Dispersed vacuum ultraviolet (VUV) fluorescence spectra of neutral fragments formed in the extreme ultraviolet photodissociation of O2 and their excitation spectra at the incident synchrotron radiation (SR) wavelength of 57-85 nm have been obtained using a secondary VUV monochromator to clarify the dissociation mechanism of O2 in superexcited states. The VUV fluorescence from dissociation fragments has been observed at the lowest dissociation limits of O(n(l)) + O(3P). The dissociation of the Rydberg states converging on the O2+(b4-SIGMA(g)-) and O2+(B2-SIGMA(g)-) states has been shown to prefer dissociation limits higher than the lowest limit of O(3s3S)+O(3P) via multichannel crossing. An intensity enhancement in the O(3s3S-->3P) fluorescence excitation spectrum (FES) around the incident wavelength of 58 nm has been explained by the direct dissociation of the free (c4-SIGMA(u)-)3s-sigma(g) state.