Abstract
When a projectile with several hundred MeV of kinetic energy per nucleon interacts with a target nucleus, a very large number of final states are available in the interaction. A significant fraction of the reaction products will be ejectiles of more than a few nucleons. Certainly, nucleon emission dominates, but the yields of higher mass fragments are also substantial. Further, a large portion of the integrated cross section comes from emission of particles with more than a few MeV of kinetic energy per nucleon; that is, with energies beyond those associated with emission from a large system of nucleons in thermal and chemical equilibrium.
Published Version
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
