1. Measurements of production cross sections of 10Be and 26Al by 120 GeV and 392 MeV proton bombardment of 89Y, 159Tb, and natCu targets
- Author
-
A. Soha, Atsushi Shinohara, S. Shibata, Hiroshi Yashima, Yoshimi Kasugai, S. Okumura, Kazuhiko Ninomiya, T. Omoto, Yuki Matsushi, Tatsushi Shima, Akihiro Toyoda, R. Coleman, E. J. Ramberg, Shun Sekimoto, Hiroyuki Matsuzaki, Kamran Vaziri, G. Lauten, N.V. Mokhov, David Boehnlein, Hiroshi Nakashima, Tsutomu Ohtsuki, Hiroshi Matsumura, Naruto Takahashi, Koji Oishi, Marc W. Caffee, Y. Sakamoto, Kees C. Welten, Kunihiko Nishiizumi, Norihiro Matsuda, and Anthony Leveling
- Subjects
Mass number ,Nuclear and High Energy Physics ,Range (particle radiation) ,Proton ,Chemistry ,Binding energy ,chemistry.chemical_element ,Zinc ,Al-26 ,120 GeV proton ,Nuclear physics ,Nickel ,Atomic physics ,Impact parameter ,Nuclear Experiment ,Fragmentation process ,Instrumentation ,Be-10 ,Accelerator mass spectrometry - Abstract
The production cross sections of 10Be and 26Al were measured by accelerator mass spectrometry using 89Y, 159Tb, and natCu targets bombarded by protons with energies Ep of 120 GeV and 392 MeV. The production cross sections obtained for 10Be and 26Al were compared with those previously reported using Ep = 50 MeV–24 GeV and various targets. It was found that the production cross sections of 10Be monotonically increased with increasing target mass number when the proton energy was greater than a few GeV. On the other hand, it was also found that the production cross sections of 10Be decreased as the target mass number increased from that of carbon to those near the mass numbers of nickel and zinc when the proton energy was below approximately 1 GeV. They also increased as the target mass number increased from near those of nickel and zinc to that of bismuth, in the same proton energy range. Similar results were observed in the production cross sections of 26Al, though the absolute values were quite different between 10Be and 26Al. The difference between these production cross sections may depend on the impact parameter (nuclear radius) and/or the target nucleus stiffness.
- Published
- 2015
- Full Text
- View/download PDF