Decorative banner

E.2.2 De Broglie wavelength and diffraction (HL only)

De Broglie Hypothesis, Particle Diffraction, and Compton Scattering

  1. Imagine watching a tennis ball fly through the air. Would you ever think of it as a wave? Probably not.
  2. But what if I told you that every moving object, even a tennis ball, has an associated "wavelength"?
This idea might seem counterintuitive, but it lies at the heart of quantum mechanics.

The De Broglie Hypothesis: Particles as Waves

  1. In 1923, Louis de Broglie proposed a revolutionary idea: particles, such as electrons or protons, can exhibit wave-like properties.
  2. He introduced the concept of the de Broglie wavelength, which relates a particle’s momentum to its wavelength:

λ=hp

where:

  • λ is the particle’s wavelength (in meters),
  • h is Planck’s constant 6.63×1034Js,
  • p is the particle’s momentum p=mv, where m is mass and v is velocity.

Note

This hypothesis suggests that all moving particles, no matter how small or large, have an associated wavelength.

Why Does This Matter?

  1. The de Broglie hypothesis bridges the classical and quantum worlds.
  2. It shows that particles, which we often think of as discrete points, can behave like waves under certain conditions.
  3. This duality—particles behaving as waves—is a fundamental concept in quantum mechanics.

Analogy

Think of a particle like a musician playing a single note. The de Broglie wavelength is like the pitch of that note, revealing deeper information about the particle’s behavior, especially when it interacts with its surroundings.

Particle Diffraction: Evidence for Wave Behavior

  1. If particles truly exhibit wave-like properties, we should be able to observe phenomena like diffraction and interference, which are characteristic of waves.
  2. This was experimentally confirmed in 1927 by the Davisson-Germer experiment.

The Davisson-Germer Experiment

  1. In this experiment, electrons were accelerated through a potential difference and directed at a nickel crystal.
  2. The scattered electrons produced a pattern of bright and dark spots, similar to the diffraction patterns seen with light waves passing through a slit.
Schematics drawing of the Davisson-Germer experiment.
Schematics drawing of the Davisson-Germer experiment.
  • The key finding: the spacing of the diffraction pattern matched the de Broglie wavelength of the electrons, calculated using:

λ=h2meqV

where:

  • me is the electron’s mass 9.11×1031kg,
  • q is the electron’s charge 1.60×1019C,
  • V is the accelerating voltage.

Example

For example, if electrons are accelerated through a potential difference of 54 V, their de Broglie wavelength is approximately 1.7×1010m, which is comparable to the spacing between atoms in a crystal.

  • This experiment provided direct evidence that particles like electrons exhibit wave-like properties, validating de Broglie’s hypothesis.

Tip

Electron diffraction is a key technique in electron microscopy, enabling scientists to study materials at the atomic scale.

Compton Scattering: Photons as Particles

While the de Broglie hypothesis showed that particles can behave like waves, Compton scattering demonstrated that waves (light) can behave like particles.

The Compton Effect

  1. In 1923, Arthur Compton observed that when X-rays scatter off electrons, the wavelength of the scattered X-rays increases.
  2. This phenomenon is best explained by treating light as a stream of particles, or photons.
  3. When a photon collides with an electron, it transfers energy and momentum to the electron, causing the photon to lose energy (and increase its wavelength).
  4. The change in wavelength, Δλ, is described by:

Δλ=hmec(1cosθ)

where:

  • Δλ is the wavelength shift (in meters),
  • me is the electron’s mass,
  • c is the speed of light 3.0×108m/s,
  • θ is the scattering angle.
Illustration of the Compton effect.
Illustration of the Compton effect.

Key Observations

  • The wavelength shift depends only on the scattering angle θ, not on the photon’s initial wavelength.
  • The largest shift occurs when θ=180 (backscattering).

Example

For instance, consider an X-ray photon with a wavelength of 1.0×1012m scattering off an electron at an angle of 90.

The wavelength shift is:

Δλ=6.63×10349.11×1031×3.0×108(1cos90)

Δλ=2.43×1012,m

The scattered photon’s wavelength becomes 1.0×1012+2.43×1012=3.43×1012m.

Why Is This Important?

Compton scattering confirmed that photons have momentum, a property traditionally associated with particles. This discovery further solidified the concept of wave-particle duality.

Note

The quantity hmec, known as the Compton wavelength, is approximately 2.43×1012m for an electron. It is a fundamental constant in quantum mechanics.

Applications: Electron Microscopy and Material Analysis

The principles of wave-particle duality and diffraction have led to transformative technologies, particularly in electron microscopy.

Electron Microscopy

  1. Electron microscopes exploit the wave-like properties of electrons to achieve resolutions far beyond those of optical microscopes.
  2. Since the de Broglie wavelength of electrons is much smaller than the wavelength of visible light, electron microscopes can resolve structures at the atomic scale.

Material Analysis

  1. Electron diffraction is a powerful tool for studying the arrangement of atoms in materials.
  2. By analyzing diffraction patterns, scientists can determine the crystal structure of a material, which is essential for fields like materials science and nanotechnology.

Reflection

Self review

  1. What is the de Broglie wavelength of an electron moving at 2.0×106m/s?
  2. How does Compton scattering provide evidence for the particle nature of light?
  3. Why is electron diffraction significant in confirming the wave-like properties of particles?

Theory of Knowledge

  1. How does the wave-particle duality of electrons challenge our classical understanding of observation?
  2. Could this idea connect to broader philosophical questions about the nature of reality?

The de Broglie hypothesis, particle diffraction, and Compton scattering reveal the dual nature of matter and light: particles can behave like waves, and waves can behave like particles.

Jojo winking

You've read 2/2 free chapters this week.

Upgrade to PLUS or PRO to unlock all notes, for every subject.

Questions

Recap questions

1 of 5

Question 1

Consider an electron moving with a velocity of 2.0×106m/s2.0 \times 10^6 \, \mathrm{m/s}. The mass of an electron is 9.11×1031kg9.11 \times 10^{-31} \, \mathrm{kg} and Planck's constant is 6.63×1034Js6.63 \times 10^{-34} \, \mathrm{Js}.

End of article
Flashcards

Remember key concepts with flashcards

22 flashcards

What is momentum in terms of mass and velocity?

Lesson

Recap your knowledge with an interactive lesson

9 minute activity

Note

Wave-Particle Duality

  • In 1924, Louis de Broglie proposed that all matter exhibits both particle and wave properties
  • This means that every moving object has a wavelength, just like light waves
  • The concept was revolutionary because it suggested that particles like electrons could behave like waves under certain conditions

Analogy

Think of a basketball - we usually see it as a solid object, but de Broglie's idea is like saying it also has an invisible wave pattern surrounding it as it moves.

Definition

Wave-Particle Duality

The concept that all matter exhibits both particle and wave properties.

Example

An electron moving through space has a wavelength, just like a beam of light.

Note

This idea laid the foundation for quantum mechanics.