The electric field due to an infinite sheet of charge is given by:
\[
E = \frac{\sigma}{2\varepsilon_0} \text{ on each side.}
\]
However, since the sheet radiates field symmetrically on both sides, the net field on either side is:
\[
E = \frac{\sigma}{\varepsilon_0}
\]
if we consider both contributions from either side of the sheet at a point. Hence, the correct expression is: \(\dfrac{\sigma}{\varepsilon_0}\).