22CCarbon
Z:  
Z = 6N = 16
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
1547.41e-22012-05-0748Ca 345MeVBe 20mm9.4000120.0120.0 ---
1586.95e-22012-05-0548Ca 345MeVBe 20mm9.4000120.0120.0Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)
2445.30e-22008-12-1648Ca 345MeVBe 20mm9.4000120.0120.0Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)



Publication
Title Journal First Author
First Observation of 20B and 21BPhys. Rev. Lett. 121, 262502 (2018)S. Leblond
Interaction cross section study of the two-neutron halo nucleus 22CPhys. Lett. B 761, 412 (2016)Y. Togano
One- and two-neutron removal reactions from the most neutron-rich carbon isotopesPhys. Rev. C 86, 054604 (2012)N. Kobayashi

Experiment
Proposal No. Spokesperson Start-Date End-Date Beam Course
NP1412-RIBF132R. Kanungo2016-11-222016-11-2548Ca 345 MeV/u ZeroDegree
NP1512-SAMURAI36N. Orr2016-11-162016-11-1948Ca 345 MeV/u SAMURAI
NP1106-SAMURAI04N. Orr2012-05-142012-05-1748Ca 345 MeV/u SAMURAI
NP1106-SAMURAI03/04T. Nakamura2012-05-052012-05-1448Ca 345 MeV/u SAMURAI
NP0802-RIBF55T. Nakamura2008-12-152008-12-2148Ca 345 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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