The minimum coefficient of friction \( \mu \) required to prevent slipping is determined by the maximum acceleration \( a_{{max}} \) the body experiences during the oscillations. For simple harmonic motion (SHM), the maximum acceleration is given by:
\[
a_{{max}} = \omega^2 A
\]
where \( \omega \) is the angular frequency and \( A \) is the amplitude. The angular frequency \( \omega \) can be calculated from the period \( T \) as:
\[
\omega = \frac{2\pi}{T}
\]
Substituting \( T = 4 \, {s} \) and \( A = 0.3 \, {m} \), we find:
\[
\omega = \frac{2\pi}{4} = \frac{\pi}{2} \, {rad/s}
\]
\[
a_{{max}} = \left(\frac{\pi}{2}\right)^2 \times 0.3 = \frac{\pi^2}{4} \times 0.3
\]
The frictional force needed to prevent slipping is \( f = \mu mg \), equating this to the necessary centripetal force \( ma_{{max}} \), we have:
\[
\mu = \frac{a_{{max}}}{g}
\]
Given \( g = 9.81 \, {m/s}^2 \), substituting the values:
\[
\mu = \frac{\frac{\pi^2}{4} \times 0.3}{9.81}
\]
\[
\mu \approx 0.075
\]