Introduction to Quantum Mechanics · Problem 2.23

Time-Independent Schrödinger Equation — David J. Griffiths

Physics — Quantum Mechanics · delta_function_properties

Problem

Delta functions live under integral signs, and two expressions (D1(x)D_1(x) and D2(x)D_2(x)) involving delta functions are said to be equal if ∫−∞+∞f(x) D1(x) dx=∫−∞+∞f(x) D2(x) dx,\int_{-\infty}^{+\infty} f(x)\,D_1(x)\,dx = \int_{-\infty}^{+\infty} f(x)\,D_2(x)\,dx, for every (ordinary) function f(x)f(x). (a) Show that δ(cx)=1∣c∣δ(x),\delta(cx) = \frac{1}{|c|}\delta(x), where cc is a real constant. (Be sure to check the case where cc is negative.) (b) Let θ(x)\theta(x) be the step function: θ(x)≡{1,x>0,0,x<0.\theta(x) \equiv \begin{cases} 1, & x > 0, \\ 0, & x < 0. \end{cases} (In the rare case where it actually matters, we define θ(0)\theta(0) to be 1/21/2.) Show that dθ/dx=δ(x)d\theta/dx = \delta(x).

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