Step 1: Use the torque formula for a magnetic dipole.
The torque on a magnetic needle is
\[
\tau = MB\sin\theta,
\]
where
\[
M=\text{magnetic dipole moment},
\]
\[
B=\text{magnetic field},
\]
and
\[
\theta=\text{angle between } \vec{M} \text{ and } \vec{B}.
\]
Step 2: Determine the angle in the first case.
The magnetic field is along
\[
\hat{i}.
\]
The needle is directed along
\[
(\sqrt3\hat{i}+\hat{j}).
\]
Therefore,
\[
\tan\theta_1=\frac{1}{\sqrt3}.
\]
Hence,
\[
\theta_1=30^\circ.
\]
Given torque,
\[
\tau_1=0.06\ \text{N m}.
\]
Thus,
\[
0.06=MB\sin30^\circ.
\]
\[
0.06=MB\left(\frac12\right).
\]
\[
MB=0.12.
\]
Step 3: Determine the angle in the second case.
The magnetic field is along
\[
\hat{j}.
\]
The needle is directed along
\[
(\hat{i}+\sqrt3\hat{j}).
\]
Now,
\[
\tan\theta_2=\frac{1}{\sqrt3}.
\]
Hence,
\[
\theta_2=30^\circ.
\]
The magnetic field magnitude is
\[
2B.
\]
Therefore,
\[
\tau_2=M(2B)\sin30^\circ.
\]
\[
\tau_2=2MB\left(\frac12\right).
\]
\[
\tau_2=MB.
\]
Using
\[
MB=0.12,
\]
we obtain
\[
\tau_2=0.12\ \text{N m}.
\]
Step 4: Final conclusion.
Hence, the torque experienced by the magnetic needle is
\[
\boxed{0.12\ \text{N m}}
\]
Therefore, the correct option is
\[
\boxed{(1)}
\]