We calculate the dispersion relation of the single hole for the realis
tic bilayer t-J model within the self-consistent Born approximation ta
king into account both many-body effects and the local-density approxi
mation band structure. We show that the many-body effects strongly red
uce the band splitting. The large excitation energy arising at (pi,0),
compared with the pure t-J model, results from the specific band stru
cture where the function of in-plane hopping terms are dominant. Our r
esults are similar to the angle-resolved photoemission data of the sin
gle-layer antiferromagnetic insulator Sr2CuO2Cl2, and suggests that in
the presence of strong many-body effects the role of the interlayer c
ouplings in forming the quasiparticle bands is significantly suppresse
d.