If two light waves of intensities \( I \) and \( 4I \) superimpose at a point with a phase difference of \( \frac{\pi}{2} \), then the resultant intensity at that point is
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When light waves interfere with a phase difference of \( \frac{\pi}{2} \), the cross-term vanishes due to \( \cos\left( \frac{\pi}{2} \right) = 0 \).