We present a novel approach to the analysis of the normal state in-plane
\(\sigma _{ab} \)
and out-of-plane σc
conductivities of anisotropic layered crystals such as oxygen deficient YBa
2
Cu
3
O
x
. It can be shown that the resistive anisotropy is determined by the ratio of the phase coherence lengths in the respective directions; i.e.,
\(\sigma _{ab} /\sigma _c = \ell _{ab}^2 /\ell _c^2 \). From the idea that at all doping levels and temperatures T the out-of-plane transport in these crystals is incoherent, follows that
\(\ell _c \)
is T-independent, equal to the spacing
\(\ell _0 \)
between the neighboring bilayers. Thus, the T-dependence of
\(\ell _{ab} \)
is given by the measured anisotropy, and
\(\sigma _{ab} (\ell _{ab} )\)
dependence is obtained by plotting
\(\sigma _{ab} {\text{ }}vs{\text{ }}\ell = {\text{ (}}\sigma _{ab} /\sigma _c )^{1/2} \ell _0 \).The analysis of several single crystals of YBa
2
Cu
3
O
x
(6.35 < x < 6.93) shows that for all of them
\(\sigma _{ab} (\ell ) \)
is described by a universal dependence
\(\sigma _{ab} /\overline \sigma = f(\ell /\overline \ell ) \)
with doping dependent parameters
\(\overline \sigma {\text{ }}and{\text{ }}\overline \ell \).