method

path integral

A path integral is a quantum mechanical method that sums over all possible paths a particle can take between two points.
15 related articles · 4 formulas · 2 who worked here

Description

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.

History

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.

How it works

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.

In practice

Predicting the behavior of financial options, designing quantum computers, computing properties of new materials before they are synthesized.

Fun fact

Feynman invented the path integral while pondering how light could travel along all rays at once, like threads in steamed-up glass.

Concept graph →

Formulas

$$S_E = \int L_E d\tau$$
Action in Euclidean time for path integral weighting.
What is in the formula
S_EvariableEuclidean action — action joule second
L_EvariableEuclidean Lagrangian — lagrangian joule
τvariableEuclidean time — time second
∫operatorIntegration over Euclidean time — integral operator
dτoperatorInfinitesimal time element — differential element
s_e=2π^2\intdτ(-3a\dot{a}^2+\frac{1}{2}a^3\dot{φ}^2-3a+a^3v(φ)+\frac{q_a^2}{a^3}+\frac{q_m^2}{a}) · 2605.10548v1
$$\Psi = \int \mathcal{D}\phi\, e^{iS[\phi]/\hbar}$$
Quantum amplitude is sum over histories with phase from action.
What is in the formula
Ψvariablequantum amplitude (transition amplitude or wavefunction) — probability amplitude varies
φvariablefield configuration (path variable) — field varies
S[φ]variableaction functional of the field configuration — action joule second
ℏconstantSets the scale of quantum fluctuations — reduced planck constant = 1.054571817e-34 joule second
∫ 𝒟φoperatorsums over all possible histories of the field — functional integral
\psi(b,t)=\intdφa(φ)e^{i(p(b;φ,m)-φt)} · 2606.02514v1
$$\lambda = \frac{1}{n \sigma}$$
Average distance between particle collisions.
What is in the formula
\lambdavariablemean free path — mean free path metre
nvariablenumber density of particles — number density per cubic metre
\sigmavariablecollision cross-section — cross section square metre
λ_ν=\frac{1}{n_ν\langleσ_{{weak}}\rangle} · 2607.09285
$$P(r) = \frac{\int_{r}^{r_c} \frac{du}{u^2 \sqrt{f(u)}}}{\int_{r_H}^{r_c} \frac{du}{u^2 \sqrt{f(u)}}}$$
Probability of particle capture between two horizons via metric integrals.
What is in the formula
P(r)variablecapture probability at radius r — probability
rvariableradial coordinate — radius metre
r_cvariableouter horizon radius — radius metre
r_Hvariableinner horizon radius — radius metre
uvariableintegration variable — radius metre
f(u)variablemetric function — metric function
∫operatorcomputes the area under the curve of the integrand — integral operator
√operatorcomputes the principal square root — square root
p_h(r)=\frac{\int_r^{r_c}\frac{du}{u^2\sqrt{f(u)}}}{\int_{r_h}^{r_c}\frac{du}{u^2\sqrt{f(u)}}} · 2607.14626

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