Use partial fraction decompostion. This requires factoring the quadratic first.
$$
I(s)=\frac{6}{L}\frac{1}{s^2 + \frac{R}{L}s + \frac{1}{LC}}
$$
The roots of that quadratic are
$$
s_{1,2} = -\frac{R}{2L}\pm\sqrt{\left(\frac{R}{2L}\right)^2-\frac{1}{LC}}
$$
If $s_{1,2}$ are distinct, your function can be represented as
$$
I(s)=\frac{6}{L}\frac{1}{(s-s_1)(s-s_2)} = \frac{A}{s-s_1} + \frac{B}{s-s_2}
$$
$A$ can be found by multiplying the equation through by $s-s_1$ and then taking $\lim_{s\rightarrow s_1}$; $B$ can be found in the analogous way with $s_2$. The form of each term is in the Laplace transform tables; each term will correspond to an exponential.
If $s_{1,2}$ happen to be identical (i.e. the discriminant is exactly zero), you'll use the representation
$$
I(s)=\frac{6}{L}\frac{1}{(s-s_1)^2} = \frac{A}{s-s_1} + \frac{B}{(s-s_1)^2}
$$
and again, find constants $A$ and $B$ that satisfy the above. Each of that kind of term will also be found in the transform tables.
The top case is more likely, where the roots are distinct. In that case you'll either get two real roots or a complex conjugate pair. If there are two real roots, you'll get two decaying exponentials after the inverse Laplace transform. If you have a complex conjugate pair, you'll get an exponentially decaying sinusoid, where the decay will look like $e^{-\frac{R}{2L}}$ and the sinusoidal part will have real frequency $\sqrt{\frac{1}{LC}-\left(\frac{R}{2L}\right)^2}$
In the second case, you should get something like $(C_1t+C_2)e^{-\frac{R}{2L} t}$ for some constants $C_1,C_2$.