Step 1: Determine the arrangement of dielectric slabs.
The two dielectric slabs have area equal to the plate area and each occupies half of the plate separation.
Hence, the slabs are placed one after another along the electric field direction. Therefore, they behave as two capacitors connected in series.
Let the plate separation be
\[
d
\]
Then each slab has thickness
\[
\frac{d}{2}
\]
and plate area
\[
A
\]
Step 2: Find the capacitance of the first dielectric slab.
For dielectric constant \(K_1\),
\[
C_1=\frac{K_1\varepsilon_0A}{d/2}
\]
\[
C_1=\frac{2K_1\varepsilon_0A}{d}
\]
Since
\[
C_0=\frac{\varepsilon_0A}{d}
\]
therefore,
\[
C_1=2K_1C_0
\]
Step 3: Find the capacitance of the second dielectric slab.
Similarly, for dielectric constant \(K_2\),
\[
C_2=\frac{K_2\varepsilon_0A}{d/2}
\]
\[
C_2=\frac{2K_2\varepsilon_0A}{d}
\]
\[
C_2=2K_2C_0
\]
Step 4: Use the series combination formula.
Since the two dielectric regions act as capacitors in series,
\[
\frac{1}{C}
=
\frac{1}{C_1}
+
\frac{1}{C_2}
\]
Substituting \(C_1\) and \(C_2\),
\[
\frac{1}{C}
=
\frac{1}{2K_1C_0}
+
\frac{1}{2K_2C_0}
\]
\[
\frac{1}{C}
=
\frac{1}{2C_0}
\left(
\frac{1}{K_1}
+
\frac{1}{K_2}
\right)
\]
\[
\frac{1}{C}
=
\frac{K_1+K_2}
{2C_0K_1K_2}
\]
Therefore,
\[
C=
\frac{2C_0K_1K_2}
{K_1+K_2}
\]
Step 5: Final conclusion.
Hence, the new capacitance is
\[
\boxed{
2C_0\left(\frac{K_1K_2}{K_1+K_2}\right)
}
\]