Abstract
Experimental evidence is presented for the effect of photoionization of $n{s}^{2}$ atomic subshells with unpolarized radiation that leads to highly polarized photoelectrons in angular-resolved measurements. Like the Fano effect, the observed phenomenon is caused by spin-orbit interaction in the continuous spectrum. The spin polarization essentially depends on the phase-shift difference between the $\ensuremath{\epsilon}{p}_{\frac{1}{2}}$ and $\ensuremath{\epsilon}{p}_{\frac{3}{2}}$ continua.
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