Step 1: Understanding the Concept:
The electric field at the origin is the vector sum of the electric fields produced by each individual charge. An electric field points away from a positive charge and toward a negative charge.
Step 2: Key Formula or Approach:
Electric field due to a point charge: \(\vec{E} = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2} \hat{r}\).
Step 3: Detailed Explanation:
1. Charge \(-Q\) is at \((d, 0)\). The distance is \(d\). Since it is negative, the field \(\vec{E}_1\) at the origin points \textit{toward} the charge, i.e., in the \(+\hat{i}\) direction:
\[ \vec{E}_1 = \frac{1}{4\pi\epsilon_0} \frac{Q}{d^2} \hat{i} \]
2. Charge \(+Q\) is at \((0, d)\). The distance is \(d\). Since it is positive, the field \(\vec{E}_2\) at the origin points \textit{away} from the charge, i.e., in the \(-\hat{j}\) direction:
\[ \vec{E}_2 = \frac{1}{4\pi\epsilon_0} \frac{Q}{d^2} (-\hat{j}) \]
3. Resultant field \(\vec{E} = \vec{E}_1 + \vec{E}_2\):
\[ \vec{E} = \frac{1}{4\pi\epsilon_0} \frac{Q}{d^2} \hat{i} - \frac{1}{4\pi\epsilon_0} \frac{Q}{d^2} \hat{j} = \frac{1}{4\pi\epsilon_0} \frac{Q}{d^2} (\hat{i} - \hat{j}) \]
Note: The magnitude is \(\frac{Q\sqrt{2}}{4\pi\epsilon_0 d^2}\), but the vector form matches option (A) if we consider the unit vector components.
Step 4: Final Answer:
The electric field is \(\frac{1}{4\pi\epsilon_0} \frac{Q}{d^2} (\hat{i} - \hat{j})\). (Note: There appears to be a factor of \(\sqrt{2}\) discrepancy in the option labels versus the sum, but (A) is the closest vector representation).