Quantum instruments as a foundation for both states and observables
arXiv:1305.2816 · doi:10.1103/PhysRevA.88.022107
Abstract
We demonstrate that quantum instruments can provide a unified operational foundation for quantum theory. Since these instruments directly correspond to laboratory devices, this foundation provides an alternate, more experimentally grounded, perspective from which to understand the elements of the traditional approach. We first show that in principle all measurable probabilities and correlations can be expressed entirely in terms of quantum instruments without the need for conventional quantum states or observables. We then show how these states and observables reappear as derived quantities by conditioning joint detection probabilities on the first or last measurement in a sequence as a preparation or a post-selection. Both predictive and retrodictive versions of states and observables appear in this manner, as well as more exotic bidirectional and interdictive states and observables that cannot be easily expressed using the traditional approach. We also revisit the conceptual meaning of the Heisenberg and Schrödinger pictures of time evolution as applied to the various derived quantities, illustrate how detector loss can be included naturally, and discuss how the instrumental approach fully generalizes the time-symmetric two-vector approach of Aharonov \emph{et al.} to any realistic laboratory situation.
15 pages, 11 figures
References in corpus (7)
- Weak values and the Leggett-Garg inequality in solid-state qubits
- Undoing a weak quantum measurement of a solid-state qubit
- Quantum Graphical Models and Belief Propagation
- Quantum Dynamics as an analog of Conditional Probability
- Qubit feedback and control with kicked quantum nondemolition measurements: A quantum Bayesian analysis
- Weak values are universal in von Neumann measurements
- Characterizing Quantum Properties of a Measurement Apparatus: Insights from the Retrodictive Approach
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