The work done in bringing a unit positive charge from infinity to a point P in an electric field is called:
By definition, 'V at a point P is the work done in bringing a unit positive charge from infinity to the point P.' (Section 2.8.1). Also confirmed earlier in Section 2.3, 'Potential at P due to the charge Q is $V(r) = \frac{Q}{4\pi\epsilon_0 r}$'.