Problem 1:
Let A and B be two observables of a system with a two dimensional state space, and suppose measurements are made of A, B, and A again in quick succession. Show that the probability that the second measurement of A gives the same result as the first is independent of the initial state of the system.
Problem 2:
Find <x> and ∆x for the nth stationary state of a free particle in one dimension restricted to the interval 0 < x < a. Show that as n--> ∞ these become the classical values.
Problem 3:
A system makes transitions between eigenstates of H0
under the action of the time dependent Hamiltonian H0 + Wcosωt, W << H0.
Find an expression for the probability of transition from
||ψ1> to ||ψ2>,
where ||ψ1> and ||ψ2>
are eigenstates of H0 with eigenvalues E1 and E2.
Show that this probability is small unless E2 - E1 ≈ ħω.
[This shows that a charged particle in an oscillating electric field with angular
frequency w will exchange energy with the field only in
multiples of
E ≈ ħω.]
Consider
a one-dimensional system, with momentum operator p and position operator q.
(a) Show that
[q,pn] = iħ n pn-1.
(b) Show that
[q,F(p)] = iħ ∂F/∂p, if
the function F(p) can be defined by a finite polynomial or convergent power series
in the operator p.
(c) Show that
[q,p2F(q)] = 2iħ pF(q) if F(q)
is some function of q only.
Problem 5:
If
baryon number were not conserved in nature, the wave functions for neutrons
(n) and anti-neutrons (n) would not be stationary mass-energy
eigenfunctions.
Rather, the wave functions of such particles would be
oscillating, time-dependent superposition of neutron and anti-neutron
components, given by
Suppose
that such oscillations occur and the Hamiltonian of the system, neglecting
all degrees of freedom except for the one corresponding to the oscillations,
is
where E1 = m + U1 and E2 = m +
U2 are energies for n and
n
individually, and α
is a real mixing amplitude.
In
an external magnetic field B, the potential energies are U1
= μ∙B
and U2
= -μ∙B
where μ
≈ μn = -μn.
Suppose
that at time t = 0 the initial state is that of a neutron.
(a) Calculate the time-dependent probability for observing an anti-neutron.
Determine the period of oscillation.