Title: Final Exam
1Final Exam
- Comprehensive
- Date Tuesday May 4, 2004
- Location MSC 220
- Time 6-8 pm
227.6 Photons and Electromagnetic Waves
- Light has a dual nature. It exhibits both wave
and particle characteristics - Applies to all electromagnetic radiations
- The photoelectric effect and Compton scattering
offer evidence for the particle nature of light - When light and matter interact, light behaves as
if it were composed of particles - Interference and diffraction offer evidence of
the wave nature of light
3Possible Application of the Particle Feature in
Space
- Sunlight striking the sail creates a force that
pushes the spaceship away from the sun, much as
the wind propels a sail-boat.
427.7 Wave Properties of Particles
- In 1924, Louis de Broglie postulated that because
photons have wave and particle characteristics,
perhaps all forms of matter have both properties - Furthermore, the frequency and wavelength of
matter waves can be determined
5Matter waves The de Broglie Wavelength and
Frequency
- Since a photon travels with speed of light, we
treat it as a massless particle with the
momentum - pE/chf/ch/l (Photons only m0!)
- Wavelength of the matter wave
- lh/ph/(mv) (Classical particles m?0!)
- A particle has a wave with frequency fE/h
associated with it!
6The Davisson-Germer Experiment
- In 1927, Davisson and Germer, working at Bell
Labs, were studying the nature of the surface of
a nickel crystal by directing a beam of electrons
at the surface and observing the electrons
reflected at various angles. They found that the
electrons were reflected in almost the same way
that x-ray would be reflected. The results gave
strong support to de Broglies hypothesis.
7The Transmission Electron Microscope
- The electron microscope depends on the wave
characteristics of electrons - Microscopes can only resolve details that are
slightly smaller than the wavelength of the
radiation used to illuminate the object - The electrons can be accelerated to high energies
and have small wavelengths
827.8 The Wave Function
- In 1926 Schrödinger proposed a wave equation that
describes the manner in which matter waves change
in space and time - Schrödingers wave equation is a key element in
quantum mechanics - Schrödingers wave equation is generally solved
for the wave function, ?
9Wavefunction, cont.
- In quantum mechanics ???2 is proportional to the
probability of finding the particle at a given
location.
The probability of finding the ground state
hydrogen electron (n1) as a function of the
radial distance from the proton.
10The Wave Function, final
- The wave function depends on the particles
position and the time - The value of ???2 at some location at a given
time is proportional to the probability of
finding the particle at that location at that time
1127.9 The Uncertainty Principle
Moving car
Past
Future
-x
x
Now
12The Uncertainty Principle, cont.
- What means exact? ? Deterministic view of nature
- ? This is ok in our world! But not in the world
of the electron
13The Uncertainty Principle, cont.
- (a) A photon hits an electron and (b) transfers
momentum to the electron.
The observation "destroys" the phenomen
14The Uncertainty Principle, cont.
- It is impossible to know (or to measure)
simultaneously an electrons EXACT position and
momentum! - Erwin Schroedinger (1887-1961) and Werner
Heisenberg (1901-1976) independently developed a
new branch of physics called quantum mechanics.
Quantum theory (its a small world!) predicts
limits on the accuracy of measurements. This idea
was introduced in 1927 by Heisenberg and
complemented Schroedingers wave theory.
15The Uncertainty Principle, cont.
To see more clearly into the nature of
uncertainty, we consider electrons passing
through a slit
Momentum uncertainty in the y component
We apply the formula for single slit diffraction,
sin?l/W, and postulate that l is the de Broglie
wavelength.
16The Uncertainty Principle, cont.
- sinq?tanq (for small q)
- tanqDpy/px ? Dpy/px?l/W
-
17The Uncertainty Principle, cont.
- Since the electron can pass the slit through
anywhere over the width W, the uncertainty in the
y position of the electron is DyW.
18The Uncertainty Principle, cont.
- Heisenberg found that at the very best
- DpyDy?h/(4p)
Momentum
Position
Uncertainty
19The Uncertainty Principle, cont.
- Dy/c?l/c ? Dt?l/c (This is the time that the
particle needs to traverse its own uncertainty,
which is on the order of its wavelength) - DE?hc/l
- (DE)(Dt)?(hcl)/(lc)
- (DE)(Dt)?h
20The Uncertainty Principle, final
(DE)(Dt)?h/(4p)
Energy uncertainty of a particle when the
particle is in a certain state
Time interval during which the particle is in the
state
21- Example Assume the position of an object is
known so precisely that the uncertainty in the
position is only Dy1.5?10-11 m. Determine the
minimum uncertainty in the momentum of the object
and find the corresponding minimum uncertainty in
the speed if the object in an electron. - Dpyh/(4pDy)(6.63?10-34 Js)/(4p1.5?10-11 m)
- Dpy3.5?10-24 kgm/s ? small
- DvyDpy/m(3.5?10-24 kgm/s)/(9.1?10-31 kg)
- Dvy3.9?106 m/s ? large
22Scanning Tunneling Microscope (STM)
- Allows highly detailed images with resolution
comparable to the size of a single atom - A conducting probe with a sharp tip is brought
near the surface - The electrons can tunnel across the barrier of
empty space
23Scanning Tunneling Microscope, cont.
- By applying a voltage between the surface and the
tip, the electrons can be made to tunnel
preferentially from surface to tip - The tip samples the distribution of electrons
just above the surface - The STM is very sensitive to the distance between
the surface and the tip - Allows measurements of the height of surface
features within 0.001 nm
24Limitation of the STM
- There is a serious limitation to the STM since it
depends on the conductivity of the surface and
the tip - Most materials are not conductive at their
surface - An atomic force microscope (AFM) has been
developed that overcomes this limitation - It measures the force between the tip and the
sample surface - Has comparable sensitivity