The wire carries a current I in the negative z-direction. We have to consider the magnetic vector field B→ at (x, y) in the z = 0 plane.
Magnetic field B→ is perpendicular to OP. ∴ B→ = b sin θ i^ - B cos θ j^​ sin θ = ry​ , cos θ = rx​ , B = 2πrμ0​I​ ∴ B→ = 2πr2μ0​I​(yi​−xj​) or B→ = 2π(x2+y2)μ0​I(yi​−xj​)​