concept

quantum tunneling

Quantum tunneling is a quantum mechanical phenomenon where particles pass through energy barriers.
18 related articles · 2 formulas · 5 who worked here

Description

Imagine you're rolling a ball over a hill, but it miraculously appears on the other side without even climbing over the top. For microscopic particles, this is routine – it's called quantum tunneling.

History

The first theoretical explanation of tunneling was given in 1928 independently by George Gamow, and also by Ronald Gurney and Edward Condon for alpha decay of nuclei. Subsequently, the phenomenon was applied in solid-state physics: Leo Esaki in 1958 created the tunnel diode, for which he received the Nobel Prize. In astrophysics, tunneling explained the mechanism of stellar nucleosynthesis (Hans Bethe, 1938). Later, Stephen Hawking used the concept of tunneling to describe black hole radiation.

How it works

Within nonrelativistic quantum mechanics, tunneling is described by solving the stationary Schrödinger equation for a potential with a barrier. The wavefunction inside the barrier (E < V₀) has the form ψ(x) ∝ e^{-κx}, where κ = √(2m(V₀−E))/ħ. The transmission coefficient (tunneling probability) for a rectangular barrier of width L: T ≈ e^{-2κL}. The Heisenberg uncertainty principle allows a temporary violation of energy conservation, making tunneling possible. This effect is also used to explain the cosmological birth of the Universe and Hawking radiation.

Fun fact

Quantum tunneling is like walking through a wall without breaking it. Electrons do this constantly in microchips, seeping through barriers.

Concept graph →

Formulas

$$T \approx \exp\left(-2\int_{z_1}^{z_2} \sqrt{\frac{2m}{\hbar^2}(V(z)-E)}\, dz\right)$$
Approximate quantum tunneling probability through a barrier.
What is in the formula
Tvariabletunneling probability — transmission probability
z1variableleft turning point of the barrier — position metre
z2variableright turning point of the barrier — position metre
mvariablemass of the tunneling particle — mass kilogram
Vvariablepotential energy as a function of position — potential energy joule
Evariableenergy of the particle — energy joule
ħconstantfundamental quantum of action divided by 2π — reduced planck constant = 1.054571817e-34 joule second
∫operatorsums the integrand over the interval — integral
√operatortakes the non-negative root — square root
expoperatorraises e to the given power — exponential
d\approx\exp[-\sqrt{\frac{8m_{e}}{ħ^{2}}}\int_{z_{1}}^{z_{2}}m^{1/2}(φ,f,z)dz] · 2505.00872v4
$$\Gamma \propto e^{-S}$$
Quantum tunneling rates are exponentially suppressed by the bounce action.
What is in the formula
\GammavariableTunneling rate (probability per unit time) — rate per second
SvariableEuclidean action of the bounce solution — action joule second
\proptooperatorIndicates proportionality — proportional to
e^{-S}operatorExponential function with exponent -S — exponential
\gamma/v=m^4e^{-s} · 2606.06587v1

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