Electron Double-Slit Interference
1 · Predict
Electrons fired one at a time through two narrow slits build up an interference pattern on a screen, just like light waves do. Does a faster electron (shorter de Broglie wavelength) produce wider or narrower interference fringes?
- Narrower fringes — fringe spacing is proportional to wavelength, and faster electrons have shorter wavelengths.
- Wider fringes for faster electrons.
- Fringe spacing doesn't depend on electron speed.
2 · Set Up
- Open the electron-double-slit preset and press Reset. Slit separation = 100 nm, screen distance = 50 cm.
- Enable the de Broglie wavelength and fringe-spacing readouts.
- Set the electron's kinetic energy for each trial and record the interference fringe spacing on the screen.
3 · Collect Data
| Kinetic energy K (eV) | De Broglie wavelength λ (pm) | Fringe spacing y (cm) |
|---|---|---|
| 100.00 | ||
| 150.00 | ||
| 200.00 |
Plot fringe spacing y (y-axis) against wavelength λ (x-axis) for your three trials. Is the line straight through the origin?
4 · Analyze
- For one trial, compute λ = h/√(2m_eK), then fringe spacing y = λL/d using screen distance L = 50 cm and slit separation d = 100 nm. Compare both to the table.
- Explain why this is the exact same double-slit fringe formula used for light — once you accept that electrons have a wavelength, their interference pattern obeys identical wave mathematics.
5 · Extend
- Remarkably, this interference pattern builds up even when electrons are fired through the apparatus one at a time, with long gaps between them. Explain why this rules out the idea that electrons are simply interfering with EACH OTHER, and instead suggests each electron somehow 'interferes with itself.'
- If you set up a detector to determine which slit each electron actually passed through, the interference pattern disappears — you get two simple bands instead. Why might 'measuring which path' fundamentally destroy the wave interference?
The Physics Behind This Experiment
De Broglie Wavelength
An electron with momentum p behaves as a wave with wavelength λ = h/p = h/√(2mK) — this is the wavelength that then sets the interference pattern. Just as with light, two coherent sources separated by distance d produce fringes spaced by y = λL/d on a screen at distance L; a faster (higher-K) electron has a shorter λ and so more tightly-spaced fringes.
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