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Quantum tunnelling University Quantum Mechanics I · Physics IV

Barrier Runner

Tune a barrier and electron energy to reach a target transmission probability.

Best score0 / 300 0 / 9 stars
LEVEL1

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0/3 challenges0/9 stars

Challenge 1 of 3

Narrow the barrier

Electrons have less energy than the barrier height. Control how thick a forbidden region they meet.

Mission targetExpected transmission10–15 %
SETUP PREVIEWWIDTHINCIDENT WAVETRANSMITTED WAVE0.1%Barrier: 0.80 nmOrange = particle energy · Wave height ∝ √probability

Challenge cleared. Continue to unlock the next experiment.Handles also support arrow keys; the sliders offer the same controls.

Electron energy0.50 eV
Barrier height1.50 eV
Particle masselectron mass

Tune the expected transmitted percentage into 10–15%.

Build your setup

Test 1

Restoring your saved experiment…

Adjust the experiment
0.8 nm
0.1 nm1 nm

3 stars on your first test; 2 within three; 1 after that. A first clear earns 100 XP plus 10 per star. Better star records earn the difference; repeating a record earns no extra XP.

Your experiment is ready.

Explore the exact rectangular-barrier transmission probability below and above the barrier, including above-barrier reflection.

0 of 3 challenges cleared · Best stars, unlocked rounds and your experiment are saved in this browser.

From the course to the controls

The physics behind the game

Explore the exact rectangular-barrier transmission probability below and above the barrier, including above-barrier reflection.

For E < V₀: T = [1 + V₀² sinh²(κa)/(4E(V₀ − E))]⁻¹; κ = √[2mₑ(V₀ − E)]/ℏ

Model assumptions. Exact stationary scattering for one electron mass and a real, one-dimensional rectangular barrier, with zero potential on both sides. Above the barrier, sin replaces sinh; the continuous E = V₀ limit is handled explicitly. The visual shows ensemble probabilities, not particle trajectories inside the barrier.