Quantum tunneling is a physical process where a particle passes directly through an energy barrier it lacks the energy to climb over. Because subatomic particles behave like probability waves rather than solid objects, part of their wave function can appear on the far side of a barrier. This probability allows particles like electrons and protons to cross physical and electrical obstacles that classical physics would call impassable.
By the edgi team We find the most surprising true thing about an idea and build a 60-second lesson around it.
Imagine throwing a tennis ball at a brick wall. It bounces back every time. But at the subatomic scale, particles do not act like solid balls. They act like fuzzy clouds of probability.
This means there is a non-zero chance the particle simply appears on the other side of the barrier. It tunnels through.
The core of the sun is hot, but not hot enough to force two hydrogen atoms to fuse. They should repel each other like magnets. They only fuse because they quantum tunnel through the electrical barrier that should keep them apart.
Without this constant cheating, the sun would just be a cold, dark rock.
We even use this glitch to see atoms. A scanning tunneling microscope brings a sharp needle incredibly close to a surface.
Electrons jump from the sample to the needle, creating a current that maps the atomic landscape.
A particle's position and behavior are described by a mathematical wave function rather than a fixed trajectory. When this wave packet encounters a short, narrow potential barrier, the wave does not entirely bounce off. Part of it penetrates and emerges on the other side.
The likelihood that a particle makes it across falls exponentially as the barrier gets thicker, the barrier energy rises, and the particle's mass increases. Because light particles cross narrow gaps far more easily, tunneling appears most often in low-mass particles like electrons, though researchers have observed it in protons and entire atoms as well.
Tunneling makes modern electronics work while simultaneously setting their physical boundaries. Flash memory chips and tunnel diodes depend on electrons crossing barriers to store data and control electrical current. Scanning tunneling microscopes pass an electric current through the gap between a needle and a surface to map individual atoms.
The effect also creates a hard limit for computer chips. When insulating layers and transistors are manufactured thinner than roughly one nanometer, electrons begin tunneling through them on their own, causing electrical leakage.
In quantum tunneling, what lets a particle cross a barrier it cannot climb over?
Its wave-like behavior gives it a chance to appear beyond it. A particle’s wave-like nature gives it a nonzero chance of being found beyond the barrier, even without enough energy to surmount it.
How does a scanning tunneling microscope use quantum tunneling to map a surface?
It measures electron current between a nearby tip and the sample. Electrons tunnel between the sample and a very nearby tip; changes in current reveal the surface’s atomic landscape.
Why can a subatomic particle pass through a solid barrier it lacks the energy to climb over?
It exists as a probability wave. Subatomic particles aren't solid dots; their positions are fuzzy probability clouds. There is always a non-zero chance they simply materialize on the other side.
Collectible card
Play the lesson in edgi and the card is yours. It lands on your Map next to the ideas it connects to, and turns from matte to foil to gold as you learn more around it.
Nuclear fusion in stars depends on hydrogen nuclei tunneling through their mutual electrical repulsion to fuse together. Alpha radioactive decay in unstable atomic nuclei also occurs because alpha particles tunnel out of the confining nuclear potential barrier.
Yes. An optical analog called frustrated total internal reflection occurs when light reflects inside a prism and a second prism is placed within a few wavelengths of the surface, causing some light to cross the narrow gap.
Friedrich Hund first applied the Schrödinger equation to a barrier problem in 1927. Leonid Mandelstam and Mikhail Leontovich discovered it independently in 1928, the same year George Gamow, Ronald Gurney, and Edward Condon used it to explain alpha decay.
Part of the Set · 8 cards
Fire electrons at two slits one at a time, and they still paint stripes that no single particle should.
Learn the whole SetLesson complete
You finished the lesson. In edgi, the card goes on your Map next to everything else you learn.
