The quasi-two-dimensional, metallic conduction in the CuO2 planes and
activated out-of-plane conduction seem typical for most of the cuprate
superconductors. The counteraction of overlap and charging energies D
elta U yield the activated out-of-plane resonant tunneling in the nor
mal state and the Josephson tunneling in the superconducting state whi
ch is quantitatively described by accepted parameters for various cupr
ate superconductors and oxygen contents. In addition, the localized, o
ut-of-plane charge exchange obstructed by Delta U of states of the bl
ocking layer may explain spectroscopic observations, like the tunnel o
r the photoelectron pseudo-gap, or may scatter phonons and in-plane qu
asi-particles. The latter relates Delta Usimilar or equal to kT* to t
he in-plane pseudo-gap temperature T, where the scattering rate decre
ases below T because of the obstructed out-of-plane exchange.