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 2.5, Problem 2.27P

(a)

To determine

To sketch the given double delta potential.

(b)

To determine

The number of bound states, the allowed energies for α=2/ma, and α=2/4ma and to sketch the wave functions.

(c)

To determine

The bound state energies for the limiting cases (i) a0 and (ii) a.

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Problem 2. Consider the double delta-function potential V(x) = a[8(x + a) + 8(x − a)], where a and a are positive constants. (a) Sketch this potential. (b) How many bound states does it possess? Find the allowed energies, for a = ħ²/ma and for a = ħ²/4ma, and sketch the wave functions.
Consider a quantum system in the initial state ly (0) = |x,) at r = 0, and the Hamiltonian H = (252 0 written in the ΠΩ standard basis {12+). Iz-)}, and 2 a constant frequency. Let (r)) be the state of the system at later time 7. What is the probability that a measurement of S, at 1>0 yields +h/2? a. P (S, = +) (t) = [1 + 2 cos(r)] b. P (S,+) (1)= [1 + cos(20)] C. = P(S,+) (1)= [1 + sin(r)] d. P(S,+)(t)= |sin(r)| = e. P(S,+) (1)= [1 + cos(r)]
A quantum mechanical particle is confined to a one-dimensional infinite potential well described by the function V(x) = 0 in the region 0 < x < L, V(x) = ∞ elsewhere. The normalised eigenfunctions for a particle moving in this potential are: Yn(x) = √ 2 Nπ sin -X L L where n = 1, 2, 3, .. a) Write down the expression for the corresponding probability density function. Sketch the shape of this function for a particle in the ground state (n = 1). b) Annotate your sketch to show the probability density function for a classical particle moving at constant speed in the well. Give a short justification for the shape of your sketch. c) Briefly describe, with the aid of a sketch or otherwise, the way in which the quantum and the classical probability density functions are consistent with the correspondence principle for large values of n.
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