Particle in a box
Boundary value problem where one needs to find the solution for the problem given that the potential is ∞ at the boundaries. Thus the particle is completely confined to a region and the wave function that describes this state must reflect that condition.
Method divide the spce up into regions and solve the problem in each region:
Region 1: x<0 ![]()
Region 3: x>0 ![]()
Region 2: a>x>0
Solutions that are
energy eigenstates.
Examine the Hamitonian and find the eigenstates

To get the BC one has B=0 and ![]()

We find that :
· Energy eigenstates are not eigenstates of either momentum or position.
· We can find the average location and average momentum for any eigenstates.
· There are many acceptable states that have a definite energy.
· The time evolution for a specific state is a solution to the Schrodinger equation

· A general solution, a legitimate possibility for the particle located in a box is

A solution at some time that will now need to evolve based on the Schrödinger equation.
Be clear:
·
is a solution or a
prepared state at a fixed time that must evolve
·
is
a very specific solution it usually has
the property that the wavefunction is a solution to
some operator eigenequation and therefore there are an associated set of eginevalues labeled by n.
·
implies
that that time dependence of this state is included. This can be very general.
So far we have only examined the particularly simple time evolution of an
energy eigenstates.
Consider the earth in orbit around the sun.
State
the earth is located
at some distance from the sun and moving with some momentum.
Result is an orbit.
|
State |
|
|
This state evolves in time based on ·
· Lagrangian · Hamiltonian · Your favorite formulation |
This state evolves in time based on ·
· Lagrangian · Hamiltonian · Your favorite formulation |
|
Classical formulation
|
Quantum formulation
|
|
Result is an orbit. |
|