To address this problem, we must apply the principles of superposition and interference for coherent light waves. When two coherent light waves, each with amplitude 'a', interfere, the resultant intensity \( I \) is determined by the equation:
Here, \( I_1 \) and \( I_2 \) represent the intensities of the individual waves, and \( ϕ \) is the phase difference between them. The intensity of a wave is directly proportional to the square of its amplitude:
Given that \( I_1 = a^2 \) and \( I_2 = a^2 \) for each wave, substituting these values into the interference intensity equation yields:
This equation simplifies to:
The intensity's value fluctuates based on \( cosϕ \), which can range from -1 to 1. Consequently, the minimum intensity \( I_{min} \) is achieved when \( cosϕ = -1 \):
The maximum intensity \( I_{max} \) occurs when \( cosϕ = 1 \):
Therefore, the light intensity spans a range from 0 to \( 4a^2 \). The conclusive answer is:
0 and \( 4a^2 \)