The Action and Path Integral in Quantum Mechanics
Core Concept Overview
This framework connects classical and quantum mechanics through the concept of the action and extends it via the path integral, which provides a complete reformulation of quantum theory.
1. The Classical Action (S)
In classical mechanics, the action is a fundamental quantity within the Lagrangian formulation. It is a functional—a function of a function—that assigns a single real number to any conceivable path q(t) between two points in configuration space.
Here, L is the Lagrangian (typically Kinetic Energy minus Potential Energy: T - V), q(t) is the generalized coordinate (like position), and ˙q(t) is its time derivative (velocity).
Principle of Least Action (Hamilton's Principle)
The actual path taken by a classical particle between two points is the one that makes the action stationary (typically a minimum). This variational principle yields the Euler-Lagrange equations of motion, which are mathematically equivalent to Newton's laws.
Classical Summary: Nature selects the one unique path that extremizes the action.
2. The Quantum Path Integral (Feynman's Formulation)
Richard Feynman revolutionized quantum mechanics by reinterpreting the action. In the quantum domain, determinism dissolves.
Core Quantum Idea
A quantum particle does not take a single, definite path between an initial point A and a final point B. Instead, it theoretically explores every possible path simultaneously. Each path contributes to the total quantum amplitude for the transition from A to B.
The Path Integral Mechanism
Step 1: Amplitude per Path
To each hypothetical path q(t), we assign a complex phase factor:
Here, S[q(t)] is the classical action for that specific path, and ħ is the reduced Planck constant. The magnitude of this factor is always 1; only its phase (angle in the complex plane) changes, dictated by the action.
Step 2: Sum Over All Paths (The Integral)
The total probability amplitude K(A → B) (the propagator) is found by summing (integrating) this phase factor over all paths connecting A and B:
The symbol ∫ 𝒟q(t) represents a functional integral—an infinite-dimensional integral over all possible functions (paths).
Step 3: Quantum Interference
Paths with very different actions have wildly different phases and tend to interfere destructively (cancel out). Paths where the action is stationary (i.e., the classical path and its neighbors) have nearly identical phases and interfere constructively.
Step 4: From Amplitude to Probability
The probability for the particle to go from A to B is the absolute square of the total amplitude:
Key Implications
Emergence of Classical Physics: The classical path of least action is the path of stationary phase. In the limit where ħ → 0 (the classical limit), constructive interference is infinitely sharp, isolating only the classical path.
Double-Slit Explained: The path integral naturally accounts for a particle going through both slits. The amplitude sums over the path through the left slit and the path through the right slit; their interference creates the observed pattern.
Advantages: This formulation is conceptually elegant, makes symmetries transparent, and generalizes seamlessly to quantum field theory, where one sums over all possible field configurations.
Analogy: The Drunkard's Walk
Classical (Sober Walk): A person takes the single, shortest, most efficient route from the pub to home.
Quantum (Drunkard's Walk): Imagine a profoundly drunk person who, in a sense, stumbles along every conceivable zigzag path at once. For each path, we attach a spinning arrow (the phase eiS/ħ). Adding all arrows, most cancel (pointing in random directions). Arrows for paths similar to the sober walk point in nearly the same direction and reinforce each other. Thus, the highest probability concentrates near the classical path.
Summary: Classical vs. Quantum View
| Concept | Role in Classical Mechanics | Role in Quantum Mechanics (Path Integral) |
|---|---|---|
| Action (S) | A number to be minimized. It selects the one true path. | A number determining the quantum phase eiS/ħ for each possible path. |
| Path | A single trajectory q(t) obeying deterministic laws. | All possible trajectories q(t) connecting the two points. |
| Core Principle | Principle of Least Action. | Sum over all histories/paths, weighted by eiS/ħ. |
| Outcome | Deterministic trajectory. | Probability amplitude, from which observable probability is derived. |
In Essence
The action is the fundamental quantity that dictates the quantum phase. The path integral is the rule for summing these phases over all conceivable paths to calculate quantum probabilities. It reveals quantum mechanics as a theory of "everything that might have happened" (Feynman).