
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.