The Bi2Sr2(Ca1-xYx)Cu2O8+delta system over the homogeneity range x = 0 simi
lar to 1.0 has a maximal superconducting transition temperature (T-c) of ar
ound 92 K at x = 0.2. The hole distribution of overdoped, optimum doped and
underdoped states in Bi2Sr2(Ca1-xYx)Cu2O8+delta has been investigated by h
igh-resolution O Kedge X-ray-absorption near-edge-structure (XANES) spectra
. Near the O 1s edge, a well-pronounced pre-edge peak with maximum at simil
ar to 528.3 eV is found, which is ascribed to the excitations of O 1s elect
ron to O 2p hole states located in the CuO2 planes. The intensity of this p
re-edge peak decreases as the Y doping increases, demonstrating that the ch
emical substitution of Y3+ for Ca2+ in Bi2Sr2(Ca(1-)xY(x))C2O8+delta gives
rise to a decrease in hole concentrations within the CuO2 planes. Moreover,
the correlation between T-c and critical current density (J(c)) as a funct
ion of doping concentration has been studied. It is important to point out
that the highest J(c) across the system is appeared at the overdoped side w
ith x = 0 in Bi2Sr2(Ca(1-x)Yx)Cu2O8+delta.