Kinetics of muon catalyzed fusion processes in solid H/D mixture

Energy distribution of μd1s muonic atom and its spin states effecting on muonic X-Ray transfer yield in solid thin film method

“…The nonresonant formation rate of µdd is relatively low. [13][14][15][16] The µd 1s atoms slow down by elastic scattering collisions, until they are moderated at temperature of T = 3 K. The thermalized µd F =3/2 1s atoms take part in the resonant molecular formation, [17][18][19] …”

Forced chemical confinement fusion: μ-catalysed fusion by taking resonance escape probability of tμ(1s) atoms using an alternative kinetic model

“…where r 1 P (r) is the resonance escape probability. The resonance escape probability means the probability that degraded atoms of tµ(1s) are not absorbed before falling into the energy E r , where P (1) 1, P (2) 0.94 and P (2) . N ( ) ( ) (t) is the evolution of the density of muon/muonic atoms or molecules in the layers (averaged density over the whole layer), where their role appears in the muon cycling coefficient X c and also in the muon conversion efficiency.…”

“…Negative muons (1-10 MeV) can stop and form muonic atoms (µt, µd and µp) in different solid hydrogen targets cooled to 3 K [1,2]. Such atoms, created in the excited states, cascade to the ground state quickly (10 −12 s) [1], where their energy is much higher than the thermal equilibrium energies.…”

“…λ pt (E) is the isotope exchange rate versus energy [5]. These atoms subsequently lose their energy in elastic collisions (2), until the energy reaches the range of the RT minimum in the cross section σ el. s (E).…”

Quantum Mechanical Three-Body Systems and Its Application in Muon Catalyzed Fusion

“…This lifetime is amply long for most experiments. Muon catalyzed fusion (μCF) is a physical phenomenon in which the negative muon is able to cause fusion at room temperature and thereby eliminating the need for high temperature plasmas or powerful lasers (Owski, 2007;Imo et al, 2006;Filchenkov et al, 2005;Filipowicz et al, 2008;, 2009Marshal, 2001;Bystritsky et al, 2006, Nagamine et al, 1987Nagamine, 2001;Ponomarev, 2001). In comparison with (μCF), hot fusion schemes are made difficulty by the electrostatic (Coulomb) repulsion between positively charged nuclei.…”