116TcTechnetiumm
Z:  
Z = 43N = 73
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
1352.65e-12012-12-08238U 345MeVBe 3mm7.657021.164.2 ---
1367.30e-32012-12-06238U 345MeVBe 3mm7.970043.064.2 ---
1381.56e-22012-11-26238U 345MeVBe 3mm7.931022.064.2 ---
2501.27e+02008-11-21238U 345MeVBe 3mm7.990064.264.2J. Phys. Soc. Jpn. 79, 073201 (2010)
2522.63e+02007-05-28238U 345MeVBe 7mm7.250021.021.0J. Phys. Soc. Jpn. 77, 083201 (2008)
2549.15e-12007-05-23238U 345MeVBe 7mm7.396021.021.0J. Phys. Soc. Jpn. 77, 083201 (2008)



Publication
Title Journal First Author
β-delayed neutron emission of r-process nuclei at the N = 82 shell closurePhys. Lett. B 816, 136266 (2021)O. Hall
Shape evolution in 116,118Ru: Triaxiality and transition between the O(6) and U(5) dynamical symmetriesPhys. Rev. C 88, 024301 (2013)P.-A. Söderström
β-Decay Half-Lives of Very Neutron-Rich Kr to Tc Isotopes on the Boundary of the r-Process Path: An Indication of Fast r-Matter FlowPhys. Rev. Lett. 106, 052502 (2011)S. Nishimura


 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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