Introduction to Quantum Mechanics · Problem 2.26

Time-Independent Schrödinger Equation — David J. Griffiths

Physics — Quantum Mechanics · fourier_transform

Problem

What is the Fourier transform of δ(x)\delta(x)? Using Plancherel's theorem, show that δ(x)=12π∫−∞+∞eikx dk.\delta(x) = \frac{1}{2\pi}\int_{-\infty}^{+\infty} e^{ikx}\,dk. Comment: This formula gives any respectable mathematician apoplexy. Although the integral is clearly infinite when x=0x = 0, it doesn't converge (to zero or anything else) when x≠0x \neq 0, since the integrand oscillates forever. There are ways to patch it up (for instance, you can integrate from −L-L to +L+L, and interpret Equation 2.147 to mean the average value of the finite integral, as L→∞L \to \infty). The source of the problem is that the delta function doesn't meet the requirement (square-integrability) for Plancherel's theorem (see footnote 42). In spite of this, Equation 2.147 can be extremely useful, if handled with care.

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