Step 1: Read the figure
Current runs along \(AB\), turns down along \(BC\), and along \(DE\) turns up along \(ET\). The vertical wires are separated by \(a\), so each is at distance \(\frac a2\) from \(O\). The horizontal wires lie along the line through \(O\) and give no field there.
Step 2: Field of one semi-infinite wire
The foot of the perpendicular from \(O\) is at the end of each vertical wire, so each gives \(B = \frac{\mu_0I}{4\pi\left(\frac a2\right)} = \frac{\mu_0I}{2\pi a}\).
Step 3: Directions
Wire \(BC\) (current downward, to the left of \(O\)) and wire \(ET\) (current upward, to the right of \(O\)) both give a field out of the page at \(O\) by the right-hand rule. So the fields add.
Step 4: Total
\(B = 2\times\frac{\mu_0I}{2\pi a} = \frac{\mu_0I}{\pi a}\). Option (D).
Final Answer:
The field at O is mu0 I / (pi a).
\[ \boxed{\text{(D)}\ \frac{\mu_0I}{\pi a}} \]