Final answer:
The integral identity with exponential functions involves concepts like complex analysis and Wick rotation in quantum field theory, with a need for careful mathematical justification and selection of a branch cut for square roots of complex numbers.
Step-by-step explanation:
The integral identity in question is an example of a Gaussian integral, which is encountered frequently in quantum field theory and statistical mechanics. The use of imaginary numbers is fundamental in quantum mechanics, as indicated by wave functions like Y(x, t) = Aei(kx-wt), where the imaginary unit i = √-1 ensures compliance with the Schrödinger equation. Real functions such as sine and cosine waves cannot satisfy the Schrödinger equation; thus, the complex exponential form of the wave function is required.
To understand the integral mentioned and its issues with convergence, consider Wick rotation, which is a technique used to redefine the time coordinate in a complex plane to improve the behavior of the integral. By rotating the time axis into the complex plane, we analytically continue our functions to make certain integrals converge where they otherwise would not. However, this is not a trivial process and requires careful justification. The appearance of iε (where ε is a small positive value) in the prescriptions is to ensure the convergence of the integral and stems from the need to modify the physical problem in a way that makes mathematical sense.
The right-hand side of the integral identity involves the square root of a complex number, which indeed requires one to choose a branch cut to define the function properly. Physicists conventionally take the principal branch where the square root has a non-negative real part to maintain consistency with physical predictions.
For detailed proofs and deeper understanding, I recommend studying complex analysis, particularly residue calculus, and textbooks on quantum field theory, where such techniques are elucidated with mathematical rigor.