Emission of helium ions after antiproton annihilation in nuclei
References (23)
- et al.
Nucl. Phys.
(1982) Phys. Lett.
(1980)Phys. Lett.
(1982)- et al.
Phys. Lett.
(1982) - et al.
Phys. Lett.
(1984) - et al.
Phys. Lett.
(1984) - et al.
Phys. Lett.
(1986) - et al.
Phys. Lett.
(1986) - et al.
Phys. Lett.
(1986) At. Data Nucl. Data Tables
(1982)
Nucl. Instr. Meth.
(1975)
Cited by (40)
Antiprotonic bound systems
2022, Progress in Particle and Nuclear PhysicsAntiproton radiotherapy
2008, Radiotherapy and OncologyCitation Excerpt :The π0 meson is highly unstable and decays instantaneously into high energy gamma-rays with roughly 70–300 MeV [12]. Due to the solid angle covered by the nucleus, 1 or 2 of the charged pions are most likely penetrating the nucleus inducing an intra-nuclear cascade, causing the nucleus to break into fragments [14–16]. Charged fragments have a very short range in the target and will deposit their kinetic energy in the immediate vicinity of the annihilation vertex.
Bubble detector measurements of a mixed radiation field from antiproton annihilation
2006, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsStatistical multifragmentation of nuclei
1995, Physics ReportsAbsolute probabilities of fission induced by stopped antiprotons
1994, Nuclear Physics, Section AProduction of light particles after antiproton-nucleus annihilation and their interpretation with statistical models
1993, Nuclear Physics, Section A
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