TY - JOUR
T1 - Muon-Catalyzed Fusion
AU - Rafelski, Johann
AU - Rafelski, Helga E.
N1 - Funding Information:
directly from a coherent program of research sponsored by the Advanced Energy Projects Program of the U.S. Dept. of Energy under the leadership of its former
Funding Information:
director, R. Gajewski, to whom this work is dedicated. This work was in part supported by the U.S. Dept. of Energy, BES/Advanced Energy Projects.
PY - 1991/1/1
Y1 - 1991/1/1
N2 - This chapter discusses muon-catalyzed fusion. The natural existence of a heavy electron, the muon bridges the enormous energy gap between the atomic and nuclear domains and facilitates spontaneous nuclear-fusion reactions of hydrogen isotopes. Because of this interconnection of atomic, molecular, and nuclear phenomena, the chain of atomic and molecular processes into which a single muon engages in a target consisting of a mixture of hydrogen isotopes, is very complex. The cycle of reactions in which a single muon repeatedly initiates nuclear fusions during its lifetime is termed as “muon-catalyzed fusion” or MuCF. At the origin of the diverse effects is the muonic hydrogen atom, a small neutral object capable of entering into chains of complex resonant reactions at thermal energies. The entire wealth of neutron-like physics repeats itself with the added complication that the neutral object is now polarizable. The chapter explains the nuclear fusion, dt muon catalytic cycle and reaction rates, and muon sticking. In MuCF exothermic fusion reactions can occur between several combinations of hydrogen isotopes. The dt catalytic cycle can be repeated hundred times during the lifetime of one muon. The probability of the initial sticking is the reaction-branching ratio, which is small but significant in MuCF applications.
AB - This chapter discusses muon-catalyzed fusion. The natural existence of a heavy electron, the muon bridges the enormous energy gap between the atomic and nuclear domains and facilitates spontaneous nuclear-fusion reactions of hydrogen isotopes. Because of this interconnection of atomic, molecular, and nuclear phenomena, the chain of atomic and molecular processes into which a single muon engages in a target consisting of a mixture of hydrogen isotopes, is very complex. The cycle of reactions in which a single muon repeatedly initiates nuclear fusions during its lifetime is termed as “muon-catalyzed fusion” or MuCF. At the origin of the diverse effects is the muonic hydrogen atom, a small neutral object capable of entering into chains of complex resonant reactions at thermal energies. The entire wealth of neutron-like physics repeats itself with the added complication that the neutral object is now polarizable. The chapter explains the nuclear fusion, dt muon catalytic cycle and reaction rates, and muon sticking. In MuCF exothermic fusion reactions can occur between several combinations of hydrogen isotopes. The dt catalytic cycle can be repeated hundred times during the lifetime of one muon. The probability of the initial sticking is the reaction-branching ratio, which is small but significant in MuCF applications.
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U2 - 10.1016/S1049-250X(08)60140-8
DO - 10.1016/S1049-250X(08)60140-8
M3 - Article
AN - SCOPUS:77956832794
SN - 1049-250X
VL - 29
SP - 177
EP - 215
JO - Advances in Atomic, Molecular and Optical Physics
JF - Advances in Atomic, Molecular and Optical Physics
IS - C
ER -