Introduction To Quantum Mechanics
Introduction To Quantum Mechanics
3rd Edition
ISBN: 9781107189638
Author: Griffiths, David J., Schroeter, Darrell F.
Publisher: Cambridge University Press
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Chapter 9.1, Problem 9.1P
To determine

The allowed energies En of an infinite square well with a “shelf,” of height V0, extending half-way across V(x)={V0(0<x<a/2)0(a/2<x<a)(otherwise) using WKB approximation. And compare the result with result from Section 7.1.2 using first-order perturbation theory.

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Question 2 2.1 Consider an infinite well for which the bottom is not flat, as sketched here. If the slope is small, the potential V = 6 |x|/ a may be considered as a perturbation on the square- well potential over -a/2 ≤x≤a/2. -8 W V(x) a/2 -a/2 X Calculate the ground-state energy, correct to first order in perturbation theory. Given (0) = √²/co COS Ground state of box of size a: = Ground state energy: E(0) = 4²k² 2ma². 0 Y
Q.8: Find the center and radius of convergence of the power series 2n=1 m(n+1) (z)2n+1 Q.9: Find the McLaurin series and its radius of convergence of 3iz Q.10: Find the Laurent series that converges for 0 < I z – z,I < R and determine the precise z, = iT region of convergence: (z-in)*
PROBLEM 2. Consider a spherical potential well of radius R and depth Uo, so that the potential is U(r) = -Uo at r R. Calculate the minimum value of Uc for which the well can trap a particle with l = 0. This means that SE at Uo > Uc has at least one bound ground state at l = 0 and E < 0. At Ug = Uc the bound state disappears.
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