14BeBeryllium
Z:  
Z = 4N = 10
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
1034.05e+12014-11-2848Ca 345MeVBe 30mm9.0659120.0120.0 ---
1623.20e+22012-04-1618O 230MeVBe 20mm6.9390120.0120.0 ---



Publication
Title Journal First Author
Evolution of the two-neutron configuration from 11Li to 13LiPhys. Lett. B 857, 138977 (2024)P. André
Searching for universality of dineutron correlation at the surface of Borromean nucleiPhys. Lett. B 840, 137875 (2023)A. Corsi
Structure of 13Be probed via quasi-free scatteringPhys. Lett. B 797, 134843 (2019)A. Corsi
SAMURAI spectrometer for RI beam experimentsNucl. Instrum Methods Phys. Res., Sect. B 317, 294 (2013)T. Kobayashi

Experiment
Proposal No. Spokesperson Start-Date End-Date Beam Course
MS-EXP24-01H. Suzuki2024-04-192024-04-2018O 250 MeV/u BigRIPS
NP1412-SAMURAI30L. Stuhl2018-05-282018-06-0218O 230 MeV/u SAMURAI
NP1612-SAMURAI12R1D. Beaumel2018-05-152018-05-2318O 230 MeV/u SAMURAI
NP1312-SAMURAI18R1A. Corsi, Y. Kubota2014-11-272014-12-0848Ca 345 MeV/u SAMURAI
MS11-17S. Nishimura, P. Doornenbal2012-04-162012-04-1818O 230 MeV/u ZeroDegree
MS11-10K. Yoneda2012-03-162012-03-2318O 294 MeV/u SAMURAI
MS11-07T. Kubo2011-05-312011-06-0218O 250 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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