Fermi's golden rule is a principle that calculates the transition rate between quantum states.A quantum particle like an electron cannot just 'slightly' jump to another level — the transition either happened or it didn't. Fermi's golden rule gives the probability of such an event per second. It's like predicting how often a ball exits a maze through many exits if it is constantly nudged by weak pushes.
Paul Dirac in 1927 derived the expression for the transition probability into the continuum, laying the foundations of time-dependent perturbation theory. Enrico Fermi in the 1940s actively used this formula for neutron reaction calculations and named it 'golden rule No. 2' because it proved indispensable. Subsequently, John von Neumann and other mathematicians refined the applicability conditions, linking the rule to the spectral function theorem.
Fermi's rule underlies the calculation of particle decay widths, nuclear reaction rates, photoelectric effect cross section, and tunneling in solids. It is adequate for weak, short-range perturbations and a sufficiently dense spectrum of final states. For strong fields or long duration, non-perturbative methods are needed.
Thanks to this rule, we know why LEDs glow a specific color: electrons and holes meet at a pre-calculated rate.
| \Gamma_{i\to f} | variable | Transition rate from initial state i to final state f — transition rate per second |
| \psi_i | variable | Initial quantum state — wave function |
| \psi_f | variable | Final quantum state — wave function |
| H' | variable | Perturbation Hamiltonian — perturbation hamiltonian joule |
| \rho(E_f) | variable | Density of final states at energy E_f — density of states per joule |
| \hbar | constant | Reduced Planck constant, relating energy to angular frequency — reduced planck constant = 1.054571817e-34 joule second |
| \langle \psi_f | H' | operator | Matrix element of the perturbation between initial and final states — matrix element |
















