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===Simpler Connection Between Radial and Phase Eigenfunctions=== When it is used as an argument of ATAN, the function, <math>~D(\varpi)</math>, [[#Constant_Phase_Loci|as defined above]] smoothly steers <math>~\phi_1</math> through a phase shift of approximately <math>~\pi</math> radians principally because the function itself smoothly varies between <math>~+1</math> and <math>~0</math> (then back again). Let's play with some simpler expressions for this governing function that also vary smoothly between these limits. Define, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~\Delta_\mathrm{inner}</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~\biggl( \frac{\varpi - r_-}{r_\mathrm{mid}-r_-} \biggr)</math> </td> <td align="center"> has range of </td> <td align="left"> <math>~+0 ~~\rightarrow ~~ +1 \, ;</math> </td> </tr> <tr> <td align="right"> <math>~\Delta_\mathrm{outer}</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~\biggl( \frac{\varpi - r_+}{r_\mathrm{mid}-r_+} \biggr)</math> </td> <td align="center"> has range of </td> <td align="left"> <math>~+1 ~~\rightarrow ~~ +0 \, .</math> </td> </tr> </table> </div> The argument of ATANH, [[#Radial_Eigenfunction|as presented above]], was obtained from this relatively simple expression via the shift, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~1-2\Delta_\mathrm{inner}</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~\biggl( \frac{\varpi - r_-}{r_\mathrm{mid}-r_-} \biggr)</math> </td> <td align="center"> has range of </td> <td align="left"> <math>~+1 ~~\rightarrow ~~ -1 \, ;</math> </td> </tr> <tr> <td align="right"> <math>~1-2\Delta_\mathrm{outer}</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~\biggl( \frac{\varpi - r_+}{r_\mathrm{mid}-r_+} \biggr)</math> </td> <td align="center"> has range of </td> <td align="left"> <math>~-1 ~~\rightarrow ~~ +1 \, .</math> </td> </tr> </table> </div> For the argument of <math>~D(\varpi)</math> function, we could therefore use, <div align="center"> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~1-\Delta_\mathrm{inner}</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~\biggl( \frac{\varpi - r_-}{r_\mathrm{mid}-r_-} \biggr)</math> </td> <td align="center"> has range of </td> <td align="left"> <math>~+1 ~~\rightarrow ~~ 0 \, ;</math> </td> </tr> <tr> <td align="right"> <math>~1-\Delta_\mathrm{outer}</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~\biggl( \frac{\varpi - r_+}{r_\mathrm{mid}-r_+} \biggr)</math> </td> <td align="center"> has range of </td> <td align="left"> <math>~0 ~~\rightarrow ~~ +1 \, .</math> </td> </tr> </table> </div>
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