Step 1: Use the relation between heat supplied and volume change.
At constant pressure,
\[
Q=nC_P\Delta T.
\]
Also,
\[
P\Delta V=nR\Delta T.
\]
Eliminating \(\Delta T\),
\[
\Delta V=\frac{QR}{PC_P}.
\]
Thus,
\[
\boxed{\Delta V\propto\frac{1}{C_P}}
\]
for the same heat supplied and the same pressure.
Step 2: Write the specific heats.
For a diatomic gas,
\[
C_P=\frac{7R}{2}.
\]
For a monoatomic gas,
\[
C_P=\frac{5R}{2}.
\]
Step 3: Find the ratio of volume changes.
Therefore,
\[
\frac{\Delta V_{\text{mono}}}{\Delta V_{\text{dia}}}
=
\frac{\dfrac{1}{5R/2}}{\dfrac{1}{7R/2}}
=
\frac75
=
1.4.
\]
Hence,
\[
\Delta V_{\text{mono}}
=
1.4\,\Delta V.
\]
Thus,
\[
\boxed{\Delta V_{\text{mono}}=1.4\,\Delta V.}
\]
Therefore, the correct option is \(\boxed{(A)}\).