Step 1: Recall the magnetic force on a charged particle.
When a charged particle moves through a magnetic field, it experiences a force
\[
F=qvB\sin\theta
\]
where \(q\) is the charge of the particle.
The resulting circular motion has radius
\[
r=\frac{mv}{qB}.
\]
A smaller radius corresponds to a greater deflection.
Step 2: Compare \(\alpha\)-particles and \(\beta\)-particles.
An \(\alpha\)-particle has
\[
q=+2e
\]
but its mass is approximately
\[
4\,\text{u},
\]
which is very large.
A \(\beta\)-particle is an electron having
\[
q=-e
\]
and an extremely small mass
\[
m_e.
\]
Since
\[
r=\frac{mv}{qB},
\]
the much smaller mass of the \(\beta\)-particle makes its radius of curvature much smaller than that of the \(\alpha\)-particle. Hence it undergoes a much larger deflection.
Step 3: Consider \(\gamma\)-rays and neutrons.
\(\gamma\)-rays are electromagnetic waves and carry no charge.
Neutrons are electrically neutral particles.
Therefore,
\[
q=0
\]
for both, so they are not deflected by a magnetic field.
Step 4: Final conclusion.
Among the given options, the maximum deflection is shown by the stream of \(\beta\)-particles.
\[
\boxed{\text{Stream of }\beta\text{-particles}}
\]
Hence, the correct option is
\[
\boxed{(2)}.
\]