Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 39 - More about Matter Waves - Problems - Page 1216: 21a

Answer

See in "step by step solution"

Work Step by Step

For the region $x > L$, Schrödinger’s equation is given by $\frac{d^2\psi}{dx^2}+\frac{8\pi^2m}{h^2}(E-U_0)\psi=0$ If $\psi= De^{2kx}$, then $\frac{d^2\psi}{dx^2}+\frac{8\pi^2m}{h^2}(E-U_0)\psi\\ =D4k^2e^{2kx}+\frac{8\pi^2m}{h^2}(E-U_0)De^{2kx}\\ =De^{2kx}[4k^2+\frac{8\pi^2m}{h^2}(E-U_0)$] The above equation will be zero, if $4k^2+\frac{8\pi^2m}{h^2}(E-U_0)=0$ or, $k=\frac{\pi}{h}\sqrt{2m(U_0-E)}$ Therefore, $\psi= De^{2kx}$, is a solution of Schrödinger’s equation in its one dimensional form, where D is a constant and k is positive provided $k=\frac{\pi}{h}\sqrt{2m(U_0-E)}$.
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