In this paper, we study electromeganetic static spacetimes in the
nonrelativisitc general covariant theory of the Horava-Lifshitz (HL) gravity,
proposed recently by Horava and Melby-Thompson, and present all the electric
static solutions, which represent the generalization of the Reissner-Nordstrom
solution found in Einstein's general relativity (GR). The global/local
structures of spacetimes in the HL theory in general are different from those
given in GR, because the dispersion relations of test particles now contain
high-order momentum terms, so the speeds of these particles are unbounded in
the ultraviolet (UV). As a result, the conception of light-cones defined in GR
becomes invalid and test particles do not follow geodesics. To study black
holes in the HL theory, we adopt the geometrical optical approximations, and
define a horizon as a (two-closed) surface that is free of spacetime
singularities and on which massless test particles are infinitely redshifted.
With such a definition, we show that some of our solutions give rise to
(charged) black holes, although the radii of their horizons in general depend
on the energies of the test particles.Comment: 8 pages, To appear in JCA