| http://www.w3.org/ns/prov#value | - He proposed that in a system defined by some macroscopic parameter, such as temperature, ??, its energies can be separated into two categories: stored (coherent) energies that remain in a non-equilibrium state within a characteristic time, ??, and thermal (random) energies that exchange with each other and reach equilibrium (or equilibrate) in a time less than ?? (Figure 3).
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