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Chapter 1   Lecture 1 - Particle-Wave Duality

ie. light behaved like a electromagnetic wave in the early part of the 19th century. However when examined at low intensity it behaves more like a particle.

Matter also exibitics both a wave and particle nature.

1.1   The Photoelectric Effect (waves behaving like particles)


Figure 1.1 - Millikan's Experiment

Figure 1.2 - Graphing the Photoelectric Effect
Tmax=hn-f     (1.1)
f is the work function of the metal

Einstein postulated (1905) that EM radiation of frequency n can behave as if it consists of discrete units (quanta) with energy hn .

Light behaves like a quanta but also like a wave
Photon Properties:
E=hn     (1.2)
from Compton Scattering
p=
h
l
    (1.3)
Wave Properties:
F (the electric field amplitude) obeys a wave equation. So in free space
2F
t2
=c2
2F
x2
    (1.4)
this has a sinusoidal solution
F=F0sin(kx-w t)     (1.5)
k=2p/l wave vector, w =2pn angular frequency
using the definition that
=
h
2p
and equations I.2 and I.3 we obtain
k=
p
 
w =
E
 
    (1.6)

1.2   Electron Diffraction (particles behaving like waves)

an experiment in 1927-28 Davissan and Germer (USA) and also G.P. Thomson (IC) discovered this effect.

Figure 1.3 - Electron Diffraction Experiment
Diffraction pattern was identical to X-rays therefore since electrons give diffraction, electrons behave like waves. They found that l=h/p .

de Broglie postulated that electrons have wave like properties.
p= k E=w     (1.7)
All particles display
wave like
properties, for example
matter wave
properties (http://www.quantum.univie.ac.uk/)

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