  The Jordan-Wigner transformation is traditionally applied to one dimensional
systems, but recent works have generalized the transformation to fermionic
lattice systems in higher dimensions while keeping locality manifest. These
developments could aid the theoretical or even experimental studies of strongly
correlated electronic problems through their bosonic counterparts. In this
work, we develop a scheme for higher-dimensional Jordan-Wigner transformation
which keeps all relevant symmetries manifest on the bosonic side. Our approach
connects the discussion of exact lattice bosonization to the familiar notions
of fractionalized partons like spinons and chargeons, and works for spin-$1/2$
fermions -- like the physical electrons -- on four-coordinated lattices. The
construction is applied to fermions defined on the square, kagome and diamond
lattices, and we provide explicit expressions for the bosonized versions of
well-known models of strongly correlated electrons, like the Hubbard and
$t$-$J$ models.
