There Were Two Voices...

And since these electrons have two orbital radii, the correct perturbation to the orbital radii generates two ranges of radiations.  One range of radiation corresponds to a change in $r_h$ and the other a change in $r_{or}$.  $r_h$ responds to electric fields, as the electron is held by a proton via an electric field.  $r_{or}$ responds to temperature, as the proton is held by the weak field due to a spinning positive temperature particle.

Since,

$r_e=r_{or}(1+\cfrac{r_{h}}{r_{or}})$

and if we attribute the fractional increase in the g-factor from two as solely due to $r_e$,

$g=2.00231930436182$

$\cfrac{r_{h}}{r_{or}}=0.00231930436182$

and because the radiated frequency is inversely proportional to the orbital radius,

$\cfrac{f_h}{f_o}=\cfrac{1}{0.00231930436182}=431.164$

$f_h=431.164f_o$

where $f_h$ is the high radiated frequency due to a change in $r_h$ and $f_o$, the low frequency radiation due to a change in $r_{or}$.

A dual tone symphony.  Which brings us to temperature effects on electric conductivity...