Physics 471: Normalization & Energy Eigenstates of Infinite Wells - Set 4, Assignments of Quantum Physics

Problem set 4 from physics 471, fall 2004. The problems involve normalization and expression of wave functions in terms of energy eigenstates for particles in infinite potential wells. The potential wells have different shapes and boundary conditions. Students are asked to find the wave functions, expectation values, and allowed bound state energies.

Typology: Assignments

Pre 2010

Uploaded on 07/28/2009

koofers-user-08o-1
koofers-user-08o-1 🇺🇸

5

(2)

10 documents

1 / 1

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Physics 471 Problem Set 4 Fall 2004
15. A particle of mass min an infinite potential well of width ahas the initial wave function
Ψ(x, 0) = Asin3(πx/a).
(a) Normalize Ψ(x, 0).
(b) Express Ψ(x, 0) in terms of the energy eigenstates
ψn(x) = s2
asin(nπx/a), n = 1,2,3,··· ,
as
Ψ(x, 0) = X
n
Cnψn(x).
Hint: There are only two terms in the expansion and they can be found by expressing
sin3(x) as a combination of sin(x) and sin(3x) using
e3ix = (cos(x) + isin(x))3.
(c) Obtain Ψ(x, t) and find hxias a function of time.
16. The wave function for a particle of mass mmoving in the potential
V=
for x= 0
0 for 0 < x a
V0for xa
is
ψ(x) = (Asin(kx) for 0 < x a
Ceκx for xa
with
k=s2mE
¯h2κ=s2m(V0E)
¯h2.
(a) Apply the boundary conditions at x=aand obtain the transcendental equation
which determines the bound state energies E.
(b) If
s2mV0a2
¯h2= 3π ,
determine the allowed bound state energies.
17. (a) Normalize the wave function for the lowest energy state in the previous problem.
(b) What is the probability that a measurement of the position of a particle in the ground
state will give a result a?

Partial preview of the text

Download Physics 471: Normalization & Energy Eigenstates of Infinite Wells - Set 4 and more Assignments Quantum Physics in PDF only on Docsity!

Physics 471 Problem Set 4 Fall 2004

  1. A particle of mass m in an infinite potential well of width a has the initial wave function

Ψ(x, 0) = A sin^3 (πx/a).

(a) Normalize Ψ(x, 0). (b) Express Ψ(x, 0) in terms of the energy eigenstates

ψn(x) =

√ 2 a

sin(nπx/a) , n = 1, 2 , 3 , · · · ,

as Ψ(x, 0) =

∑ n

Cnψn(x).

Hint: There are only two terms in the expansion and they can be found by expressing sin^3 (x) as a combination of sin(x) and sin(3x) using

e 3 ix^ = (cos(x) + i sin(x))^3.

(c) Obtain Ψ(x, t) and find 〈x〉 as a function of time.

  1. The wave function for a particle of mass m moving in the potential

V =

  

∞ for x = 0 0 for 0 < x ≤ a V 0 for x ≥ a

is ψ(x) =

{ A sin(kx) for 0 < x ≤ a Ce−κx^ for x ≥ a with k =

√ 2 mE ¯h^2

κ =

√ 2 m(V 0 − E) ¯h^2

(a) Apply the boundary conditions at x = a and obtain the transcendental equation which determines the bound state energies E. (b) If (^) √ 2 mV 0 a^2 ¯h^2

= 3π ,

determine the allowed bound state energies.

  1. (a) Normalize the wave function for the lowest energy state in the previous problem. (b) What is the probability that a measurement of the position of a particle in the ground state will give a result ≥ a?