The photoluminescence spectrum of quantized Hall states near filling f
actor v=1 is investigated theoretically. For v greater than or equal t
o 1 the spectrum consists of a right-circularly polarized (RCP) line a
nd a left-circularly polarized (LCP) line, whose mean energy (i) does
not depend on the electron g factor for spin-1/2 quasielectrons; (ii)
does depend on g for charged spin-texture excitations (Skyrmions). For
v<1 the spectrum consists of a LCP Line shifted down in energy from t
he LCP line at v greater than or equal to 1. The g-factor dependence o
f the redshift of the LCP Line determines the nature of the negatively
charged excitations.