Observables as Hermitian Operators and Their Spectra · seed 1 · A4, ink-friendly. The answer key prints on its own page for grown-ups.

Measuring devices as Hermitian operators

Science · Quantum & Modern Physics · ages 22-23
Name ______________________   Date ____________
  1. What is the spectrum of an operator?

    • The set of all state vectors
    • The menu of results a measurement can return
    • The list of all possible operators
  2. Why are observables represented by Hermitian operators rather than by any matrix at all?

    • Hermitian operators always have real eigenvalues
    • Hermitian operators are always diagonal
    • Any matrix has real eigenvalues
  3. A Hermitian operator can have a non-real eigenvalue.

    Circle one:   True   False

  4. What do orthogonal eigenvectors mean physically?

    • Outcomes always occur together
    • The operator has no eigenvalues
    • Distinct outcomes match distinct, non overlapping states
  5. A state is expanded in an observable's eigenbasis with weights 0.6 and 0.8. What are the measurement probabilities?

    • 0.6 and 0.8
    • 0.36 and 0.64
    • 0.3 and 0.4
  6. What changes when an observable has a continuous spectrum, like position?

    • Probabilities come from densities with a different normalization
    • Eigenvalues stop being real
    • Every outcome becomes equally likely
  7. A state is 0.6 times one energy eigenstate plus 0.8 times another. What is the probability of measuring the second energy?

    Answer: ______________

  8. What do sharp spectral lines in an atomic spectrum record?

    • Direct photographs of electron orbits
    • Jumps between definite energies, marking eigenvalues indirectly
    • Noise in the detector
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Answer key

For grown-ups. Fold this page away before handing over the rest.

Measuring devices as Hermitian operators W1-mt_TXCN8uiWqs-s1

  1. The menu of results a measurement can return · Only eigenvalues of the operator ever appear as measurement results.
  2. Hermitian operators always have real eigenvalues · Detectors report real numbers, and Hermiticity guarantees exactly that.
  3. False · Hermiticity forces every eigenvalue to be real.
  4. Distinct outcomes match distinct, non overlapping states · Orthogonality keeps the states behind different outcomes from overlapping.
  5. 0.36 and 0.64 · The squared weights give the probability of each eigenvalue.
  6. Probabilities come from densities with a different normalization · Continuous outcomes need densities rather than a plain list of odds.
  7. 0.64 · Square the second weight: 0.8 squared is 0.64.
  8. Jumps between definite energies, marking eigenvalues indirectly · Each line marks a jump between two eigenstates of the energy operator.
Worksheet · LightMySky