Suppose that by a suitable external mechanical or electrical arrangement one can add to the energy
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P(ε) ∞ exp[ –(1 – α)ℓ/τ]
This reasoning gives the statistical basis of the Overhauser effect whereby the nuclear polarization in a magnetic field can be enhanced above the thermal equilibrium polarization. Such a condition requires the active supply of energy to the system front an external source. The system is not its equilibrium, but is said to be in a steady stare.
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