20CCarbon
Z:  
Z = 6N = 14
N:  

Setting ID1 Yield 2
[pps/pnA]
Measurement
date
Beam Target Brho01
[Tm]
F1 slit
L [mm]
F1 slit
R [mm]
Data from
1511.63e+12012-05-1348Ca 345MeVBe 20mm8.206064.064.0 ---
1522.64e+12012-05-1348Ca 345MeVBe 17mm8.403064.064.0 ---
1533.21e+12012-05-1348Ca 345MeVBe 20mm8.951064.064.0Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)
1543.27e+02012-05-0748Ca 345MeVBe 20mm9.4000120.0120.0 ---
2414.10e+12008-12-2048Ca 345MeVBe 20mm8.5906120.0120.0Nucl. Instrum. Methods Phys. Res., Sect. B 317, 756 (2013)



Publication
Title Journal First Author
Single-neutron knockout from 20C and the structure of 19CPhys. Lett. B 769, 503 (2017)J. W. Hwang
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
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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