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Quantum Mechanical Tunneling

The phenomenon where a particle can pass through a potential barrier even if it does not have enough energy to overcome it classically.
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The statement of the theorem

Consider a particle of mass mm encountering a potential barrier V(x)V(x) defined over x[a,b]x \in [a, b], such that E<V(x)E < V(x) in this region. The transmission probability TT through the barrier, derived from the WKB approximation, is given by:\nTexp(2ab2m(V(x)E)dx)T \approx \exp\left(-\frac{2}{\hbar} \int_{a}^{b} \sqrt{2m(V(x) - E)} \, dx\right)\nwhere EE is the particle's total energy.
Source: Wikipedia