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Lecture 14: Schrdinger and Matter Waves

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Title: Lecture 14: Schrdinger and Matter Waves


1
Lecture 14 Schrödinger and Matter Waves
2
Particle-like Behaviour of Light
  • Plancks explanation of blackbody radiation
  • Einsteins explanation of photoelectric effect

3
de Broglie Suggested the converse
  • All matter, usually thought of as particles,
    should exhibit wave-like behaviour
  • Implies that electrons, neutrons, etc., are waves!

Prince Louis de Broglie (1892-1987)
4
de Broglie Wavelength
Relates a particle-like property (p) to a
wave-like property (l)
5
Wave-Particle Duality
particle
wave function
6
Example de Broglie wavelength of an electron
  • Mass 9.11 x 10-31 kgSpeed 106 m / sec
  • This wavelength is in the region of X-rays

7
Example de Broglie wavelength of a ball
  • Mass 1 kgSpeed 1 m / sec
  • This is extremely small! Thus, it is very
    difficult to observe the wave-like behaviour of
    ordinary objects

8
Wave Function
  • Completely describes all the properties of
    agiven particle
  • Called y y (x,t) is a complex function of
    position x and time t
  • What is the meaning of this wave function?

9
Copenhagen Interpretationprobability waves
  • The quantity y2 is interpreted as the
    probability that the particle can be found at a
    particular point x and a particular time t
  • The act of measurement collapses the wave
    function and turns it into a particle

applet
Neils Bohr (1885-1962)
10
Imagine a Roller Coaster ...
By conservation of energy, the car will climb up
to exactly the same height it started
11
Conservation of Energy
  • E K Vtotal energy kinetic energy
    potential energy
  • In classical mechanics, K 1/2 mv2 p2/2m
  • V depends on the system
  • e.g., gravitational potential energy, electric
    potential energy

12
Electron Roller Coaster
An incoming electron will oscillate betweenthe
two outer negatively charged tubes
13
Schrödingers Equation
  • Solve this equation to obtain y
  • Tells us how y evolves or behaves in a given
    potential
  • Analogue of Newtons equation in classical
    mechanics

applet
Erwin Schrödinger (1887-1961)
14
Wave-like Behaviour of Matter
  • Evidence
  • electron diffraction
  • electron interference (double-slit experiment)
  • Also possible with more massive particles, such
    as neutrons and a-particles
  • Applications
  • Bragg scattering
  • Electron microscopes
  • Electron- and proton-beam lithography

15
Electron Diffraction
X-rays
electrons
The diffraction patterns are similar because
electrons have similar wavelengths to X-rays
16
Bragg Scattering
Bragg scattering is used to determine the
structure of the atoms in a crystal from the
spacing between the spots on a diffraction
pattern (above)
17
Resolving Power of Microscopes
  • To see or resolve an object, we need to use light
    of wavelength no larger than the object itself
  • Since the wavelength of light is about 0.4 to 0.7
    mm,an ordinary microscopecan only resolve
    objectsas small as this, such asbacteria but
    not viruses

18
Scanning Electron Microscope (SEM)
  • To resolve even smaller objects, have to use
    electronswith wavelengths equivalent to X-rays

Virtual SEM
19
Particle Accelerator
  • Extreme case of an electron microscope, where
    electrons are accelerated to very near c
  • Used to resolve extremely small distances e.g.,
    inner structure of protons and neutrons

Stanford Linear Accelerator (SLAC)
20
Conventional Lithography
21
Limits of Conventional Lithography
  • The conventional method of photolithography hits
    its limit around 200 nm (UV region)
  • It is possible to use X-rays but is difficult to
    focus
  • Use electron or proton beams instead

22
Proton Beam Micromachining (NUS)
More information ...
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