Title: Lecture 14: Schrdinger and Matter Waves
1Lecture 14 Schrödinger and Matter Waves
2Particle-like Behaviour of Light
- Plancks explanation of blackbody radiation
- Einsteins explanation of photoelectric effect
3de 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)
4de Broglie Wavelength
Relates a particle-like property (p) to a
wave-like property (l)
5Wave-Particle Duality
particle
wave function
6Example 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
7Example 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
8Wave 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?
9Copenhagen 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)
10Imagine a Roller Coaster ...
By conservation of energy, the car will climb up
to exactly the same height it started
11Conservation 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
12Electron Roller Coaster
An incoming electron will oscillate betweenthe
two outer negatively charged tubes
13Schrödingers 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)
14Wave-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
15Electron Diffraction
X-rays
electrons
The diffraction patterns are similar because
electrons have similar wavelengths to X-rays
16Bragg 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)
17Resolving 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
18Scanning Electron Microscope (SEM)
- To resolve even smaller objects, have to use
electronswith wavelengths equivalent to X-rays
Virtual SEM
19Particle 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)
20Conventional Lithography
21Limits 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
22Proton Beam Micromachining (NUS)
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