Step 1: In an EM wave, \(\vec{E}\), \(\vec{B}\), and the direction of propagation are all mutually perpendicular.
Step 2: If propagation is along the \(y\)-axis, both \(\vec{E}\) and \(\vec{B}\) must lie in the \(xz\)-plane.
Step 3: This means their components can only be in the \(x\) or \(z\) directions.
Step 4: Thus, the pairs must be (\(E_x, B_z\)) or (\(E_z, B_x\)).