Step 1: The time-averaged intensity of an electromagnetic wave in terms of the electric field amplitude \(E_0\) is
\[I=\frac{1}{2}c\varepsilon_0 E_0^{2}.\]
Step 2: Solve for \(E_0\):
\[E_0=\sqrt{\frac{2I}{c\varepsilon_0}}=\sqrt{\frac{2(2.5\times10^{14})}{(3\times10^{8})(8.85\times10^{-12})}}.\]
Step 3: Evaluate. The denominator \(c\varepsilon_0=2.655\times10^{-3}\), so
\[E_0=\sqrt{\frac{5.0\times10^{14}}{2.655\times10^{-3}}}=\sqrt{1.88\times10^{17}}=4.3\times10^{8}\,\text{N/C}.\]
Step 4: The magnetic field amplitude is
\[B_0=\frac{E_0}{c}=\frac{4.3\times10^{8}}{3\times10^{8}}=1.44\,\text{T}.\]
This matches option (A).
\[\boxed{E_0\approx4.3\times10^{8}\,\text{N/C},\quad B_0\approx1.44\,\text{T}}\]