Answer:
Option B
Explanation:
Field due to one side of loop at O= $\frac{\mu_{0}I}{4\pi (\frac{a}{2})}(2\sin 45^{0})$
Field at O due to all four sides is along untill vector $\hat{e}_{x}$
$\therefore$ Total field
$=4.\frac{\mu_{0}I}{4\pi(\frac{a}{2})}(2\sin 45^{0})= \frac{2\sqrt{2}\mu_{0}I}{\pi a}$