1. Quantum Mechanics

2. Anatomy of a classical travelling wave

3. adding varying amounts of an infinite number of waves
Given the Uncertainty Principle, how do you write an equation of motion for a particle?
First, remember that a particle is only a particle sort of, and a wave sort of, and it’s not quite like anything you’ve encountered in classical physics.
We need to use Fourier’s Theorem to represent the particle as the superposition of many waves.
adding varying amounts of an infinite number of waves
sinusoidal expression for harmonics
wavefunction of the electron
amplitude of wave with wavenumber k=2p/l

4. probability for an electron to be found between x and x+dx Y(x,t)
We saw a hint of probabilistic behavior in the double slit experiment. Maybe that is a clue about how to describe the motion of a “particle” or “wavicle” or whatever.
We can’t write a deterministic equation of motion as in Newtonian Mechanics, however, we know that a large number of events will behave in a statistically predictable way. dx
probability for an electron to be found between x and x+dx
Y(x,t) 2
Assuming this particle exists, at any given time it must be somewhere. This requirement can be expressed mathematically as:
you will find your particle once, not twice (that would be two particles) but once.
If you search from hither to yon

5. Wavefunction requirements

6. Superposition Principle
Conceptual definition
When two or more wave moving through the same region of space,
waves will superimpose and produce a well defined combined effect.
Mathematical definition
For a linear homogeneous ordinary differential equation,
if        and        are solutions, then so is               .
Standing Waves
When two waves of equal amplitude and frequency but opposite directions of travel superimpose, you get a standing wave- a wave that appears not to move-its nodes and anti-nodes stay in the same place. This happens when traveling waves on a guitar string get to the end of the string and are reflected back.

7. The wavefunction
Graphical representation of a complex number z as a point in the complex plane. The horizontal and vertical Cartesian components give the real and imaginary parts of z respectively.
Note that we can construct a wavefunction only if the momentum is not precisely defined. A plane wave is unrealistic since it is not normalizable.
You can’t get around the uncertainty principle!

8. Schrodinger Equation for a free particle
Alright, we think we might have an acceptable wavefunction. Let’s give it a whirl… If we think we know what our wavefunction looks like now, how do we propogate it through time and space?
The Schrodinger Equation:
Describes the time evolution of your wavefunction.
Takes the place of Newton’s laws and conserves energy of the system.
Since “particles” aren’t particles but wavicles, it won’t give us a precise position of an individual particle, but due to the statistical nature of things, it will precisely describe the distribution of a large number of particles.

9. Propogation of a free particle
If you know the position of a particle at time t=0, and you constructed a localized wave packet, superimposing waves of different momenta, then the wave will disperse because, by definition, waves of different momenta travel at different speeds.
the position of the real part of the wave…
time
the probability density

10. Schrodinger Equation in the presence of forces
expression for kinetic energy
kinetic plus potential energy gives the total energy
the potential
Spring analogy

11. Particle in a box
Remember our guitar string? We had the boundary condition that the ends of the string were fixed.
Quantum mechanical version- the particle is confined by an infinite potential on either side. The boundary condition- the probability of finding the particle outside of the box is ZERO!

12. The "Standing Waves" of Quantum Mechanics
For the quantum mechanical case:
For the guitar string:
Assume a general case:
Here show that time dependent part goes away when you multiply by the complex conjugate. Introduce the time independent schrodinger equation.

13. What the Uncertainty Principle tells us about the ground state
Note that while Y=0 solves the problem mathematically, it does not satisfy the conditions for the quantum mechanical wavefunction, because we know that at any given time, the particle must be found SOMEWHERE. N=0 is not a solution.
Appealing to the uncertainty principle can give us a clue.

14. The time-independent Schrodinger equation
The wavefunction can be written as the sum of two parts.
Note that:
For a “stationary state” the probability of finding a particle is static!

15. Why quantization of angular momentum?
an integer number of wavelengths fits into the circular orbit
where
l is the de Broglie wavelength
We are beginning
to understand...