A path integral is a quantum mechanical method that sums over all possible paths a particle can take between two points.The path integral abandons a single trajectory in favor of a superposition of all possible paths. Instead of the Schrödinger differential equation, it uses direct summation of amplitudes: each path contributes with a complex weight exp(iS/ħ), where S is the classical action. Quantum interference highlights paths where the action barely changes (the principle of least action), thereby recovering classical mechanics. The method proved universal: it describes elementary particles, thermal fluctuations, and even black holes.
The early trail leads to Paul Dirac, who in 1933 noted that the quantum propagator can be written via an exponential of the classical action. John Archibald Wheeler encouraged his student Richard Feynman to think that the amplitude should be a sum over all paths. Feynman developed the framework in his 1942 dissertation and published it in 1948, revolutionizing quantum electrodynamics.
The central idea is quantum superposition: the amplitudes of all virtual trajectories interfere. The phase of each is proportional to the classical action in units of ħ. In the limit ħ→0, the stationary phase method picks out a single trajectory, recovering Newton's second law. In quantum field theory, the functional integral over fields leads to a diagrammatic expansion—the basis of Standard Model calculations. Numerically, the integral is often evaluated using lattice Monte Carlo methods after switching to imaginary time.
Predicting the behavior of financial options, designing quantum computers, computing properties of new materials before they are synthesized.
Feynman invented the path integral while pondering how light could travel along all rays at once, like threads in steamed-up glass.
| S_E | variable | Euclidean action — action joule second |
| L_E | variable | Euclidean Lagrangian — lagrangian joule |
| τ | variable | Euclidean time — time second |
| ∫ | operator | Integration over Euclidean time — integral operator |
| dτ | operator | Infinitesimal time element — differential element |
| Ψ | variable | quantum amplitude (transition amplitude or wavefunction) — probability amplitude varies |
| φ | variable | field configuration (path variable) — field varies |
| S[φ] | variable | action functional of the field configuration — action joule second |
| ℏ | constant | Sets the scale of quantum fluctuations — reduced planck constant = 1.054571817e-34 joule second |
| ∫ 𝒟φ | operator | sums over all possible histories of the field — functional integral |
| \lambda | variable | mean free path — mean free path metre |
| n | variable | number density of particles — number density per cubic metre |
| \sigma | variable | collision cross-section — cross section square metre |
| P(r) | variable | capture probability at radius r — probability |
| r | variable | radial coordinate — radius metre |
| r_c | variable | outer horizon radius — radius metre |
| r_H | variable | inner horizon radius — radius metre |
| u | variable | integration variable — radius metre |
| f(u) | variable | metric function — metric function |
| ∫ | operator | computes the area under the curve of the integrand — integral operator |
| √ | operator | computes the principal square root — square root |





