The Fourier transform of e^{2\pi ikx} equals the delta function δ(k) because it behaves like a delta function, despite being a distribution rather than a conventional function. The integral does not converge for k ≠ 0, highlighting the idealized nature of the delta function, which is zero everywhere except at one point. The discussion emphasizes that while the delta function is not a function in the traditional sense, it serves a functional role similar to Fourier series coefficients in representing periodic functions. The Fourier transform operates within the framework of Hilbert space, where neither the delta function nor the exponential function fully meets the necessary criteria. For a rigorous understanding, exploring texts on distributions or generalized functions is recommended.