8Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)
1802.30e+22011-12-15124Xe 345MeVBe 4mm5.523042.842.8Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)



Publication
Title Journal First Author
Spectroscopy of nuclei around 100Sn populated via two-neutron knockout reactionsPhys. Rev. C 97, 044321 (2018)A. Corsi
Neutron-driven collectivity in light tin isotopes: Proton inelastic scattering from 104SnPhys. Lett. B 743, 451 (2015)A. Corsi
Intermediate-energy Coulomb excitation of 104Sn: Moderate E2 strength decrease approaching 100SnPhys. Rev. C 90, 061302R (2014)P. Doornenbal
Evaporation-cost dependence in heavy-ion fragmentationPhys. Rev. C 88, 041602R (2013)L. Audirac

Experiment
Proposal No. Spokesperson Start-Date End-Date Beam Course
NP1106-RIBF74A. Obaterlli2012-06-302012-07-05124Xe 345 MeV/u ZeroDegree
NP0811-RIBF70R1P. Doornenbal2012-06-302012-07-05124Xe 345 MeV/u ZeroDegree
MS11-03T. Kubo2011-12-122011-12-18124Xe 345 MeV/u BigRIPS


 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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