We consider underdoped or overdoped cuprates as disordered conductors. The
diffusion coefficient D can be as low as 10(-1) m(2) s(-1). Under these con
ditions Coulomb interaction between electrons must be taken into account. T
he main effect is to open a dip in the density of state near the Fermi leve
l. We show that this model explains most of the observed features of the so
-called "pseudogap" in the normal state including its value, anisotropy and
variation with doping. Such a model applied to disordered metals explains
the dips observed in conductance measurements. (C) 2001 Elsevier Science B.
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