(a) Resolving the magnetic moments along $OP$ and perpendicular to $OP,$ figure we find that component $OP$ perpendicular $OP$ cancel out. Resultant magnetic moment along $OP\ is = M\cos{45{^\circ} + M\ \cos 45{^\circ}}$
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$= 2\ M\cos\ 45{^\circ} = \frac{2M}{\sqrt{2}} = \sqrt{2}\ M$
The point $P$ lies on axial line of magnet of moment
$= \sqrt{2}\ M$
$\ \therefore B = \frac{\mu_{0}}{4\pi}\frac{2(\sqrt{2}\ M)}{d^{3}}$