Table of Contents

Overview
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In 1924, Louis de Broglie proposed in his PhD thesis that all matter exhibits wave-like properties. This revolutionary idea unified the wave-particle duality of light with the behavior of material particles.

The Hypothesis
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If light (waves) can behave like particles (photons), then particles might behave like waves!

de Broglie Wavelength
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$$ \lambda = \frac{h}{p} = \frac{h}{mv} $$

Where:

  • \(\lambda\): de Broglie wavelength
  • \(h\): Planck’s constant
  • \(p\): Momentum
  • \(m\): Mass
  • \(v\): Velocity

de Broglie Frequency
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$$ \nu = \frac{E}{h} $$

Reasoning
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From Photons
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For photons:

  • Energy: \(E = h\nu\)
  • Momentum: \(p = E/c = h\nu/c = h/\lambda\)

Extended to Matter
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de Broglie proposed the same relation holds for particles:

$$ p = \frac{h}{\lambda} \implies \lambda = \frac{h}{p} $$

Wave-Particle Relations
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Particle PropertyWave PropertyRelation
Energy \(E\)Frequency \(\nu\)\(E = h\nu\)
Momentum \(p\)Wavelength \(\lambda\)\(p = h/\lambda\)

Example Calculations
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Electron at 100 eV
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$$ v = \sqrt{\frac{2E}{m}} = \sqrt{\frac{2 \times 100 \times 1.6 \times 10^{-19}}{9.11 \times 10^{-31}}} \approx 5.9 \times 10^6 \text{ m/s} $$$$ \lambda = \frac{h}{mv} = \frac{6.63 \times 10^{-34}}{9.11 \times 10^{-31} \times 5.9 \times 10^6} \approx 0.12 \text{ nm} $$

Comparable to X-ray wavelengths!

Baseball (0.15 kg at 40 m/s)
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$$ \lambda = \frac{6.63 \times 10^{-34}}{0.15 \times 40} \approx 10^{-34} \text{ m} $$

Far too small to detect—explains why we don’t see quantum effects in everyday objects.

Bohr Model Connection
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de Broglie waves explain Bohr’s quantization condition:

Standing Wave Requirement
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Electron wave must form standing wave around orbit:

$$ 2\pi r = n\lambda $$

Substituting de Broglie Wavelength
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$$ 2\pi r = n \frac{h}{mv} $$$$ mvr = n\frac{h}{2\pi} = n\hbar $$

This is exactly Bohr’s quantization condition!

n = 3:  ●───●───●  (3 wavelengths around orbit)
         \     /
          ●───●

Experimental Confirmation
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Davisson-Germer Experiment (1927)
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  • Electrons scattered from nickel crystal
  • Diffraction pattern observed
  • Confirmed wave nature of electrons

Measured wavelength matched de Broglie prediction.

Thomson Electron Diffraction (1927)
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  • Electrons through thin metal foil
  • Ring diffraction pattern
  • Like X-ray diffraction

G.P. Thomson (son of J.J. Thomson who discovered the electron particle!) showed its wave nature.

Wave Properties of Matter
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Phase Velocity
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$$ v_p = \frac{\omega}{k} = \frac{E}{p} = \frac{c^2}{v} $$

Greater than \(c\) for massive particles! (Not physical velocity)

Group Velocity
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$$ v_g = \frac{d\omega}{dk} = \frac{dE}{dp} = v $$

Equals particle velocity—carries energy and information.

Wave Packet
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Particle localized by superposition of waves:

$$ \Psi(x, t) = \int A(k) e^{i(kx - \omega t)} dk $$

Implications
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1. Electron Microscopy
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  • Electron wavelength < visible light
  • Higher resolution possible
  • TEM, SEM, STEM

2. Quantum Tunneling
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  • Wave can penetrate barriers
  • Essential for many phenomena

3. Semiconductor Devices
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  • Electron wave effects in small structures
  • Quantum wells, wires, dots

4. Uncertainty Principle
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Wave packets have:

$$ \Delta x \cdot \Delta k \geq \frac{1}{2} $$

Since \(p = \hbar k\):

$$ \Delta x \cdot \Delta p \geq \frac{\hbar}{2} $$

Historical Context
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de Broglie’s thesis was initially met with skepticism. Einstein supported it enthusiastically, saying:

“He has lifted a corner of the great veil.”

Nobel Prize
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Louis de Broglie received the Nobel Prize in Physics in 1929:

“For his discovery of the wave nature of electrons”

His work laid the foundation for wave mechanics and Schrödinger’s equation.