Physics · lesson 4 of 4
Operators, commutators and uncertainty
Observables are represented by suitable self-adjoint operators. In finite dimensions they are Hermitian matrices with real eigenvalues.
Learn the ideas
Prerequisites: Linear algebra and quantum expectation values.
Operators
Observables are represented by suitable self-adjoint operators. In finite dimensions they are Hermitian matrices with real eigenvalues.
Commutator
[A,B]=AB−BA measures noncommutation. Matrix multiplication order matters.
Variance
The variance of A is ⟨A²⟩−⟨A⟩². A zero variance in a normalized state indicates a definite outcome for that observable.
Uncertainty
For canonical position and momentum, ΔxΔp≥ℏ/2. The spreads describe the quantum state, not merely careless measurement.
Worked examples
An observable has mean 3 and mean square 11 in matching units. Find its variance.
Variance=11−9=2.
2
Which expression defines [A,B]?
The commutator compares multiplication in the two orders.
AB−BA
Check your understanding
8 questionsDecimals or fractions are accepted for numeric answers. Proofs and written responses use sample answers and require human marking. This is practice, not a protected examination.
Further reading and review references
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