Concept:
According to Gauss's Law, the electric field due to an infinite plane sheet carrying a uniform surface charge density \(\sigma\) is
\[
\boxed{E=\frac{\sigma}{2\varepsilon_{0}}}
\]
This electric field is independent of the distance from the sheet.
For two parallel sheets carrying equal and opposite surface charge densities,
\[
+\sigma \qquad \text{and} \qquad -\sigma,
\]
the electric fields combine according to the principle of superposition.
• Between the sheets, both electric fields act in the same direction and hence add.
• Outside the sheets, the electric fields are equal in magnitude but opposite in direction and therefore cancel each other.
Step 1: Electric field due to a positively charged sheet.
For the positively charged sheet,
\[
E_{+}=\frac{\sigma}{2\varepsilon_{0}}.
\]
The field is directed away from the positive sheet.
Step 2: Electric field due to a negatively charged sheet.
For the negatively charged sheet,
\[
E_{-}=\frac{\sigma}{2\varepsilon_{0}}.
\]
The field is directed towards the negative sheet.
Step 3: Find the resultant electric field between the sheets.
Between the sheets, both electric fields are in the same direction.
Hence,
\[
E=E_{+}+E_{-}.
\]
Substituting,
\[
E
=
\frac{\sigma}{2\varepsilon_{0}}
+
\frac{\sigma}{2\varepsilon_{0}}.
\]
Therefore,
\[
E
=
\frac{\sigma}{\varepsilon_{0}}.
\]
Thus,
\[
\boxed{E=\frac{\sigma}{\varepsilon_{0}}.}
\]
Hence, the correct answer is
\[
\boxed{\textbf{Option (B)}}.
\]