You can proceed in two different ways:
1. Using KVL:
VL+VR+Vo=Vi
we know that the current is the same for all the components (single mesh): VR=R*i, VL=L*di/dt and i=C*dVo/dt. Deriving this last di/dt=C*d²Vo/dt². Let's now substitute in the KVL
L*C*d²Vo/dt²+R*C*dVo/dt+Vo=Vi
Laplacing: (S²*L*C+S*R*C+1)*Vo=Vi
2. Using directly the laplace transform of each single component. We have a voltage divider in which the impedance to ground is Zc=1/(S*C) while the series is ZL+R=SL+R then simply:
Vo/Vi=[1/(S*C)]/[1/(S*C)+S*L+R]=1/[1+S²*L*C+S*R*C]