Step 1: Write the given data.
Initial temperature:
\[
T_1=37^\circ\text{C}=310\ \text{K}.
\]
Ratio of specific heats:
\[
\gamma=1.5=\frac{3}{2}.
\]
The gas is compressed to half its original volume, therefore
\[
V_2=\frac{V_1}{2}.
\]
Hence,
\[
\frac{V_1}{V_2}=2.
\]
Step 2: Use the adiabatic relation.
For an adiabatic process,
\[
TV^{\gamma-1}=\text{constant}.
\]
Therefore,
\[
T_1V_1^{\gamma-1}
=
T_2V_2^{\gamma-1}.
\]
Hence,
\[
T_2
=
T_1
\left(\frac{V_1}{V_2}\right)^{\gamma-1}.
\]
Step 3: Substitute the given values.
Since
\[
\gamma-1
=
\frac{3}{2}-1
=
\frac{1}{2},
\]
we get
\[
T_2
=
310
\left(2\right)^{1/2}.
\]
\[
T_2
=
310\sqrt2.
\]
Using
\[
\sqrt2\approx1.414,
\]
\[
T_2
=
310\times1.414.
\]
\[
T_2
=
438.3\ \text{K}.
\]
Step 4: Convert into Celsius scale.
\[
T_2(^\circ\text{C})
=
438.3-273.
\]
\[
T_2
=
165.3^\circ\text{C}.
\]
Step 5: Final conclusion.
Therefore, the final temperature of the gas is
\[
\boxed{165.3^\circ\text{C}}
\]
Hence, the correct option is
\[
\boxed{(1)}
\]