The Fundamental Axioms of Quantum Mechanics
Quantum mechanics is built on a few simple yet profound axioms. These axioms describe how quantum systems behave and how we connect mathematics to physical measurements.
Axiom 1: The State Axiom
A quantum system is fully described by its wave function $\\psi(\\mathbf{r},t)$, a complex function of position and time:
It encodes the probability amplitude of finding a particle at a point and evolves according to the Schrödinger equation.
Example: A free particle along the x-axis:
Axiom 2: Linear Superposition Principle
If a system can exist in states $\\psi_1$ and $\\psi_2$, it can also exist in any linear combination:
This explains phenomena like interference. The system can be in “both states” until measured.
Example: Electron through a double slit forms an interference pattern because it is in a superposition of “slit 1” and “slit 2” states.
Axiom 3: Observable–Operator Correspondence
Every measurable quantity corresponds to a linear operator:
- Position: $\\hat{\\mathbf{r}}} = \\mathbf{r}$
- Momentum: $\\hat{\\mathbf{p}}} = -i\\hbar\\nabla$
Any function of observables $F(\\mathbf{r},\\mathbf{p})$ becomes an operator:
Axiom 4: Expectation-Value Axiom
The average value of an observable $A$ in a state $\\psi$ is:
This is the quantum analogue of classical averages and connects operators with measurable outcomes.
Axiom 5: Expansion Postulate
For a Hermitian operator $\\hat{A}$, its eigenfunctions $\\psi_1, \\psi_2, \\dots$ form a complete orthonormal set. Any state can be written as:
Coefficients $c_n$ give the probability amplitudes for each eigenvalue. This is a structured decomposition into measurement-relevant basis states.
Summary of Quantum Axioms
- State Axiom: Wave function defines the system.
- Superposition: States can combine linearly.
- Observables ↔ Operators: Measurable quantities have operator counterparts.
- Expectation Value: Average measurements from wave functions.
- Expansion Postulate: Any state can be expressed in terms of eigenstates.