Properties of ρ
A matrix qualifies as a density operator only if it satisfies three conditions. These conditions are exactly what guarantees it produces sensible probabilities for every possible measurement.
The three defining properties
A density operator on a Hilbert space must be:
- Unit trace: . The trace collects the total probability, so it must equal one.
- Hermitian: . Equivalently . Hermiticity guarantees real eigenvalues and real expectation values for observables.
- Positive semidefinite: for every . Equivalently, all eigenvalues of are . This makes every measurement probability non-negative.
Conversely, any matrix with these three properties is the density operator of some physical state. This is the complete characterization.
Why each property is forced
Write . The probability of obtaining outcome is . Because each and each , the sum is non-negative — positivity. Each is Hermitian and the are real, so is Hermitian. And , so .
The eigenvalue picture
Because is Hermitian, the spectral theorem diagonalizes it:
The eigenvalues are themselves a probability distribution. So every density operator is a mixture of orthonormal pure states (its eigenvectors) with weights given by its eigenvalues — its spectral decomposition. This is the canonical, ambiguity-free ensemble hiding inside .
Try it
Build and check all three properties.
Return true only if the trace is , the matrix is Hermitian, and both eigenvalues are non-negative.
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