Where k is Boltzmann's constant, f ( \ Gamma, 0 ) is the initial ( t = 0 ) distribution of molecular states \ Gamma, and \ Gamma ( t ) is the molecular state arrived at after time t, under the exact time reversible equations of motion . f ( \ Gamma ( t ), 0 ) is the INITIAL distribution of those time evolved states.
12.
Where k is Boltzmann's constant, f ( \ Gamma, 0 ) is the initial ( t = 0 ) distribution of molecular states \ Gamma, and \ Gamma ( t ) is the molecular state arrived at after time t, under the exact time reversible equations of motion . f ( \ Gamma ( t ), 0 ) is the INITIAL distribution of those time evolved states.
13.
The electrically neutral muonic tritium atom ( t-? ) 0 thus formed will act somewhat like an even " fatter, heavier neutron, " but it will most likely hang on to its muon, eventually forming a muonic molecular ion, most likely due to the resonant formation of a hyperfine molecular state within an entire deuterium molecule D 2 ( d = e 2 = d ), with the muonic molecular ion acting as a " fatter, heavier nucleus " of the " fatter, heavier " neutral " muonic / electronic " deuterium molecule ( [ d-?-t ] = e 2 = d ), as predicted by Vesman, an Estonian graduate student, in 1967.
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