Vector potential in classical electrodynamics is primarily viewed as a mathematical tool, with physical significance attributed only to electric and magnetic fields. Gauge transformations can alter potentials without affecting the fields, reinforcing this perspective. In quantum electrodynamics (QED), however, vector potential gains a physical interpretation, particularly demonstrated by the Aharonov-Bohm Effect, where it influences measurable outcomes despite the absence of fields. While vector potential is essential in QED, it remains non-observable, similar to wave functions, leading to debates about its reality versus its role as a mathematical representation. Ultimately, vector potential serves as a means to calculate physical observables, but its own reality is still contested.