The electric field at dipole is
\(E_0 = \frac {KP}{L^3}\)
The potential energy of a dipole placed in an electric field is
\(U = -\vec P .\vec E\)
\(U = -PE\, cos90° - PE \,cos 30° - \frac{KP^2}{L^3} cos60° \)
\(U = - 0 - PE\times \frac{\sqrt 3}2 - \frac{KP^2}{L^3} \times \frac12\)
\(U = -\left[\frac{KP^2}{2L^3 } + \frac{\sqrt3}2PE\right]\)