Right choice is (c) \(\frac{\lambda^2}{4\pi \eta}\)
To explain: For isotropic radiator, directivity is 1. So the effective aperture is given by \(A_{em}=D \frac{\lambda^2}{4\pi} = \frac{\lambda^2}{4\pi}\)
Then physical aperture =\(\frac{Effective\, aperture}{Aperture\, efficiency}=\frac{\lambda^2}{4\pi \eta}\)