The stopping potential \( V_0 \) is directly proportional to the kinetic energy of the photoelectrons. As the frequency of the incident radiation rises, so does the stopping potential. Consequently, for a fixed frequency, the metal exhibiting the highest stopping potential will yield photoelectrons with the maximum kinetic energy. In the provided graph, metal A demonstrates the highest stopping potential \( V_0 \) at any given frequency. This observation signifies that metal A liberates photoelectrons with the greatest kinetic energy.