Separating variables gives
Therefore
For , define the strong-coupling scale
Then
It decreases logarithmically toward zero in the ultraviolet and grows toward the infrared, becoming nonperturbative when approaches .
For , the theory is asymptotically free: it is weakly coupled at high energies and strongly coupled in the infrared. For , the coupling decreases toward the infrared but grows toward a finite ultraviolet Landau pole; such a theory is infrared free and requires an ultraviolet completion before that pole.
Let
Running each coupling down from the common value gives
Subtracting the equations determines , and eliminating it from the difference gives
which is the claimed gauge coupling unification relation.

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