Abstract

This paper deals with the optimization of the processes involved in muon catalyzed fusion. Muon catalyzed fusion ( μ CF ) is studied in all layers of the solid hydrogen structure H / 0.1 % T ⊕ D 2 ⊕ HD . The layer H/ T acts as an emitter source of energetic t μ atoms, due to the so-called Ramsauer–Townsend effect. These t μ atoms are slowed down in the second layer (degrader) and are forced to take place nuclear fusion in HD. The degrader affects time evolution of t μ atomic beam. This effect has not been considered until now in μ CF -multilayered targets. Due to muon cycling and this effect, considerable reactions occur in the degrader. In our calculations, it is shown that the fusion yield equals 180 ± 1.5 . It is possible to separate events that overlap in time.

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 call

Disclaimer: 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.