Carbon networks fabricated by means of a self-organized process, which is i
n the focus of our interest, represent disordered porous systems. The degre
e of disorder and, accordingly, the values of their electric conductivity e
xtending from insulator to metal behavior change via heat treatment under v
acuum conditions at process temperatures in the range from 600 to 1000 degr
eesC. Upon varying the ambient temperature from 4.2 to 295 K, four transpor
t mechanisms can be observed. For carbon nets whose conductivity is far bey
ond the metal-insulator transition (MIT), the specific resistivity rho depe
nds on the temperature T as rho (T)proportional toT(-b) exp([T-0/T ](1/p)).
In the low-temperature range, a Coulomb gap in the density of states locat
ed near the Fermi energy level occurs, which means that the characteristic
value of the exponent is p=2. At high temperatures, the pre-exponential par
t rho (T)proportional toT(-b) dominates. In the intermediate temperature ra
nge, we disclose Mott's hopping law with p=3. However, the specific resisti
vity of the carbon networks subject close to the MIT follows the power law
rho (T)proportional toT(-b) with 0 less than or similar tob less than or si
milar to3 at low temperatures. In the high-temperature range, the specific
resistivity is characterized by rho (T)proportional to exp(-[T/T-1](c-1)),
where the values for c vary from 1.3 to 1.5. The above four charge transpor
t mechanisms can be explained by the tails in the density of localized stat
es pulled out of the conduction and valence band, as a consequence of disor
der and, particularly, by some overlap between these tails. (C) 2001 Americ
an Institute of Physics.