Born's rule gives the probability of measuring a quantum state in a particular basis as the square of the amplitude.In 1926, Max Born published a paper proposing a probabilistic interpretation of the wave function introduced by Schrödinger. Before that, the Schrödinger equation predicted waves, but it was unclear what they described. Born guessed: the intensity of the wave is the probability density. For this idea he received the Nobel Prize only almost three decades later, it seemed so radical. In physics, it became established: the quantum world is fundamentally random, but this randomness is strictly mathematically predictable.
Max Born proposed the probabilistic interpretation of the wave function amplitude in a 1926 paper, analyzing particle scattering. Initially the idea met resistance, including from Schrödinger and Einstein. Born shared the 1954 Nobel Prize in Physics 'for fundamental research in quantum mechanics, especially for the statistical interpretation of the wave function'. The development of the principle continued in the works of von Neumann, who introduced the concept of the density matrix, and in the modern formulation of quantum information theory.
The Born rule is applied in all areas of quantum physics — from calculating atomic spectra to designing quantum computers. It sets the connection between mathematics and experiment. Applicability limits: the same as for quantum mechanics — distances much larger than the Planck length, energies much lower than the Planck energy. No violations of the principle have been found, but the question of its origin from the many-worlds interpretation or quantum Darwinism remains open.
Without it, one cannot understand why electrons in atoms form clouds of certain shapes — all chemical bonds and material properties depend on this.
Born himself initially doubted the probabilistic interpretation and even sent the paper to press with reservations. Only later, seeing its success, did he accept his own guess.
| P | variable | probability density — probability density per metre cubed |
| ψ | variable | wavefunction — wave function per metre to the three halves |
| a_k | variable | Probability amplitude for state k — probability amplitude |
| P_n | variable | Boltzmann weight for state n — boltzmann weight |
| χ_k | variable | Eigenstate of observable — quantum state |
| n | variable | Energy eigenstate — quantum state |
| ⟨ | ⟩ | operator | Quantum mechanical inner product — inner product |
| ∑ | operator | Sum over states — summation |
| A | variable | Operator whose expectation is taken — operator |
| ρ | variable | Density matrix (quantum state) — density matrix |
| Tr | operator | Computes the sum of diagonal elements of a matrix — trace operator |
| R^2 | variable | Coefficient of determination — coefficient of determination |
| SS_res | variable | Residual sum of squares — residual sum of squares square of dependent variable |
| SS_tot | variable | Total sum of squares — total sum of squares square of dependent variable |


















