Fragment energy correlation measurements for the proton induced fission of 226Ra
References (22)
Nucl. Phys.
(1963)- et al.
Phys. Rev.
(1968) - et al.
Phys. Rev.
(1965) - et al.
Phys. Rev.
(1965) Ark. Fys.
(1966)- et al.
Nucl. Phys.
(1965) - et al.
ORNL-report 4230
(1968) - et al.
Phys. Rev.
(1968) - et al.
Phys. Rev.
(1966)
Phys. Rev.
(1965)
et al.Cited by (11)
Interplay of fission modes in mass distribution of light actinide nuclei <sup>225,227</sup>Pa
2016, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsExcitation energy dependence of fragment-mass distributions from fission of <sup>180,190</sup>Hg formed in fusion reactions of <sup>36</sup>Ar + <sup>144,154</sup>Sm
2015, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsFusion and fission of heavy and superheavy nuclei (experiment)
2015, Nuclear Physics ACitation Excerpt :With this method, the mass of the secondary fragments (namely, after evaporation of particles) is extracted. In many works the energies of the fission fragments are measured with semiconductor detectors (see, e.g., [55–59]) or with ionization chambers. Semiconductor detectors have low radiation hardness and require corrections for the pulse height defect.
The <sup>226</sup>Th fission valleys
2008, Nuclear Physics AFragment mass and kinetic energy distribution in isomeric fission of <sup>240</sup>Pu
1974, Nuclear Physics, Section AOdd-multipole shape distortions and the fission barriers of elements in the region 84 ≦ z ≦ 120
1972, Nuclear Physics, Section A
Copyright © 1969 Published by Elsevier B.V.